Download citation
Download citation
link to html
The aggregation of molecules is usually associated with a specific type of interaction, which can be altered by thermodynamic conditions. Under normal conditions, the crystal structure of seleno­urea, SeC(NH2)2, phase α is trigonal, space group P31, Z = 27. Its large number of independent molecules (Zα′ = 9) can be associated with the formation of an NH...N hydrogen bond substituting one of 36 independent NH...Se hydrogen bonds, which prevail among intermolecular interactions. Phase α approximates the trigonal structure with a threefold smaller unit cell (Z = 9), which in turn approximates another still threefold smaller unit cell (Z = 3). The temperature-induced transformations of seleno­urea have been characterized by calorimetry and by performing 21 single-crystal X-ray diffraction structural determinations as a function of temperature. At 381.0 K, phase α undergoes a first-order displacive transition to phase γ, with space group P3121 and Z reduced to 9, when the NH...N bond is broken and an NH...Se bond is formed in its place. Previously, an analogous competition was observed between NH...N and NH...O hydrogen bonds in high-pressure phase III of urea. The lattice vectors along the (001) plane in low- and high-temperature phases of seleno­urea are related by a similarity rule, while the lattice dimensions along direction c are not affected. This similarity rule also applies to the structures of phase γ and hypothetical phase δ (Z = 3). The thermally controlled transition between enantiomorphic phases of seleno­urea contrasts with its high-pressure transition at 0.21 GPa to a centrosymmetric phase β, where both the NH...Se and NH...N bonds are present. The compression and heating reduce the number of independent molecules from Z′ = 9 in phase α, to Z′ = 2 in phase β and to Z′ = 1.5 in phase γ.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520622011623/bm5148sup1.cif
Contains datablocks global, phase_alpha_Selenourea_110K, phase_alpha_Selenourea_130K, phase_alpha_Selenourea_150K, phase_alpha_Selenourea_170K, phase_alpha_Selenourea_190K, phase_alpha_Selenourea_210K, phase_alpha_Selenourea_230K, phase_alpha_Selenourea_250K, phase_alpha_Selenourea_270K, phase_alpha_Selenourea_290K, phase_alpha_Selenourea_293K, phase_alpha_Selenourea_303K, phase_alpha_Selenourea_313K, phase_alpha_Selenourea_323K, phase_alpha_Selenourea_333K, phase_alpha_Selenourea_343K, phase_alpha_Selenourea_353K, phase_alpha_Selenourea_363K, phase_alpha_Selenourea_373K, phase_gamma_Selenourea_383K, phase_gamma_Selenourea_393K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_110Ksup2.hkl
Contains datablock phase_alpha_Selenourea_110K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_130Ksup3.hkl
Contains datablock phase_alpha_Selenourea_130K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_150Ksup4.hkl
Contains datablock phase_alpha_Selenourea_150K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_170Ksup5.hkl
Contains datablock phase_alpha_Selenourea_170K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_190Ksup6.hkl
Contains datablock phase_alpha_Selenourea_190K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_210Ksup7.hkl
Contains datablock phase_alpha_Selenourea_210K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_230Ksup8.hkl
Contains datablock phase_alpha_Selenourea_230K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_250Ksup9.hkl
Contains datablock phase_alpha_Selenourea_250K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_270Ksup10.hkl
Contains datablock phase_alpha_Selenourea_270K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_290Ksup11.hkl
Contains datablock phase_alpha_Selenourea_290K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_293Ksup12.hkl
Contains datablock phase_alpha_Selenourea_293K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_303Ksup13.hkl
Contains datablock phase_alpha_Selenourea_303K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_313Ksup14.hkl
Contains datablock phase_alpha_Selenourea_313K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_323Ksup15.hkl
Contains datablock phase_alpha_Selenourea_323K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_333Ksup16.hkl
Contains datablock phase_alpha_Selenourea_333K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_343Ksup17.hkl
Contains datablock phase_alpha_Selenourea_343K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_353Ksup18.hkl
Contains datablock phase_alpha_Selenourea_353K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_363Ksup19.hkl
Contains datablock phase_alpha_Selenourea_363K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_alpha_Selenourea_373Ksup20.hkl
Contains datablock phase_alpha_Selenourea_373K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_gamma_Selenourea_383Ksup21.hkl
Contains datablock phase_gamma_Selenourea_383K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520622011623/bm5148phase_gamma_Selenourea_393Ksup22.hkl
Contains datablock phase_gamma_Selenourea_393K

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2052520622011623/bm5148phase_gamma_Selenourea_393Ksup24.cml
Supplementary material

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520622011623/bm5148sup23.pdf
Supplementary material

CCDC references: 2159738; 2159739; 2159740; 2159741; 2159742; 2159743; 2159744; 2159745; 2159746; 2159747; 2159748; 2159749; 2159750; 2159751; 2159752; 2159753; 2159754; 2159755; 2159756; 2159757; 2159758

Computing details top

For all structures, data collection: CrysAlis PRO 1.171.40.67a (Rigaku OD, 2019); cell refinement: CrysAlis PRO 1.171.40.67a (Rigaku OD, 2019); data reduction: CrysAlis PRO 1.171.40.67a (Rigaku OD, 2019). Program(s) used to solve structure: SHELXD (Sheldrick, 2008) for phase_alpha_Selenourea_110K, phase_alpha_Selenourea_293K, phase_alpha_Selenourea_303K, phase_alpha_Selenourea_333K, phase_alpha_Selenourea_343K, phase_alpha_Selenourea_353K, phase_alpha_Selenourea_363K, phase_alpha_Selenourea_373K, phase_gamma_Selenourea_383K; SHELXS (Sheldrick, 2008) for phase_alpha_Selenourea_130K, phase_alpha_Selenourea_150K, phase_alpha_Selenourea_170K, phase_alpha_Selenourea_210K, phase_alpha_Selenourea_270K, phase_alpha_Selenourea_313K, phase_alpha_Selenourea_323K; SHELXT 2018/2 (Sheldrick, 2018) for phase_alpha_Selenourea_190K, phase_alpha_Selenourea_230K, phase_alpha_Selenourea_250K, phase_alpha_Selenourea_290K, phase_gamma_Selenourea_393K. For all structures, program(s) used to refine structure: SHELXL 2018/3 (Sheldrick, 2015); molecular graphics: Olex2 1.3 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 1.3 (Dolomanov et al., 2009).

Selenourea (phase_alpha_Selenourea_110K) top
Crystal data top
CH4N2SeDx = 2.150 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6736 reflections
a = 15.1354 (1) Åθ = 3.4–72.0°
c = 12.9308 (1) ŵ = 11.51 mm1
V = 2565.33 (4) Å3T = 110 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3849 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3836 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.040
Detector resolution: 10.5384 pixels mm-1θmax = 72.4°, θmin = 3.4°
ω scansh = 1816
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1817
Tmin = 0.218, Tmax = 1.000l = 1413
6546 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.037 w = 1/[σ2(Fo2) + (0.0637P)2 + 4.4956P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.100(Δ/σ)max = 0.001
S = 1.12Δρmax = 0.75 e Å3
3849 reflectionsΔρmin = 1.84 e Å3
325 parametersAbsolute structure: Refined as a perfect inversion twin.
1 restraintAbsolute structure parameter: 0.5
Primary atom site location: dual
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30691 (6)0.35156 (7)0.09667 (6)0.0125 (2)
Se20.39775 (7)0.35996 (7)0.75778 (6)0.0136 (2)
Se30.30521 (6)0.26969 (6)0.42640 (7)0.0122 (2)
Se40.63152 (7)0.60773 (7)0.70782 (6)0.0140 (2)
Se50.72047 (6)0.69453 (6)0.05215 (7)0.0124 (2)
Se60.63317 (6)0.70244 (7)0.38394 (6)0.0126 (2)
Se70.72785 (6)0.37694 (7)0.47721 (8)0.0168 (2)
Se80.29852 (6)0.69993 (6)0.66392 (8)0.0143 (2)
Se91.06916 (7)1.02422 (7)0.45218 (9)0.0183 (2)
C60.7511 (6)0.6921 (6)0.3931 (6)0.0126 (15)
C20.2605 (6)0.3242 (6)0.7543 (6)0.0131 (16)
C90.9341 (6)0.9954 (6)0.4485 (7)0.0156 (16)
C30.4179 (6)0.4028 (6)0.4156 (6)0.0139 (16)
C10.3873 (7)0.2903 (7)0.0944 (7)0.0172 (18)
N160.8070 (5)0.7058 (6)0.3097 (6)0.0185 (15)
H16A0.8619030.7024070.3139280.022*
H16B0.7884410.7181870.2511050.022*
N210.2120 (5)0.3217 (6)0.8403 (6)0.0206 (16)
H21A0.1492520.3068150.8377530.025*
H21B0.2432340.3350520.8986800.025*
N190.8889 (6)1.0050 (6)0.5321 (6)0.0207 (15)
H19A0.8266450.9915450.5289120.025*
H19B0.9218801.0247550.5894590.025*
N290.8818 (6)0.9649 (7)0.3615 (6)0.0266 (18)
H29A0.8196040.9518070.3597130.032*
H29B0.9099320.9582610.3064860.032*
N220.2125 (6)0.3039 (7)0.6655 (6)0.031 (2)
H22A0.1496970.2889850.6633510.038*
H22B0.2436920.3054110.6093960.038*
N260.7806 (6)0.6732 (6)0.4823 (6)0.0225 (16)
H26A0.8356600.6699490.4856620.027*
H26B0.7448080.6641450.5370200.027*
N110.4379 (5)0.2919 (6)0.0109 (6)0.0165 (14)
H11A0.4732600.2617470.0109200.020*
H11B0.4355280.3231450.0436760.020*
N120.3937 (6)0.2405 (6)0.1773 (6)0.0246 (17)
H12A0.4298010.2111410.1745800.030*
H12B0.3616450.2378440.2331920.030*
N280.3912 (7)0.5989 (7)0.7519 (6)0.0272 (19)
H28A0.4283820.5707320.7518220.033*
H28B0.3619420.6012940.8080400.033*
N250.5239 (6)0.6261 (6)0.1280 (6)0.0200 (15)
H25A0.4583730.5932970.1252310.024*
H25B0.5545280.6600390.1826080.024*
N170.5405 (5)0.2429 (6)0.3884 (6)0.0217 (16)
H17A0.4759200.2005630.3880900.026*
H17B0.5742630.2591740.3314320.026*
N180.4255 (6)0.6331 (7)0.5813 (6)0.0285 (19)
H18A0.4623560.6044750.5831340.034*
H18B0.4186960.6583440.5243090.034*
N230.4782 (5)0.4449 (5)0.4977 (6)0.0227 (16)
H23A0.5310890.5046930.4930090.027*
H23B0.4641620.4120720.5552400.027*
N140.6783 (6)0.8030 (6)0.6456 (6)0.0266 (17)
H14A0.7050990.8680030.6522330.032*
H14B0.6422710.7728260.5918720.032*
N240.7476 (6)0.7981 (5)0.7987 (6)0.0213 (16)
H24A0.7738290.8630940.8040090.026*
H24B0.7576220.7646220.8465700.026*
N270.5328 (6)0.2558 (6)0.5629 (6)0.0251 (17)
H27A0.4683630.2133010.5603780.030*
H27B0.5617500.2807440.6213580.030*
N130.4394 (7)0.4528 (6)0.3284 (6)0.0284 (18)
H13A0.4923320.5125940.3239100.034*
H13B0.4006890.4258650.2754600.034*
C70.5878 (6)0.2830 (6)0.4766 (7)0.0159 (16)
C50.5781 (6)0.6244 (6)0.0476 (6)0.0124 (15)
C80.3790 (7)0.6382 (7)0.6667 (7)0.0192 (18)
C40.6923 (6)0.7500 (7)0.7175 (7)0.0170 (17)
N150.5298 (5)0.5721 (6)0.0352 (6)0.0224 (16)
H15A0.4642160.5396000.0369190.027*
H15B0.5638230.5703180.0876730.027*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0119 (4)0.0117 (4)0.0155 (5)0.0069 (3)0.0006 (3)0.0003 (3)
Se20.0089 (4)0.0140 (4)0.0172 (5)0.0054 (3)0.0003 (3)0.0015 (3)
Se30.0109 (4)0.0093 (4)0.0156 (4)0.0045 (3)0.0005 (3)0.0002 (3)
Se40.0127 (4)0.0100 (4)0.0181 (5)0.0049 (3)0.0000 (3)0.0004 (3)
Se50.0095 (4)0.0106 (4)0.0172 (5)0.0051 (3)0.0007 (3)0.0006 (3)
Se60.0107 (4)0.0114 (4)0.0166 (5)0.0062 (3)0.0003 (3)0.0002 (3)
Se70.0101 (4)0.0143 (4)0.0188 (5)0.0007 (3)0.0011 (3)0.0008 (4)
Se80.0160 (4)0.0131 (4)0.0167 (5)0.0093 (4)0.0015 (3)0.0008 (3)
Se90.0110 (4)0.0210 (5)0.0237 (5)0.0085 (4)0.0026 (3)0.0062 (4)
C60.020 (4)0.006 (3)0.016 (4)0.010 (3)0.001 (3)0.001 (3)
C20.008 (4)0.011 (4)0.016 (4)0.002 (3)0.002 (3)0.002 (3)
C90.015 (4)0.011 (4)0.018 (4)0.004 (3)0.000 (3)0.000 (3)
C30.014 (4)0.012 (4)0.014 (4)0.005 (3)0.003 (3)0.002 (3)
C10.027 (5)0.014 (4)0.012 (4)0.011 (4)0.003 (3)0.004 (3)
N160.013 (3)0.027 (4)0.018 (4)0.012 (3)0.004 (3)0.007 (3)
N210.013 (3)0.025 (4)0.023 (4)0.009 (3)0.000 (3)0.001 (3)
N190.016 (3)0.032 (4)0.015 (4)0.013 (3)0.003 (3)0.002 (3)
N290.023 (4)0.038 (5)0.018 (4)0.015 (4)0.004 (3)0.008 (3)
N220.020 (4)0.060 (6)0.020 (4)0.024 (4)0.009 (3)0.016 (4)
N260.017 (4)0.038 (4)0.020 (4)0.019 (3)0.003 (3)0.002 (3)
N110.017 (3)0.022 (4)0.017 (4)0.015 (3)0.004 (3)0.004 (3)
N120.034 (4)0.038 (5)0.015 (4)0.028 (4)0.003 (3)0.003 (3)
N280.036 (5)0.040 (5)0.023 (4)0.032 (4)0.010 (3)0.015 (4)
N250.014 (3)0.021 (4)0.022 (4)0.007 (3)0.002 (3)0.005 (3)
N170.011 (3)0.023 (4)0.023 (4)0.002 (3)0.003 (3)0.002 (3)
N180.037 (5)0.054 (6)0.015 (4)0.038 (5)0.005 (3)0.009 (4)
N230.018 (4)0.014 (3)0.027 (4)0.002 (3)0.001 (3)0.004 (3)
N140.036 (5)0.015 (4)0.026 (4)0.010 (3)0.006 (3)0.000 (3)
N240.027 (4)0.010 (3)0.022 (4)0.006 (3)0.002 (3)0.002 (3)
N270.014 (4)0.031 (4)0.024 (4)0.007 (3)0.002 (3)0.005 (3)
N130.036 (5)0.011 (3)0.022 (4)0.000 (3)0.001 (3)0.002 (3)
C70.012 (4)0.018 (4)0.021 (4)0.009 (3)0.001 (3)0.001 (3)
C50.012 (4)0.015 (4)0.007 (4)0.004 (3)0.005 (3)0.002 (3)
C80.021 (4)0.030 (5)0.014 (4)0.019 (4)0.006 (3)0.000 (3)
C40.013 (4)0.022 (4)0.012 (4)0.005 (3)0.003 (3)0.004 (3)
N150.010 (3)0.034 (4)0.017 (4)0.007 (3)0.000 (3)0.008 (3)
Geometric parameters (Å, º) top
Se1—C11.863 (9)N11—H11B0.8600
Se2—C21.868 (8)N12—H12A0.8600
Se3—C31.885 (8)N12—H12B0.8600
Se4—C41.875 (9)N28—H28A0.8600
Se5—C51.868 (8)N28—H28B0.8600
Se6—C61.872 (8)N28—C81.307 (12)
Se7—C71.871 (8)N25—H25A0.8600
Se8—C81.871 (9)N25—H25B0.8600
Se9—C91.865 (8)N25—C51.332 (11)
C6—N161.321 (11)N17—H17A0.8600
C6—N261.319 (11)N17—H17B0.8600
C2—N211.322 (11)N17—C71.321 (12)
C2—N221.310 (11)N18—H18A0.8600
C9—N191.326 (11)N18—H18B0.8600
C9—N291.319 (12)N18—C81.333 (11)
C3—N231.336 (11)N23—H23A0.8600
C3—N131.304 (11)N23—H23B0.8600
C1—N111.317 (11)N14—H14A0.8600
C1—N121.341 (11)N14—H14B0.8600
N16—H16A0.8600N14—C41.314 (12)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.312 (12)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.329 (11)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.315 (11)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6119.8 (6)C8—N28—H28B120.0
N26—C6—Se6120.9 (6)H25A—N25—H25B120.0
N26—C6—N16119.2 (7)C5—N25—H25A120.0
N21—C2—Se2120.6 (6)C5—N25—H25B120.0
N22—C2—Se2119.7 (6)H17A—N17—H17B120.0
N22—C2—N21119.7 (7)C7—N17—H17A120.0
N19—C9—Se9121.3 (6)C7—N17—H17B120.0
N29—C9—Se9120.0 (7)H18A—N18—H18B120.0
N29—C9—N19118.7 (8)C8—N18—H18A120.0
N23—C3—Se3119.2 (6)C8—N18—H18B120.0
N13—C3—Se3120.9 (6)C3—N23—H23A120.0
N13—C3—N23119.8 (7)C3—N23—H23B120.0
N11—C1—Se1121.4 (6)H23A—N23—H23B120.0
N11—C1—N12117.5 (8)H14A—N14—H14B120.0
N12—C1—Se1121.0 (6)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.0 (6)
H29A—N29—H29B120.0N17—C7—N27118.1 (8)
C2—N22—H22A120.0N27—C7—Se7121.8 (6)
C2—N22—H22B120.0N25—C5—Se5120.7 (6)
H22A—N22—H22B120.0N15—C5—Se5120.3 (6)
C6—N26—H26A120.0N15—C5—N25119.0 (7)
C6—N26—H26B120.0N28—C8—Se8121.2 (6)
H26A—N26—H26B120.0N28—C8—N18118.3 (8)
C1—N11—H11A120.0N18—C8—Se8120.5 (7)
C1—N11—H11B120.0N14—C4—Se4121.2 (7)
H11A—N11—H11B120.0N24—C4—Se4120.1 (6)
C1—N12—H12A120.0N24—C4—N14118.7 (8)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_130K) top
Crystal data top
CH4N2SeDx = 2.145 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6743 reflections
a = 15.14832 (11) Åθ = 3.4–72.4°
c = 12.93947 (13) ŵ = 11.49 mm1
V = 2571.44 (5) Å3T = 130 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3884 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3869 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.032
Detector resolution: 10.5384 pixels mm-1θmax = 72.4°, θmin = 3.4°
ω scansh = 1817
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1818
Tmin = 0.189, Tmax = 1.000l = 1413
6643 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0634P)2 + 4.140P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.036(Δ/σ)max < 0.001
wR(F2) = 0.098Δρmax = 1.57 e Å3
S = 1.12Δρmin = 0.77 e Å3
3884 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00044 (5)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30687 (6)0.35156 (6)0.09676 (6)0.0144 (2)
Se20.39743 (7)0.35999 (7)0.75782 (6)0.0153 (2)
Se30.30519 (6)0.26987 (6)0.42643 (6)0.01408 (19)
Se40.63146 (7)0.60775 (7)0.70780 (6)0.0159 (2)
Se50.72068 (6)0.69452 (6)0.05194 (6)0.0145 (2)
Se60.63318 (6)0.70236 (7)0.38377 (6)0.0144 (2)
Se70.72782 (6)0.37690 (7)0.47695 (8)0.0198 (2)
Se80.29851 (6)0.70000 (6)0.66399 (8)0.0168 (2)
Se91.06917 (7)1.02484 (7)0.45348 (9)0.0212 (2)
C60.7519 (6)0.6924 (5)0.3930 (6)0.0155 (15)
C20.2600 (6)0.3237 (6)0.7552 (6)0.0162 (16)
C90.9341 (6)0.9951 (6)0.4500 (7)0.0198 (17)
C30.4178 (6)0.4021 (6)0.4159 (6)0.0171 (16)
C10.3875 (7)0.2898 (6)0.0945 (6)0.0169 (17)
N160.8064 (5)0.7049 (5)0.3096 (6)0.0216 (15)
H16A0.8604190.6997760.3131590.026*
H16B0.7881350.7180880.2513750.026*
N210.2117 (5)0.3211 (6)0.8404 (6)0.0248 (16)
H21A0.1488770.3056460.8378300.030*
H21B0.2429760.3348270.8987620.030*
N190.8891 (6)1.0056 (6)0.5329 (6)0.0276 (17)
H19A0.8271080.9927730.5293610.033*
H19B0.9219121.0253720.5902960.033*
N290.8815 (6)0.9646 (7)0.3628 (6)0.0323 (19)
H29A0.8195660.9521300.3609450.039*
H29B0.9093390.9572630.3080110.039*
N220.2117 (6)0.3027 (8)0.6663 (6)0.037 (2)
H22A0.1488290.2872570.6642430.044*
H22B0.2429280.3042720.6102610.044*
N260.7799 (6)0.6722 (6)0.4818 (6)0.0264 (16)
H26A0.8339110.6671570.4853480.032*
H26B0.7442950.6640850.5364300.032*
N110.4376 (5)0.2916 (5)0.0108 (5)0.0193 (14)
H11A0.4731270.2616610.0104320.023*
H11B0.4347490.3226560.0436640.023*
N120.3939 (6)0.2408 (7)0.1773 (6)0.0297 (18)
H12A0.4299510.2114620.1750010.036*
H12B0.3618520.2384860.2330800.036*
N280.3905 (7)0.5982 (7)0.7524 (7)0.0330 (19)
H28A0.4273790.5697510.7521510.040*
H28B0.3612750.6005600.8084620.040*
N250.5237 (6)0.6257 (6)0.1281 (6)0.0241 (16)
H25A0.4581670.5924050.1255820.029*
H25B0.5542010.6593590.1828600.029*
N170.5404 (5)0.2428 (6)0.3888 (6)0.0251 (16)
H17A0.4759940.2000870.3882520.030*
H17B0.5742990.2594090.3318900.030*
N180.4252 (7)0.6328 (7)0.5814 (6)0.033 (2)
H18A0.4616380.6037950.5837730.040*
H18B0.4190110.6581050.5242230.040*
N230.4783 (5)0.4451 (6)0.4978 (6)0.0251 (15)
H23A0.5304120.5053300.4928600.030*
H23B0.4651120.4124530.5552910.030*
N140.6784 (7)0.8027 (6)0.6450 (6)0.0319 (18)
H14A0.7054150.8675930.6515620.038*
H14B0.6427440.7725390.5911440.038*
N240.7466 (6)0.7975 (5)0.7994 (6)0.0258 (17)
H24A0.7729660.8624800.8045190.031*
H24B0.7560190.7640090.8476000.031*
N270.5326 (6)0.2551 (6)0.5626 (6)0.0303 (18)
H27A0.4682700.2123250.5601400.036*
H27B0.5614850.2801110.6210150.036*
N130.4393 (7)0.4533 (6)0.3290 (6)0.034 (2)
H13A0.4917010.5134390.3252730.041*
H13B0.4011050.4266120.2757590.041*
C70.5872 (6)0.2825 (6)0.4767 (7)0.0190 (16)
C50.5779 (6)0.6250 (6)0.0473 (6)0.0155 (15)
C80.3785 (7)0.6384 (7)0.6662 (6)0.0201 (17)
C40.6916 (6)0.7492 (6)0.7177 (6)0.0188 (17)
N150.5299 (5)0.5731 (6)0.0354 (6)0.0254 (16)
H15A0.4643870.5401690.0370240.030*
H15B0.5640100.5720390.0881040.030*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0149 (4)0.0155 (4)0.0146 (5)0.0090 (3)0.0004 (3)0.0001 (3)
Se20.0122 (4)0.0181 (4)0.0156 (5)0.0075 (3)0.0002 (3)0.0013 (3)
Se30.0143 (4)0.0126 (4)0.0145 (4)0.0062 (3)0.0004 (3)0.0001 (3)
Se40.0164 (4)0.0135 (4)0.0165 (5)0.0065 (3)0.0000 (3)0.0003 (3)
Se50.0130 (4)0.0141 (4)0.0161 (5)0.0066 (3)0.0011 (3)0.0008 (3)
Se60.0144 (4)0.0149 (4)0.0150 (4)0.0082 (3)0.0002 (3)0.0002 (3)
Se70.0138 (4)0.0187 (4)0.0190 (5)0.0021 (3)0.0012 (3)0.0008 (3)
Se80.0208 (4)0.0172 (4)0.0159 (5)0.0122 (3)0.0017 (3)0.0009 (3)
Se90.0149 (4)0.0262 (5)0.0231 (5)0.0107 (4)0.0029 (3)0.0071 (4)
C60.019 (4)0.011 (3)0.021 (4)0.010 (3)0.001 (3)0.002 (3)
C20.014 (4)0.019 (4)0.017 (4)0.009 (3)0.002 (3)0.001 (3)
C90.020 (4)0.017 (4)0.024 (5)0.010 (3)0.004 (3)0.001 (3)
C30.020 (4)0.018 (4)0.012 (4)0.008 (3)0.002 (3)0.006 (3)
C10.025 (4)0.016 (4)0.012 (4)0.012 (3)0.000 (3)0.002 (3)
N160.019 (3)0.028 (4)0.020 (4)0.013 (3)0.003 (3)0.004 (3)
N210.019 (4)0.035 (4)0.021 (4)0.015 (3)0.000 (3)0.002 (3)
N190.022 (4)0.044 (5)0.022 (4)0.022 (4)0.002 (3)0.000 (3)
N290.026 (4)0.046 (5)0.022 (4)0.016 (4)0.005 (3)0.008 (4)
N220.022 (4)0.075 (7)0.017 (4)0.027 (4)0.005 (3)0.012 (4)
N260.023 (4)0.051 (5)0.017 (4)0.027 (4)0.002 (3)0.001 (3)
N110.021 (3)0.025 (4)0.017 (4)0.015 (3)0.004 (3)0.003 (3)
N120.041 (5)0.049 (5)0.015 (4)0.034 (4)0.005 (3)0.006 (3)
N280.041 (5)0.050 (5)0.024 (4)0.035 (4)0.010 (4)0.014 (4)
N250.021 (3)0.026 (4)0.023 (4)0.010 (3)0.005 (3)0.005 (3)
N170.014 (3)0.027 (4)0.026 (4)0.003 (3)0.002 (3)0.001 (3)
N180.045 (5)0.062 (6)0.014 (4)0.044 (5)0.005 (3)0.010 (4)
N230.021 (4)0.022 (4)0.025 (4)0.006 (3)0.000 (3)0.000 (3)
N140.043 (5)0.015 (3)0.031 (4)0.009 (3)0.011 (4)0.000 (3)
N240.032 (4)0.015 (3)0.026 (4)0.008 (3)0.001 (3)0.004 (3)
N270.019 (4)0.039 (5)0.023 (4)0.008 (3)0.002 (3)0.005 (3)
N130.049 (5)0.014 (4)0.022 (4)0.002 (3)0.002 (4)0.001 (3)
C70.017 (4)0.020 (4)0.020 (4)0.009 (3)0.003 (3)0.004 (3)
C50.015 (4)0.021 (4)0.010 (4)0.008 (3)0.003 (3)0.000 (3)
C80.029 (4)0.034 (5)0.008 (4)0.023 (4)0.002 (3)0.002 (3)
C40.020 (4)0.021 (4)0.013 (4)0.008 (3)0.006 (3)0.003 (3)
N150.013 (3)0.041 (4)0.017 (4)0.009 (3)0.004 (3)0.013 (3)
Geometric parameters (Å, º) top
Se1—C11.874 (8)N11—H11B0.8600
Se2—C21.870 (8)N12—H12A0.8600
Se3—C31.877 (8)N12—H12B0.8600
Se4—C41.868 (9)N28—H28A0.8600
Se5—C51.874 (8)N28—H28B0.8600
Se6—C61.883 (7)N28—C81.325 (11)
Se7—C71.881 (8)N25—H25A0.8600
Se8—C81.863 (8)N25—H25B0.8600
Se9—C91.863 (8)N25—C51.333 (11)
C6—N161.315 (11)N17—H17A0.8600
C6—N261.313 (11)N17—H17B0.8600
C2—N211.312 (11)N17—C71.316 (12)
C2—N221.313 (11)N18—H18A0.8600
C9—N191.321 (11)N18—H18B0.8600
C9—N291.324 (12)N18—C81.331 (11)
C3—N231.337 (11)N23—H23A0.8600
C3—N131.311 (11)N23—H23B0.8600
C1—N111.315 (11)N14—H14A0.8600
C1—N121.335 (11)N14—H14B0.8600
N16—H16A0.8600N14—C41.319 (11)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.318 (12)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.323 (12)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.312 (11)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6119.5 (6)C8—N28—H28B120.0
N26—C6—Se6120.5 (6)H25A—N25—H25B120.0
N26—C6—N16120.0 (7)C5—N25—H25A120.0
N21—C2—Se2121.0 (6)C5—N25—H25B120.0
N21—C2—N22119.6 (7)H17A—N17—H17B120.0
N22—C2—Se2119.4 (6)C7—N17—H17A120.0
N19—C9—Se9121.4 (6)C7—N17—H17B120.0
N19—C9—N29118.5 (8)H18A—N18—H18B120.0
N29—C9—Se9120.0 (6)C8—N18—H18A120.0
N23—C3—Se3119.9 (6)C8—N18—H18B120.0
N13—C3—Se3121.2 (6)C3—N23—H23A120.0
N13—C3—N23119.0 (7)C3—N23—H23B120.0
N11—C1—Se1121.1 (6)H23A—N23—H23B120.0
N11—C1—N12118.2 (7)H14A—N14—H14B120.0
N12—C1—Se1120.8 (6)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7119.7 (6)
H29A—N29—H29B120.0N17—C7—N27118.3 (8)
C2—N22—H22A120.0N27—C7—Se7122.0 (6)
C2—N22—H22B120.0N25—C5—Se5120.8 (6)
H22A—N22—H22B120.0N15—C5—Se5120.0 (6)
C6—N26—H26A120.0N15—C5—N25119.1 (7)
C6—N26—H26B120.0N28—C8—Se8121.0 (6)
H26A—N26—H26B120.0N28—C8—N18117.7 (8)
C1—N11—H11A120.0N18—C8—Se8121.3 (6)
C1—N11—H11B120.0N14—C4—Se4121.2 (7)
H11A—N11—H11B120.0N24—C4—Se4120.1 (6)
C1—N12—H12A120.0N24—C4—N14118.6 (8)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_150K) top
Crystal data top
CH4N2SeDx = 2.140 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6761 reflections
a = 15.16245 (9) Åθ = 3.4–72.2°
c = 12.94774 (11) ŵ = 11.46 mm1
V = 2577.89 (4) Å3T = 150 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
4445 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source4440 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.019
Detector resolution: 10.5384 pixels mm-1θmax = 72.4°, θmin = 3.4°
ω scansh = 1816
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1817
Tmin = 0.291, Tmax = 0.564l = 1413
7392 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0317P)2 + 3.3746P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.023(Δ/σ)max = 0.001
wR(F2) = 0.065Δρmax = 0.74 e Å3
S = 1.13Δρmin = 0.51 e Å3
4445 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00040 (3)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30678 (5)0.35154 (5)0.09692 (5)0.01748 (15)
Se20.39715 (5)0.36000 (5)0.75795 (5)0.01852 (15)
Se30.30514 (5)0.26989 (5)0.42647 (5)0.01733 (14)
Se40.63137 (5)0.60757 (5)0.70759 (5)0.01921 (16)
Se50.72074 (5)0.69442 (5)0.05182 (5)0.01760 (15)
Se60.63320 (5)0.70231 (5)0.38371 (5)0.01752 (15)
Se70.72790 (5)0.37689 (5)0.47674 (6)0.02375 (17)
Se80.29846 (5)0.70001 (5)0.66376 (6)0.02029 (17)
Se91.06937 (5)1.02531 (5)0.45448 (7)0.02527 (16)
C60.7513 (4)0.6916 (4)0.3927 (5)0.0193 (12)
C20.2595 (4)0.3230 (5)0.7549 (5)0.0211 (13)
C90.9335 (5)0.9946 (5)0.4509 (5)0.0227 (13)
C30.4171 (5)0.4027 (4)0.4162 (5)0.0217 (13)
C10.3876 (5)0.2895 (5)0.0946 (5)0.0196 (13)
N160.8065 (4)0.7043 (4)0.3096 (4)0.0260 (12)
H16A0.8603440.6991790.3136460.031*
H16B0.7886080.7177000.2513130.031*
N210.2112 (4)0.3199 (4)0.8407 (5)0.0286 (12)
H21A0.1481390.3034310.8385290.034*
H21B0.2428520.3342780.8988190.034*
N190.8893 (4)1.0057 (5)0.5331 (5)0.0312 (13)
H19A0.8276410.9936360.5294980.037*
H19B0.9220481.0249990.5905250.037*
N290.8815 (4)0.9650 (5)0.3640 (5)0.0373 (15)
H29A0.8199190.9532740.3619880.045*
H29B0.9092190.9572790.3093770.045*
N220.2108 (5)0.3011 (6)0.6672 (5)0.0431 (17)
H22A0.1477460.2846700.6656070.052*
H22B0.2418380.3029460.6108880.052*
N260.7793 (4)0.6712 (5)0.4813 (4)0.0320 (13)
H26A0.8332230.6662310.4847230.038*
H26B0.7436050.6628870.5358800.038*
N110.4370 (4)0.2918 (4)0.0108 (4)0.0238 (11)
H11A0.4727740.2621950.0098330.029*
H11B0.4337270.3229660.0433240.029*
N120.3934 (5)0.2412 (5)0.1774 (4)0.0326 (14)
H12A0.4293990.2117660.1756490.039*
H12B0.3612410.2391860.2328360.039*
N280.3896 (5)0.5977 (5)0.7515 (5)0.0396 (16)
H28A0.4263930.5692230.7512150.047*
H28B0.3602450.5998330.8075460.047*
N250.5247 (4)0.6263 (4)0.1278 (4)0.0273 (12)
H25A0.4592720.5931940.1255690.033*
H25B0.5555920.6601460.1822160.033*
N170.5412 (4)0.2426 (4)0.3890 (5)0.0316 (14)
H17A0.4769210.1997020.3888620.038*
H17B0.5748870.2585500.3320240.038*
N180.4251 (5)0.6331 (6)0.5811 (5)0.0397 (16)
H18A0.4614550.6040520.5831380.048*
H18B0.4190510.6587920.5241740.048*
N230.4773 (4)0.4453 (4)0.4971 (5)0.0294 (12)
H23A0.5293540.5054970.4921020.035*
H23B0.4643540.4127110.5545960.035*
N140.6781 (5)0.8020 (4)0.6446 (5)0.0367 (15)
H14A0.7050580.8669010.6503970.044*
H14B0.6423460.7713180.5909560.044*
N240.7460 (4)0.7971 (4)0.7991 (5)0.0290 (13)
H24A0.7726720.8620660.8042000.035*
H24B0.7551880.7635410.8474000.035*
N270.5334 (4)0.2568 (5)0.5617 (5)0.0346 (14)
H27A0.4691410.2137280.5594660.042*
H27B0.5622690.2825420.6197670.042*
N130.4376 (5)0.4531 (4)0.3288 (5)0.0397 (16)
H13A0.4897620.5133110.3243110.048*
H13B0.3988810.4259820.2759990.048*
C70.5878 (5)0.2833 (4)0.4756 (5)0.0218 (13)
C50.5782 (4)0.6251 (5)0.0470 (5)0.0202 (12)
C80.3782 (5)0.6381 (5)0.6662 (5)0.0248 (14)
C40.6914 (5)0.7493 (5)0.7180 (5)0.0225 (13)
N150.5301 (4)0.5729 (5)0.0362 (4)0.0323 (14)
H15A0.4646620.5399620.0379340.039*
H15B0.5642990.5718160.0887470.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0174 (3)0.0180 (3)0.0188 (4)0.0102 (3)0.0007 (2)0.0004 (2)
Se20.0144 (3)0.0205 (3)0.0204 (4)0.0085 (3)0.0001 (3)0.0020 (2)
Se30.0172 (3)0.0147 (3)0.0193 (3)0.0074 (2)0.0006 (2)0.0002 (3)
Se40.0189 (3)0.0151 (3)0.0217 (4)0.0071 (2)0.0002 (3)0.0001 (2)
Se50.0154 (3)0.0164 (3)0.0208 (4)0.0078 (2)0.0010 (2)0.0004 (2)
Se60.0165 (3)0.0173 (3)0.0201 (3)0.0094 (2)0.0000 (3)0.0001 (2)
Se70.0165 (3)0.0215 (3)0.0237 (4)0.0024 (3)0.0012 (3)0.0004 (3)
Se80.0244 (3)0.0198 (3)0.0209 (4)0.0142 (3)0.0018 (3)0.0007 (3)
Se90.0170 (3)0.0302 (4)0.0295 (4)0.0125 (3)0.0034 (3)0.0081 (3)
C60.022 (3)0.015 (3)0.024 (3)0.011 (2)0.001 (2)0.003 (2)
C20.019 (3)0.025 (3)0.019 (3)0.011 (2)0.001 (2)0.003 (3)
C90.019 (3)0.021 (3)0.026 (4)0.009 (3)0.006 (3)0.003 (3)
C30.025 (3)0.021 (3)0.016 (3)0.009 (3)0.001 (2)0.004 (2)
C10.022 (3)0.021 (3)0.017 (3)0.011 (3)0.001 (2)0.001 (2)
N160.020 (2)0.034 (3)0.027 (3)0.016 (2)0.005 (2)0.005 (2)
N210.019 (3)0.042 (3)0.026 (3)0.016 (2)0.001 (2)0.004 (3)
N190.024 (3)0.048 (4)0.027 (3)0.023 (3)0.001 (2)0.002 (3)
N290.023 (3)0.054 (4)0.030 (4)0.016 (3)0.000 (3)0.011 (3)
N220.024 (3)0.080 (5)0.029 (4)0.029 (3)0.007 (3)0.013 (3)
N260.031 (3)0.060 (4)0.020 (3)0.034 (3)0.001 (2)0.003 (3)
N110.027 (3)0.033 (3)0.019 (3)0.020 (2)0.006 (2)0.007 (2)
N120.044 (3)0.050 (4)0.023 (3)0.038 (3)0.005 (3)0.004 (3)
N280.055 (4)0.059 (4)0.032 (4)0.049 (4)0.015 (3)0.014 (3)
N250.022 (3)0.027 (3)0.029 (3)0.009 (2)0.001 (2)0.006 (2)
N170.017 (3)0.033 (3)0.031 (4)0.002 (2)0.004 (2)0.001 (3)
N180.051 (4)0.075 (5)0.019 (3)0.051 (4)0.009 (3)0.015 (3)
N230.024 (3)0.022 (3)0.029 (3)0.002 (2)0.001 (2)0.002 (2)
N140.059 (4)0.022 (3)0.027 (3)0.019 (3)0.010 (3)0.002 (2)
N240.035 (3)0.015 (3)0.032 (3)0.008 (2)0.002 (3)0.000 (2)
N270.019 (3)0.047 (4)0.029 (4)0.010 (3)0.002 (2)0.005 (3)
N130.053 (4)0.019 (3)0.025 (3)0.001 (3)0.002 (3)0.002 (2)
C70.021 (3)0.021 (3)0.023 (3)0.011 (3)0.002 (2)0.003 (2)
C50.020 (3)0.019 (3)0.020 (3)0.009 (2)0.001 (2)0.001 (2)
C80.028 (3)0.037 (4)0.017 (3)0.022 (3)0.003 (3)0.004 (3)
C40.024 (3)0.024 (3)0.020 (3)0.013 (3)0.006 (2)0.000 (3)
N150.019 (3)0.048 (4)0.022 (3)0.010 (2)0.000 (2)0.010 (3)
Geometric parameters (Å, º) top
Se1—C11.881 (6)N11—H11B0.8600
Se2—C21.872 (6)N12—H12A0.8600
Se3—C31.881 (6)N12—H12B0.8600
Se4—C41.873 (6)N28—H28A0.8600
Se5—C51.873 (6)N28—H28B0.8600
Se6—C61.881 (6)N28—C81.315 (9)
Se7—C71.875 (6)N25—H25A0.8600
Se8—C81.864 (6)N25—H25B0.8600
Se9—C91.871 (6)N25—C51.329 (8)
C6—N161.317 (8)N17—H17A0.8600
C6—N261.311 (8)N17—H17B0.8600
C2—N211.318 (8)N17—C71.304 (9)
C2—N221.303 (9)N18—H18A0.8600
C9—N191.312 (9)N18—H18B0.8600
C9—N291.317 (9)N18—C81.336 (9)
C3—N231.326 (8)N23—H23A0.8600
C3—N131.313 (9)N23—H23B0.8600
C1—N111.309 (8)N14—H14A0.8600
C1—N121.327 (8)N14—H14B0.8600
N16—H16A0.8600N14—C41.320 (9)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.309 (9)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.323 (9)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.320 (8)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6119.9 (5)C8—N28—H28B120.0
N26—C6—Se6120.6 (5)H25A—N25—H25B120.0
N26—C6—N16119.5 (5)C5—N25—H25A120.0
N21—C2—Se2120.6 (5)C5—N25—H25B120.0
N22—C2—Se2119.9 (5)H17A—N17—H17B120.0
N22—C2—N21119.5 (6)C7—N17—H17A120.0
N19—C9—Se9121.2 (5)C7—N17—H17B120.0
N19—C9—N29118.6 (6)H18A—N18—H18B120.0
N29—C9—Se9120.1 (5)C8—N18—H18A120.0
N23—C3—Se3119.9 (5)C8—N18—H18B120.0
N13—C3—Se3120.6 (5)C3—N23—H23A120.0
N13—C3—N23119.5 (6)C3—N23—H23B120.0
N11—C1—Se1120.5 (5)H23A—N23—H23B120.0
N11—C1—N12119.3 (6)H14A—N14—H14B120.0
N12—C1—Se1120.2 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.3 (5)
H29A—N29—H29B120.0N17—C7—N27118.2 (6)
C2—N22—H22A120.0N27—C7—Se7121.4 (5)
C2—N22—H22B120.0N25—C5—Se5120.4 (5)
H22A—N22—H22B120.0N15—C5—Se5120.0 (5)
C6—N26—H26A120.0N15—C5—N25119.6 (6)
C6—N26—H26B120.0N28—C8—Se8121.2 (5)
H26A—N26—H26B120.0N28—C8—N18117.9 (6)
C1—N11—H11A120.0N18—C8—Se8120.9 (5)
C1—N11—H11B120.0N14—C4—Se4120.6 (5)
H11A—N11—H11B120.0N24—C4—Se4120.2 (5)
C1—N12—H12A120.0N24—C4—N14119.3 (6)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_170K) top
Crystal data top
CH4N2SeDx = 2.134 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6746 reflections
a = 15.17648 (10) Åθ = 3.4–72.1°
c = 12.95625 (12) ŵ = 11.43 mm1
V = 2584.35 (4) Å3T = 170 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
4459 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source4448 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.020
Detector resolution: 10.5384 pixels mm-1θmax = 72.2°, θmin = 3.4°
ω scansh = 1817
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1818
Tmin = 0.193, Tmax = 1.000l = 1413
7405 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0368P)2 + 2.7838P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.025(Δ/σ)max = 0.001
wR(F2) = 0.069Δρmax = 0.79 e Å3
S = 1.11Δρmin = 0.58 e Å3
4459 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00047 (3)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30672 (5)0.35149 (5)0.09698 (5)0.01991 (15)
Se20.39680 (5)0.36003 (5)0.75797 (5)0.02087 (15)
Se30.30504 (5)0.26999 (5)0.42644 (5)0.01957 (14)
Se40.63129 (5)0.60749 (5)0.70746 (5)0.02163 (16)
Se50.72080 (5)0.69430 (5)0.05159 (5)0.01984 (15)
Se60.63328 (5)0.70225 (5)0.38356 (5)0.01977 (15)
Se70.72795 (5)0.37686 (5)0.47637 (6)0.02686 (18)
Se80.29844 (5)0.70000 (5)0.66372 (6)0.02298 (17)
Se91.06947 (5)1.02587 (5)0.45562 (7)0.02830 (17)
C60.7507 (4)0.6911 (4)0.3927 (5)0.0226 (12)
C20.2590 (5)0.3222 (5)0.7550 (5)0.0236 (13)
C90.9337 (5)0.9950 (5)0.4520 (5)0.0256 (13)
C30.4169 (5)0.4027 (5)0.4166 (5)0.0245 (13)
C10.3873 (5)0.2892 (5)0.0948 (5)0.0216 (13)
N160.8061 (4)0.7037 (4)0.3098 (4)0.0297 (12)
H16A0.8597690.6984070.3139460.036*
H16B0.7885300.7173660.2514330.036*
N210.2111 (4)0.3192 (5)0.8408 (5)0.0322 (13)
H21A0.1479910.3025130.8389350.039*
H21B0.2429670.3339640.8987870.039*
N190.8896 (4)1.0059 (5)0.5337 (5)0.0352 (13)
H19A0.8277820.9933790.5300950.042*
H19B0.9223061.0255040.5909940.042*
N290.8819 (5)0.9648 (5)0.3650 (5)0.0423 (16)
H29A0.8201640.9526390.3626990.051*
H29B0.9098400.9572910.3104830.051*
N220.2104 (5)0.2998 (6)0.6676 (5)0.0490 (19)
H22A0.1472520.2831750.6661020.059*
H22B0.2413300.3016990.6113820.059*
N260.7787 (5)0.6703 (5)0.4810 (4)0.0363 (14)
H26A0.8325410.6651540.4842620.044*
H26B0.7431650.6618570.5357080.044*
N110.4367 (4)0.2916 (4)0.0108 (4)0.0274 (12)
H11A0.4728310.2624570.0098830.033*
H11B0.4329530.3223720.0433320.033*
N120.3935 (5)0.2416 (5)0.1778 (4)0.0358 (14)
H12A0.4297830.2126030.1764260.043*
H12B0.3612960.2397710.2331390.043*
N280.3889 (5)0.5972 (6)0.7511 (5)0.0440 (17)
H28A0.4254770.5685230.7506680.053*
H28B0.3594420.5990880.8070870.053*
N250.5251 (4)0.6265 (4)0.1281 (5)0.0309 (12)
H25A0.4597490.5935890.1259640.037*
H25B0.5560880.6600930.1825820.037*
N170.5414 (4)0.2427 (5)0.3885 (5)0.0360 (14)
H17A0.4771150.2000820.3883070.043*
H17B0.5750960.2585570.3316050.043*
N180.4250 (5)0.6336 (6)0.5812 (5)0.0465 (18)
H18A0.4610690.6044460.5830730.056*
H18B0.4192160.6598290.5245480.056*
N230.4766 (4)0.4453 (4)0.4972 (5)0.0337 (13)
H23A0.5283120.5055840.4922460.040*
H23B0.4636750.4127510.5546460.040*
N140.6779 (5)0.8015 (4)0.6450 (5)0.0420 (16)
H14A0.7046200.8663240.6511120.050*
H14B0.6425390.7710670.5911660.050*
N240.7452 (5)0.7969 (4)0.7990 (5)0.0341 (14)
H24A0.7714140.8617300.8040450.041*
H24B0.7544560.7635070.8473000.041*
N270.5340 (4)0.2575 (5)0.5616 (5)0.0397 (15)
H27A0.4697180.2147170.5597220.048*
H27B0.5631340.2834430.6194910.048*
N130.4372 (5)0.4530 (5)0.3291 (5)0.0452 (17)
H13A0.4890400.5133060.3246550.054*
H13B0.3985700.4256870.2763820.054*
C70.5880 (5)0.2835 (4)0.4753 (5)0.0243 (13)
C50.5784 (5)0.6253 (5)0.0472 (5)0.0221 (12)
C80.3780 (5)0.6383 (5)0.6661 (5)0.0274 (14)
C40.6911 (5)0.7490 (5)0.7178 (5)0.0259 (14)
N150.5303 (4)0.5734 (5)0.0362 (5)0.0362 (14)
H15A0.4648650.5406330.0379760.043*
H15B0.5643670.5723390.0887960.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0200 (3)0.0203 (3)0.0214 (4)0.0115 (3)0.0009 (2)0.0001 (3)
Se20.0165 (3)0.0233 (3)0.0225 (4)0.0097 (3)0.0000 (3)0.0023 (2)
Se30.0197 (3)0.0167 (3)0.0215 (3)0.0084 (3)0.0007 (2)0.0004 (3)
Se40.0216 (3)0.0171 (3)0.0241 (4)0.0081 (2)0.0003 (3)0.0000 (2)
Se50.0173 (3)0.0188 (3)0.0233 (4)0.0089 (2)0.0011 (2)0.0004 (2)
Se60.0188 (3)0.0200 (3)0.0221 (4)0.0109 (3)0.0001 (3)0.0001 (2)
Se70.0187 (3)0.0245 (3)0.0266 (4)0.0028 (3)0.0015 (3)0.0005 (3)
Se80.0278 (3)0.0226 (3)0.0235 (4)0.0163 (3)0.0019 (3)0.0009 (3)
Se90.0192 (3)0.0340 (4)0.0325 (4)0.0140 (3)0.0037 (3)0.0089 (3)
C60.025 (3)0.018 (3)0.029 (3)0.014 (2)0.001 (2)0.002 (2)
C20.022 (3)0.029 (3)0.020 (3)0.013 (3)0.000 (2)0.002 (3)
C90.024 (3)0.022 (3)0.030 (4)0.010 (3)0.007 (3)0.004 (3)
C30.028 (3)0.023 (3)0.020 (3)0.011 (3)0.001 (3)0.005 (2)
C10.025 (3)0.024 (3)0.018 (3)0.013 (3)0.002 (2)0.002 (2)
N160.024 (3)0.040 (3)0.029 (3)0.019 (2)0.004 (2)0.004 (2)
N210.023 (3)0.049 (3)0.027 (3)0.019 (3)0.002 (2)0.006 (3)
N190.029 (3)0.056 (4)0.028 (3)0.028 (3)0.001 (2)0.003 (3)
N290.025 (3)0.062 (4)0.033 (4)0.016 (3)0.000 (3)0.010 (3)
N220.027 (3)0.096 (6)0.028 (4)0.034 (3)0.008 (3)0.014 (4)
N260.037 (3)0.068 (4)0.022 (3)0.040 (3)0.001 (2)0.005 (3)
N110.030 (3)0.036 (3)0.023 (3)0.022 (2)0.006 (2)0.006 (2)
N120.050 (4)0.056 (4)0.023 (3)0.042 (3)0.005 (3)0.005 (3)
N280.060 (4)0.066 (4)0.036 (4)0.054 (4)0.016 (3)0.017 (3)
N250.025 (3)0.033 (3)0.032 (3)0.012 (2)0.002 (2)0.007 (2)
N170.021 (3)0.037 (3)0.035 (4)0.004 (2)0.002 (2)0.005 (3)
N180.059 (4)0.087 (5)0.024 (3)0.059 (4)0.012 (3)0.017 (3)
N230.029 (3)0.024 (3)0.034 (3)0.002 (2)0.001 (2)0.002 (2)
N140.068 (4)0.024 (3)0.032 (3)0.022 (3)0.013 (3)0.001 (2)
N240.041 (3)0.018 (3)0.035 (4)0.008 (2)0.002 (3)0.002 (2)
N270.020 (3)0.050 (4)0.036 (4)0.008 (3)0.001 (2)0.003 (3)
N130.060 (4)0.023 (3)0.027 (3)0.002 (3)0.000 (3)0.002 (2)
C70.022 (3)0.024 (3)0.026 (4)0.011 (3)0.002 (2)0.002 (3)
C50.021 (3)0.023 (3)0.021 (3)0.010 (2)0.000 (2)0.000 (2)
C80.028 (3)0.041 (4)0.020 (3)0.022 (3)0.000 (3)0.001 (3)
C40.029 (3)0.028 (3)0.023 (3)0.016 (3)0.009 (3)0.001 (3)
N150.021 (3)0.051 (4)0.029 (3)0.012 (3)0.001 (2)0.012 (3)
Geometric parameters (Å, º) top
Se1—C11.883 (6)N11—H11B0.8600
Se2—C21.873 (6)N12—H12A0.8600
Se3—C31.880 (6)N12—H12B0.8600
Se4—C41.872 (7)N28—H28A0.8600
Se5—C51.873 (6)N28—H28B0.8600
Se6—C61.877 (6)N28—C81.316 (9)
Se7—C71.874 (6)N25—H25A0.8600
Se8—C81.862 (6)N25—H25B0.8600
Se9—C91.872 (6)N25—C51.329 (8)
C6—N161.317 (8)N17—H17A0.8600
C6—N261.313 (8)N17—H17B0.8600
C2—N211.317 (8)N17—C71.307 (9)
C2—N221.300 (9)N18—H18A0.8600
C9—N191.306 (9)N18—H18B0.8600
C9—N291.318 (9)N18—C81.331 (9)
C3—N231.320 (8)N23—H23A0.8600
C3—N131.315 (9)N23—H23B0.8600
C1—N111.311 (8)N14—H14A0.8600
C1—N121.325 (8)N14—H14B0.8600
N16—H16A0.8600N14—C41.313 (9)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.308 (9)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.325 (9)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.322 (9)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.1 (5)C8—N28—H28B120.0
N26—C6—Se6120.8 (5)H25A—N25—H25B120.0
N26—C6—N16119.1 (5)C5—N25—H25A120.0
N21—C2—Se2120.4 (5)C5—N25—H25B120.0
N22—C2—Se2119.9 (5)H17A—N17—H17B120.0
N22—C2—N21119.7 (6)C7—N17—H17A120.0
N19—C9—Se9121.2 (5)C7—N17—H17B120.0
N19—C9—N29118.8 (6)H18A—N18—H18B120.0
N29—C9—Se9119.9 (5)C8—N18—H18A120.0
N23—C3—Se3120.1 (5)C8—N18—H18B120.0
N13—C3—Se3120.3 (5)C3—N23—H23A120.0
N13—C3—N23119.6 (6)C3—N23—H23B120.0
N11—C1—Se1120.3 (5)H23A—N23—H23B120.0
N11—C1—N12119.6 (6)H14A—N14—H14B120.0
N12—C1—Se1120.2 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.3 (5)
H29A—N29—H29B120.0N17—C7—N27118.5 (6)
C2—N22—H22A120.0N27—C7—Se7121.2 (5)
C2—N22—H22B120.0N25—C5—Se5120.5 (5)
H22A—N22—H22B120.0N15—C5—Se5119.8 (5)
C6—N26—H26A120.0N15—C5—N25119.6 (6)
C6—N26—H26B120.0N28—C8—Se8121.2 (5)
H26A—N26—H26B120.0N28—C8—N18118.0 (6)
C1—N11—H11A120.0N18—C8—Se8120.8 (5)
C1—N11—H11B120.0N14—C4—Se4120.7 (5)
H11A—N11—H11B120.0N24—C4—Se4120.3 (5)
C1—N12—H12A120.0N24—C4—N14118.9 (6)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_190K) top
Crystal data top
CH4N2SeDx = 2.128 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6736 reflections
a = 15.1910 (1) Åθ = 3.4–72.3°
c = 12.9669 (1) ŵ = 11.40 mm1
V = 2591.43 (4) Å3T = 190 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3945 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3925 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.037
Detector resolution: 10.5384 pixels mm-1θmax = 72.5°, θmin = 3.4°
ω scansh = 1817
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1818
Tmin = 0.357, Tmax = 1.000l = 1413
6693 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0643P)2 + 0.9764P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max < 0.001
wR(F2) = 0.092Δρmax = 0.93 e Å3
S = 1.08Δρmin = 0.60 e Å3
3945 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00057 (5)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30657 (6)0.35137 (6)0.09706 (5)0.02247 (18)
Se20.39638 (6)0.35999 (6)0.75795 (5)0.02338 (19)
Se30.30500 (6)0.27010 (5)0.42643 (6)0.02181 (18)
Se40.63111 (6)0.60742 (6)0.70730 (5)0.0239 (2)
Se50.72083 (5)0.69421 (5)0.05141 (6)0.02212 (18)
Se60.63330 (6)0.70216 (6)0.38338 (5)0.02224 (18)
Se70.72802 (6)0.37685 (7)0.47603 (7)0.0300 (2)
Se80.29840 (6)0.70002 (5)0.66368 (7)0.0254 (2)
Se91.06957 (6)1.02643 (7)0.45665 (8)0.0315 (2)
C60.7501 (5)0.6907 (5)0.3919 (6)0.0240 (13)
C20.2585 (5)0.3210 (6)0.7557 (6)0.0260 (15)
C90.9339 (5)0.9957 (5)0.4519 (6)0.0274 (15)
C30.4157 (5)0.4032 (5)0.4167 (5)0.0266 (15)
C10.3871 (6)0.2897 (6)0.0948 (6)0.0251 (15)
N160.8056 (5)0.7030 (5)0.3098 (5)0.0327 (14)
H16A0.8590120.6973990.3145130.039*
H16B0.7884920.7167010.2513370.039*
N210.2106 (5)0.3185 (6)0.8413 (5)0.0364 (15)
H21A0.1476330.3019540.8392800.044*
H21B0.2423980.3333450.8992900.044*
N190.8901 (5)1.0062 (6)0.5346 (5)0.0360 (15)
H19A0.8279720.9926500.5319120.043*
H19B0.9235381.0267810.5914070.043*
N290.8822 (5)0.9645 (6)0.3666 (6)0.0436 (18)
H29A0.8201260.9511390.3648240.052*
H29B0.9101000.9572920.3119710.052*
N220.2106 (6)0.2985 (8)0.6681 (6)0.058 (3)
H22A0.1475810.2819930.6660050.070*
H22B0.2418800.3001660.6122430.070*
N260.7782 (5)0.6696 (6)0.4811 (5)0.0413 (17)
H26A0.8319140.6642960.4842860.050*
H26B0.7427670.6612800.5357170.050*
N110.4368 (5)0.2920 (5)0.0112 (5)0.0309 (14)
H11A0.4725140.2623650.0106020.037*
H11B0.4337590.3230030.0429040.037*
N120.3934 (6)0.2411 (6)0.1772 (5)0.0405 (17)
H12A0.4294500.2120080.1750280.049*
H12B0.3613060.2387830.2327760.049*
N280.3878 (6)0.5967 (7)0.7505 (6)0.048 (2)
H28A0.4240100.5676840.7495800.058*
H28B0.3584630.5983010.8066620.058*
N250.5249 (5)0.6267 (5)0.1272 (5)0.0347 (15)
H25A0.4595880.5934850.1239220.042*
H25B0.5547090.6603000.1820060.042*
N170.5412 (5)0.2427 (5)0.3879 (5)0.0377 (16)
H17A0.4769350.2004610.3874520.045*
H17B0.5751020.2585030.3311830.045*
N180.4246 (6)0.6339 (8)0.5819 (5)0.053 (2)
H18A0.4602100.6042070.5836810.064*
H18B0.4194520.6605610.5253270.064*
N230.4760 (5)0.4455 (5)0.4975 (6)0.0391 (16)
H23A0.5282210.5053420.4923910.047*
H23B0.4628510.4129510.5548810.047*
N140.6779 (6)0.8008 (5)0.6452 (6)0.0453 (19)
H14A0.7047210.8656100.6508870.054*
H14B0.6424200.7700620.5916490.054*
N240.7449 (6)0.7965 (5)0.7989 (6)0.0392 (17)
H24A0.7714630.8613400.8038550.047*
H24B0.7540170.7631020.8472740.047*
N270.5341 (5)0.2577 (6)0.5602 (5)0.0423 (17)
H27A0.4698260.2152530.5579480.051*
H27B0.5629640.2832970.6182300.051*
N130.4360 (7)0.4528 (5)0.3301 (6)0.055 (2)
H13A0.4883340.5126510.3253550.066*
H13B0.3971550.4256930.2775040.066*
C70.5878 (6)0.2833 (6)0.4753 (6)0.0289 (15)
C50.5796 (5)0.6262 (5)0.0476 (6)0.0235 (14)
C80.3775 (6)0.6385 (6)0.6667 (6)0.0327 (17)
C40.6910 (6)0.7489 (6)0.7182 (6)0.0287 (16)
N150.5308 (5)0.5733 (6)0.0361 (5)0.0390 (17)
H15A0.4654220.5406520.0375560.047*
H15B0.5646150.5718340.0885740.047*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0226 (4)0.0229 (4)0.0241 (4)0.0130 (3)0.0008 (3)0.0001 (3)
Se20.0180 (3)0.0262 (4)0.0252 (4)0.0105 (3)0.0000 (3)0.0026 (3)
Se30.0218 (4)0.0181 (3)0.0243 (4)0.0090 (3)0.0010 (3)0.0004 (3)
Se40.0237 (4)0.0192 (3)0.0266 (5)0.0091 (3)0.0002 (3)0.0001 (3)
Se50.0188 (3)0.0208 (3)0.0264 (4)0.0096 (3)0.0014 (3)0.0005 (3)
Se60.0209 (4)0.0221 (4)0.0257 (4)0.0122 (3)0.0006 (3)0.0001 (3)
Se70.0206 (4)0.0274 (4)0.0300 (5)0.0030 (3)0.0017 (3)0.0008 (3)
Se80.0308 (4)0.0250 (4)0.0259 (5)0.0180 (3)0.0021 (3)0.0010 (3)
Se90.0213 (4)0.0379 (4)0.0364 (5)0.0156 (3)0.0041 (3)0.0095 (3)
C60.028 (3)0.018 (3)0.029 (4)0.014 (3)0.005 (3)0.002 (3)
C20.022 (3)0.035 (4)0.024 (4)0.017 (3)0.001 (3)0.004 (3)
C90.026 (3)0.027 (4)0.030 (4)0.013 (3)0.003 (3)0.003 (3)
C30.029 (3)0.024 (3)0.023 (4)0.010 (3)0.004 (3)0.001 (3)
C10.030 (4)0.024 (3)0.022 (4)0.013 (3)0.000 (3)0.000 (3)
N160.027 (3)0.049 (4)0.028 (3)0.023 (3)0.005 (3)0.006 (3)
N210.028 (3)0.054 (4)0.031 (4)0.023 (3)0.002 (3)0.005 (3)
N190.032 (3)0.057 (4)0.026 (4)0.027 (3)0.003 (3)0.002 (3)
N290.030 (3)0.066 (5)0.030 (4)0.020 (4)0.001 (3)0.013 (3)
N220.032 (4)0.119 (8)0.029 (4)0.042 (5)0.011 (3)0.021 (4)
N260.037 (4)0.075 (5)0.030 (4)0.041 (4)0.001 (3)0.006 (3)
N110.033 (3)0.039 (3)0.029 (4)0.024 (3)0.007 (3)0.008 (3)
N120.058 (5)0.066 (5)0.025 (4)0.051 (4)0.003 (3)0.005 (3)
N280.062 (5)0.076 (6)0.036 (4)0.057 (5)0.016 (4)0.023 (4)
N250.026 (3)0.040 (4)0.032 (4)0.011 (3)0.007 (3)0.005 (3)
N170.023 (3)0.038 (4)0.036 (4)0.004 (3)0.004 (3)0.004 (3)
N180.070 (5)0.103 (7)0.025 (4)0.072 (6)0.019 (4)0.025 (4)
N230.036 (4)0.028 (3)0.036 (4)0.003 (3)0.003 (3)0.004 (3)
N140.071 (5)0.026 (3)0.036 (4)0.022 (4)0.011 (4)0.002 (3)
N240.053 (4)0.021 (3)0.038 (4)0.014 (3)0.005 (3)0.001 (3)
N270.022 (3)0.057 (4)0.033 (4)0.009 (3)0.003 (3)0.008 (3)
N130.074 (6)0.024 (3)0.033 (4)0.000 (4)0.007 (4)0.001 (3)
C70.027 (3)0.030 (4)0.032 (4)0.016 (3)0.002 (3)0.005 (3)
C50.025 (3)0.023 (3)0.021 (3)0.010 (3)0.002 (3)0.001 (3)
C80.033 (4)0.046 (4)0.029 (4)0.028 (4)0.007 (3)0.003 (3)
C40.032 (4)0.030 (4)0.022 (4)0.014 (3)0.008 (3)0.004 (3)
N150.020 (3)0.058 (4)0.029 (4)0.012 (3)0.001 (3)0.012 (3)
Geometric parameters (Å, º) top
Se1—C11.876 (7)N11—H11B0.8600
Se2—C21.870 (7)N12—H12A0.8600
Se3—C31.880 (7)N12—H12B0.8600
Se4—C41.874 (8)N28—H28A0.8600
Se5—C51.859 (7)N28—H28B0.8600
Se6—C61.870 (7)N28—C81.308 (11)
Se7—C71.879 (7)N25—H25A0.8600
Se8—C81.854 (7)N25—H25B0.8600
Se9—C91.872 (7)N25—C51.328 (10)
C6—N161.311 (10)N17—H17A0.8600
C6—N261.327 (9)N17—H17B0.8600
C2—N211.317 (10)N17—C71.315 (11)
C2—N221.299 (10)N18—H18A0.8600
C9—N191.314 (10)N18—H18B0.8600
C9—N291.301 (11)N18—C81.334 (10)
C3—N231.327 (10)N23—H23A0.8600
C3—N131.300 (10)N23—H23B0.8600
C1—N111.312 (10)N14—H14A0.8600
C1—N121.329 (10)N14—H14B0.8600
N16—H16A0.8600N14—C41.309 (10)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.302 (11)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.308 (10)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.333 (10)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.7 (5)C8—N28—H28B120.0
N16—C6—N26118.7 (6)H25A—N25—H25B120.0
N26—C6—Se6120.6 (5)C5—N25—H25A120.0
N21—C2—Se2120.7 (5)C5—N25—H25B120.0
N22—C2—Se2119.2 (6)H17A—N17—H17B120.0
N22—C2—N21120.1 (7)C7—N17—H17A120.0
N19—C9—Se9120.3 (6)C7—N17—H17B120.0
N29—C9—Se9120.5 (6)H18A—N18—H18B120.0
N29—C9—N19119.2 (7)C8—N18—H18A120.0
N23—C3—Se3119.8 (5)C8—N18—H18B120.0
N13—C3—Se3120.4 (6)C3—N23—H23A120.0
N13—C3—N23119.7 (7)C3—N23—H23B120.0
N11—C1—Se1120.7 (5)H23A—N23—H23B120.0
N11—C1—N12118.6 (7)H14A—N14—H14B120.0
N12—C1—Se1120.7 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.0 (6)
H29A—N29—H29B120.0N27—C7—Se7121.6 (6)
C2—N22—H22A120.0N27—C7—N17118.4 (7)
C2—N22—H22B120.0N25—C5—Se5121.9 (5)
H22A—N22—H22B120.0N25—C5—N15118.3 (7)
C6—N26—H26A120.0N15—C5—Se5119.8 (5)
C6—N26—H26B120.0N28—C8—Se8121.9 (6)
H26A—N26—H26B120.0N28—C8—N18117.5 (7)
C1—N11—H11A120.0N18—C8—Se8120.6 (6)
C1—N11—H11B120.0N14—C4—Se4120.2 (6)
H11A—N11—H11B120.0N24—C4—Se4120.5 (6)
C1—N12—H12A120.0N24—C4—N14119.3 (7)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_210K) top
Crystal data top
CH4N2SeDx = 2.122 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6757 reflections
a = 15.2065 (1) Åθ = 3.4–72.3°
c = 12.9770 (1) ŵ = 11.37 mm1
V = 2598.74 (4) Å3T = 210 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3970 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3937 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.037
Detector resolution: 10.5384 pixels mm-1θmax = 72.5°, θmin = 3.4°
ω scansh = 1618
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1818
Tmin = 0.399, Tmax = 1.000l = 1314
6773 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0592P)2 + 1.765P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max < 0.001
wR(F2) = 0.095Δρmax = 0.59 e Å3
S = 1.13Δρmin = 0.61 e Å3
3970 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00075 (6)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30649 (6)0.35131 (6)0.09711 (6)0.02522 (19)
Se20.39603 (6)0.36002 (6)0.75804 (6)0.0261 (2)
Se30.30493 (6)0.27021 (6)0.42647 (6)0.02469 (19)
Se40.63110 (6)0.60739 (6)0.70724 (6)0.0269 (2)
Se50.72092 (6)0.69408 (6)0.05120 (6)0.0248 (2)
Se60.63338 (6)0.70210 (6)0.38322 (6)0.02499 (19)
Se70.72815 (6)0.37680 (7)0.47558 (7)0.0338 (2)
Se80.29835 (6)0.70003 (6)0.66373 (7)0.0286 (2)
Se91.06965 (6)1.02694 (7)0.45769 (9)0.0351 (2)
C60.7498 (5)0.6899 (5)0.3919 (6)0.0264 (14)
C20.2581 (6)0.3201 (6)0.7556 (6)0.0293 (17)
C90.9336 (6)0.9957 (6)0.4523 (7)0.0318 (17)
C30.4151 (6)0.4032 (6)0.4169 (6)0.0318 (17)
C10.3866 (6)0.2897 (6)0.0947 (6)0.0272 (16)
N160.8047 (5)0.7017 (6)0.3092 (5)0.0364 (16)
H16A0.8579240.6958040.3134300.044*
H16B0.7872410.7152190.2508730.044*
N210.2105 (5)0.3180 (6)0.8412 (6)0.0414 (17)
H21A0.1476390.3017110.8391360.050*
H21B0.2422910.3328540.8990500.050*
N190.8901 (5)1.0068 (6)0.5350 (6)0.0394 (17)
H19A0.8280290.9933810.5323520.047*
H19B0.9236061.0276260.5916490.047*
N290.8821 (6)0.9644 (7)0.3680 (6)0.050 (2)
H29A0.8200970.9511930.3663320.060*
H29B0.9096970.9567990.3134300.060*
N220.2099 (6)0.2976 (9)0.6691 (7)0.067 (3)
H22A0.1470120.2814080.6675710.081*
H22B0.2405900.2988410.6130370.081*
N260.7779 (6)0.6692 (7)0.4806 (6)0.047 (2)
H26A0.8313420.6635300.4837200.057*
H26B0.7427410.6613280.5352710.057*
N110.4368 (5)0.2922 (6)0.0113 (5)0.0339 (15)
H11A0.4729510.2631390.0110420.041*
H11B0.4335960.3229010.0429530.041*
N120.3932 (7)0.2416 (6)0.1771 (5)0.0434 (19)
H12A0.4298290.2131030.1750540.052*
H12B0.3609970.2390160.2324890.052*
N280.3876 (7)0.5966 (8)0.7508 (7)0.054 (2)
H28A0.4236290.5674870.7502830.065*
H28B0.3579810.5983400.8065820.065*
N250.5253 (5)0.6264 (6)0.1272 (6)0.0394 (17)
H25A0.4600980.5932620.1241550.047*
H25B0.5553490.6598620.1819270.047*
N170.5409 (5)0.2422 (6)0.3878 (6)0.0434 (19)
H17A0.4765700.2002830.3876720.052*
H17B0.5744390.2573710.3309270.052*
N180.4246 (7)0.6337 (9)0.5825 (6)0.060 (3)
H18A0.4601550.6040830.5843440.072*
H18B0.4195140.6604140.5259770.072*
N230.4751 (6)0.4460 (5)0.4971 (6)0.0433 (17)
H23A0.5269110.5060190.4917350.052*
H23B0.4623340.4138140.5545960.052*
N140.6776 (7)0.8005 (6)0.6451 (6)0.052 (2)
H14A0.7041940.8651800.6509770.063*
H14B0.6423750.7698780.5914250.063*
N240.7445 (6)0.7963 (5)0.7990 (6)0.0436 (19)
H24A0.7707190.8610660.8039610.052*
H24B0.7536470.7630310.8472800.052*
N270.5340 (6)0.2581 (7)0.5601 (6)0.049 (2)
H27A0.4698120.2159160.5575310.059*
H27B0.5626540.2835770.6181870.059*
N130.4352 (7)0.4527 (6)0.3303 (6)0.059 (3)
H13A0.4871770.5127120.3255900.071*
H13B0.3965180.4254220.2776980.071*
C70.5883 (6)0.2834 (6)0.4754 (7)0.0339 (17)
C50.5797 (6)0.6259 (6)0.0473 (6)0.0259 (15)
C80.3777 (7)0.6382 (7)0.6666 (7)0.0367 (19)
C40.6907 (6)0.7486 (6)0.7179 (6)0.0316 (17)
N150.5311 (5)0.5735 (6)0.0363 (6)0.0443 (19)
H15A0.4658000.5408060.0377770.053*
H15B0.5649180.5721780.0888060.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0252 (4)0.0251 (4)0.0278 (4)0.0145 (3)0.0007 (3)0.0002 (3)
Se20.0202 (4)0.0289 (4)0.0286 (5)0.0118 (3)0.0002 (3)0.0026 (3)
Se30.0242 (4)0.0200 (4)0.0282 (4)0.0097 (3)0.0009 (3)0.0006 (3)
Se40.0264 (4)0.0212 (4)0.0305 (5)0.0099 (3)0.0002 (3)0.0002 (3)
Se50.0211 (4)0.0230 (4)0.0298 (4)0.0107 (3)0.0014 (3)0.0006 (3)
Se60.0229 (4)0.0247 (4)0.0295 (4)0.0135 (3)0.0007 (3)0.0001 (3)
Se70.0229 (4)0.0303 (4)0.0349 (5)0.0033 (3)0.0019 (3)0.0008 (4)
Se80.0342 (5)0.0278 (4)0.0297 (5)0.0199 (4)0.0023 (3)0.0011 (3)
Se90.0235 (4)0.0414 (5)0.0413 (5)0.0170 (4)0.0044 (3)0.0098 (4)
C60.027 (3)0.025 (3)0.031 (4)0.015 (3)0.004 (3)0.001 (3)
C20.025 (4)0.037 (4)0.030 (4)0.018 (3)0.001 (3)0.005 (3)
C90.028 (4)0.029 (4)0.037 (5)0.014 (3)0.003 (3)0.003 (3)
C30.032 (4)0.028 (4)0.030 (4)0.011 (3)0.005 (3)0.002 (3)
C10.029 (4)0.026 (4)0.025 (4)0.013 (3)0.000 (3)0.001 (3)
N160.033 (3)0.050 (4)0.033 (4)0.026 (3)0.007 (3)0.006 (3)
N210.032 (4)0.059 (5)0.036 (4)0.025 (4)0.001 (3)0.002 (4)
N190.033 (3)0.061 (5)0.032 (4)0.029 (3)0.005 (3)0.004 (3)
N290.032 (4)0.081 (6)0.033 (4)0.025 (4)0.004 (3)0.017 (4)
N220.037 (4)0.143 (10)0.034 (5)0.054 (6)0.012 (4)0.022 (5)
N260.043 (4)0.083 (6)0.034 (4)0.046 (4)0.000 (3)0.006 (4)
N110.033 (3)0.047 (4)0.032 (4)0.029 (3)0.007 (3)0.008 (3)
N120.063 (5)0.069 (5)0.027 (4)0.054 (5)0.005 (3)0.007 (3)
N280.074 (6)0.082 (6)0.041 (5)0.066 (6)0.019 (4)0.026 (4)
N250.029 (3)0.047 (4)0.036 (4)0.014 (3)0.006 (3)0.007 (3)
N170.028 (3)0.045 (4)0.041 (5)0.006 (3)0.004 (3)0.006 (3)
N180.074 (6)0.119 (8)0.031 (4)0.081 (7)0.018 (4)0.024 (5)
N230.043 (4)0.033 (4)0.039 (4)0.007 (3)0.003 (3)0.004 (3)
N140.084 (6)0.028 (4)0.041 (4)0.025 (4)0.014 (4)0.002 (3)
N240.059 (5)0.022 (3)0.042 (5)0.015 (3)0.008 (4)0.000 (3)
N270.027 (4)0.066 (5)0.039 (5)0.011 (4)0.002 (3)0.007 (4)
N130.077 (6)0.028 (4)0.036 (4)0.001 (4)0.007 (4)0.003 (3)
C70.026 (4)0.033 (4)0.039 (5)0.013 (3)0.004 (3)0.006 (4)
C50.027 (4)0.026 (4)0.023 (4)0.012 (3)0.001 (3)0.001 (3)
C80.040 (5)0.051 (5)0.032 (5)0.033 (4)0.007 (4)0.006 (4)
C40.038 (4)0.031 (4)0.025 (4)0.016 (3)0.006 (3)0.000 (3)
N150.024 (3)0.062 (5)0.031 (4)0.010 (3)0.001 (3)0.011 (3)
Geometric parameters (Å, º) top
Se1—C11.872 (8)N11—H11B0.8600
Se2—C21.869 (7)N12—H12A0.8600
Se3—C31.878 (8)N12—H12B0.8600
Se4—C41.872 (8)N28—H28A0.8600
Se5—C51.860 (8)N28—H28B0.8600
Se6—C61.873 (7)N28—C81.309 (11)
Se7—C71.876 (8)N25—H25A0.8600
Se8—C81.864 (8)N25—H25B0.8600
Se9—C91.878 (8)N25—C51.329 (10)
C6—N161.315 (10)N17—H17A0.8600
C6—N261.320 (10)N17—H17B0.8600
C2—N211.317 (11)N17—C71.324 (12)
C2—N221.290 (11)N18—H18A0.8600
C9—N191.316 (11)N18—H18B0.8600
C9—N291.291 (12)N18—C81.324 (11)
C3—N231.321 (11)N23—H23A0.8600
C3—N131.301 (11)N23—H23B0.8600
C1—N111.314 (10)N14—H14A0.8600
C1—N121.327 (10)N14—H14B0.8600
N16—H16A0.8600N14—C41.309 (11)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.307 (11)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.311 (12)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.330 (11)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.3 (6)C8—N28—H28B120.0
N16—C6—N26119.0 (7)H25A—N25—H25B120.0
N26—C6—Se6120.7 (6)C5—N25—H25A120.0
N21—C2—Se2120.5 (6)C5—N25—H25B120.0
N22—C2—Se2119.8 (6)H17A—N17—H17B120.0
N22—C2—N21119.6 (7)C7—N17—H17A120.0
N19—C9—Se9119.9 (6)C7—N17—H17B120.0
N29—C9—Se9120.9 (6)H18A—N18—H18B120.0
N29—C9—N19119.1 (8)C8—N18—H18A120.0
N23—C3—Se3120.2 (6)C8—N18—H18B120.0
N13—C3—Se3120.3 (6)C3—N23—H23A120.0
N13—C3—N23119.4 (7)C3—N23—H23B120.0
N11—C1—Se1120.9 (6)H23A—N23—H23B120.0
N11—C1—N12118.4 (7)H14A—N14—H14B120.0
N12—C1—Se1120.7 (6)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.1 (6)
H29A—N29—H29B120.0N27—C7—Se7122.0 (6)
C2—N22—H22A120.0N27—C7—N17117.8 (8)
C2—N22—H22B120.0N25—C5—Se5121.6 (6)
H22A—N22—H22B120.0N25—C5—N15118.6 (7)
C6—N26—H26A120.0N15—C5—Se5119.8 (6)
C6—N26—H26B120.0N28—C8—Se8121.3 (6)
H26A—N26—H26B120.0N28—C8—N18117.9 (8)
C1—N11—H11A120.0N18—C8—Se8120.7 (6)
C1—N11—H11B120.0N14—C4—Se4120.4 (7)
H11A—N11—H11B120.0N24—C4—Se4120.4 (6)
C1—N12—H12A120.0N24—C4—N14119.2 (8)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_230K) top
Crystal data top
CH4N2SeDx = 2.116 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6730 reflections
a = 15.2222 (1) Åθ = 3.3–72.2°
c = 12.9882 (1) ŵ = 11.33 mm1
V = 2606.36 (4) Å3T = 230 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3976 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3955 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.031
Detector resolution: 10.5384 pixels mm-1θmax = 72.3°, θmin = 3.4°
ω scansh = 1816
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1818
Tmin = 0.166, Tmax = 1.000l = 1413
6843 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.060P)2 + 1.262P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max = 0.001
wR(F2) = 0.090Δρmax = 0.89 e Å3
S = 1.09Δρmin = 0.68 e Å3
3976 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00065 (5)
1 restraintAbsolute structure: Classical Flack method preferred over Parsons because s.u. lower.
Primary atom site location: dualAbsolute structure parameter: 0.00 (4)
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30642 (5)0.35126 (6)0.09714 (5)0.02672 (18)
Se20.39569 (6)0.36011 (6)0.75796 (5)0.02792 (19)
Se30.30497 (6)0.27042 (5)0.42647 (6)0.02614 (18)
Se40.63106 (6)0.60742 (6)0.70725 (5)0.0288 (2)
Se50.72097 (5)0.69394 (5)0.05110 (6)0.02652 (19)
Se60.63343 (6)0.70204 (6)0.38315 (5)0.02647 (18)
Se70.72825 (6)0.37668 (7)0.47495 (7)0.0363 (2)
Se80.29832 (6)0.70011 (5)0.66405 (7)0.0307 (2)
Se91.06981 (6)1.02755 (7)0.45860 (8)0.0371 (2)
C60.7494 (5)0.6896 (5)0.3910 (5)0.0279 (13)
C20.2576 (6)0.3195 (6)0.7551 (6)0.0334 (16)
C90.9341 (6)0.9960 (6)0.4527 (6)0.0336 (16)
C30.4149 (5)0.4029 (5)0.4161 (6)0.0342 (16)
C10.3869 (6)0.2899 (6)0.0942 (5)0.0291 (15)
N160.8049 (5)0.7010 (5)0.3094 (5)0.0390 (14)
H16A0.8574350.6941550.3143550.047*
H16B0.7886660.7154350.2509140.047*
N210.2100 (5)0.3168 (6)0.8405 (5)0.0439 (16)
H21A0.1469820.2999540.8385970.053*
H21B0.2417700.3319100.8983420.053*
N190.8894 (5)1.0072 (6)0.5360 (6)0.0475 (17)
H19A0.8274820.9938280.5328040.057*
H19B0.9225061.0279220.5928330.057*
N290.8824 (6)0.9647 (7)0.3682 (6)0.056 (2)
H29A0.8205480.9517210.3666140.067*
H29B0.9098940.9570060.3137160.067*
N220.2092 (6)0.2967 (9)0.6689 (6)0.072 (3)
H22A0.1462010.2798820.6676270.086*
H22B0.2398140.2982090.6127550.086*
N260.7768 (6)0.6675 (6)0.4798 (5)0.0483 (18)
H26A0.8296710.6609560.4827780.058*
H26B0.7416200.6595850.5344170.058*
N110.4364 (5)0.2917 (5)0.0105 (5)0.0363 (14)
H11A0.4719050.2620630.0099260.044*
H11B0.4332420.3225240.0436240.044*
N120.3931 (6)0.2419 (6)0.1764 (5)0.0479 (18)
H12A0.4289230.2127070.1744630.058*
H12B0.3611820.2400130.2317740.058*
N280.3870 (7)0.5968 (7)0.7511 (6)0.056 (2)
H28A0.4226760.5673620.7512230.068*
H28B0.3573760.5991410.8065240.068*
N250.5259 (5)0.6263 (6)0.1268 (6)0.0443 (16)
H25A0.4607220.5934670.1242640.053*
H25B0.5563720.6595860.1814300.053*
N170.5419 (5)0.2427 (6)0.3870 (6)0.0470 (18)
H17A0.4775710.2012480.3865490.056*
H17B0.5757980.2576280.3305080.056*
N180.4242 (7)0.6335 (8)0.5826 (6)0.063 (3)
H18A0.4593150.6034440.5852160.076*
H18B0.4196320.6599150.5257890.076*
N230.4746 (5)0.4457 (5)0.4969 (5)0.0452 (16)
H23A0.5256210.5062350.4922100.054*
H23B0.4622600.4130330.5540020.054*
N140.6778 (7)0.8003 (5)0.6439 (6)0.058 (2)
H14A0.7046180.8649860.6494350.070*
H14B0.6429170.7696160.5901640.070*
N240.7429 (6)0.7956 (5)0.7986 (6)0.0489 (19)
H24A0.7694190.8602700.8034540.059*
H24B0.7512650.7621560.8473160.059*
N270.5347 (5)0.2588 (7)0.5590 (6)0.057 (2)
H27A0.4704640.2171940.5565150.068*
H27B0.5635080.2843010.6169490.068*
N130.4345 (7)0.4531 (5)0.3308 (6)0.063 (2)
H13A0.4856720.5135250.3269160.075*
H13B0.3962280.4259850.2779980.075*
C70.5887 (6)0.2833 (6)0.4746 (6)0.0352 (16)
C50.5800 (5)0.6257 (5)0.0458 (5)0.0275 (14)
C80.3777 (6)0.6388 (6)0.6651 (6)0.0358 (16)
C40.6900 (6)0.7482 (6)0.7178 (6)0.0342 (16)
N150.5307 (5)0.5739 (6)0.0365 (5)0.0499 (19)
H15A0.4654560.5416000.0372240.060*
H15B0.5637530.5722970.0894850.060*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0285 (4)0.0287 (4)0.0258 (4)0.0164 (3)0.0006 (3)0.0001 (3)
Se20.0235 (3)0.0325 (4)0.0272 (4)0.0136 (3)0.0000 (3)0.0026 (3)
Se30.0276 (4)0.0231 (3)0.0260 (4)0.0114 (3)0.0007 (3)0.0008 (3)
Se40.0302 (4)0.0242 (3)0.0289 (5)0.0113 (3)0.0001 (3)0.0001 (3)
Se50.0242 (3)0.0269 (3)0.0280 (4)0.0125 (3)0.0015 (3)0.0006 (3)
Se60.0265 (4)0.0283 (4)0.0269 (4)0.0155 (3)0.0004 (3)0.0000 (3)
Se70.0264 (4)0.0343 (4)0.0340 (5)0.0044 (3)0.0020 (3)0.0008 (3)
Se80.0385 (4)0.0315 (4)0.0283 (5)0.0223 (3)0.0024 (3)0.0013 (3)
Se90.0271 (4)0.0459 (5)0.0392 (5)0.0190 (4)0.0045 (3)0.0103 (4)
C60.026 (3)0.029 (3)0.032 (4)0.016 (3)0.002 (3)0.004 (3)
C20.033 (4)0.046 (4)0.028 (4)0.025 (3)0.000 (3)0.003 (3)
C90.033 (3)0.032 (4)0.036 (4)0.018 (3)0.007 (3)0.003 (3)
C30.035 (4)0.032 (4)0.029 (4)0.012 (3)0.003 (3)0.007 (3)
C10.035 (4)0.032 (4)0.023 (4)0.018 (3)0.001 (3)0.002 (3)
N160.038 (3)0.051 (4)0.034 (4)0.027 (3)0.005 (3)0.003 (3)
N210.036 (3)0.070 (5)0.032 (4)0.031 (3)0.003 (3)0.002 (3)
N190.038 (3)0.076 (5)0.039 (4)0.037 (4)0.002 (3)0.001 (3)
N290.035 (4)0.092 (6)0.039 (4)0.029 (4)0.003 (3)0.012 (4)
N220.040 (4)0.154 (10)0.033 (4)0.057 (5)0.006 (3)0.012 (5)
N260.049 (4)0.086 (6)0.033 (4)0.051 (4)0.001 (3)0.005 (3)
N110.039 (3)0.049 (4)0.031 (4)0.030 (3)0.006 (3)0.004 (3)
N120.066 (5)0.074 (5)0.030 (4)0.055 (4)0.005 (3)0.008 (3)
N280.077 (5)0.084 (6)0.041 (4)0.065 (5)0.020 (4)0.022 (4)
N250.034 (3)0.052 (4)0.041 (4)0.017 (3)0.002 (3)0.011 (3)
N170.029 (3)0.055 (4)0.037 (4)0.007 (3)0.001 (3)0.007 (3)
N180.080 (6)0.120 (8)0.031 (4)0.081 (6)0.015 (4)0.021 (4)
N230.043 (4)0.035 (3)0.039 (4)0.006 (3)0.001 (3)0.001 (3)
N140.095 (6)0.032 (3)0.046 (4)0.030 (4)0.015 (4)0.001 (3)
N240.068 (5)0.028 (3)0.042 (4)0.017 (3)0.011 (4)0.000 (3)
N270.031 (3)0.081 (6)0.043 (4)0.016 (4)0.002 (3)0.007 (4)
N130.084 (6)0.027 (3)0.038 (4)0.003 (4)0.003 (4)0.005 (3)
C70.028 (3)0.036 (4)0.038 (4)0.013 (3)0.006 (3)0.007 (3)
C50.030 (3)0.030 (3)0.021 (3)0.014 (3)0.000 (3)0.004 (3)
C80.041 (4)0.055 (5)0.023 (4)0.033 (4)0.003 (3)0.001 (3)
C40.043 (4)0.031 (4)0.027 (4)0.018 (3)0.008 (3)0.003 (3)
N150.027 (3)0.072 (5)0.034 (4)0.013 (3)0.004 (3)0.013 (3)
Geometric parameters (Å, º) top
Se1—C11.877 (7)N11—H11B0.8600
Se2—C21.871 (7)N12—H12A0.8600
Se3—C31.874 (7)N12—H12B0.8600
Se4—C41.869 (7)N28—H28A0.8600
Se5—C51.860 (7)N28—H28B0.8600
Se6—C61.869 (6)N28—C81.329 (11)
Se7—C71.875 (7)N25—H25A0.8600
Se8—C81.859 (7)N25—H25B0.8600
Se9—C91.873 (7)N25—C51.339 (10)
C6—N161.312 (10)N17—H17A0.8600
C6—N261.326 (10)N17—H17B0.8600
C2—N211.315 (10)N17—C71.319 (11)
C2—N221.289 (11)N18—H18A0.8600
C9—N191.334 (10)N18—H18B0.8600
C9—N291.295 (11)N18—C81.309 (10)
C3—N231.326 (10)N23—H23A0.8600
C3—N131.293 (11)N23—H23B0.8600
C1—N111.314 (10)N14—H14A0.8600
C1—N121.323 (10)N14—H14B0.8600
N16—H16A0.8600N14—C41.316 (11)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.300 (11)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.307 (11)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.318 (10)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6121.4 (5)C8—N28—H28B120.0
N16—C6—N26118.2 (6)H25A—N25—H25B120.0
N26—C6—Se6120.4 (5)C5—N25—H25A120.0
N21—C2—Se2120.3 (6)C5—N25—H25B120.0
N22—C2—Se2120.2 (6)H17A—N17—H17B120.0
N22—C2—N21119.5 (7)C7—N17—H17A120.0
N19—C9—Se9120.1 (6)C7—N17—H17B120.0
N29—C9—Se9121.2 (6)H18A—N18—H18B120.0
N29—C9—N19118.6 (7)C8—N18—H18A120.0
N23—C3—Se3119.7 (6)C8—N18—H18B120.0
N13—C3—Se3121.0 (6)C3—N23—H23A120.0
N13—C3—N23119.3 (7)C3—N23—H23B120.0
N11—C1—Se1121.1 (5)H23A—N23—H23B120.0
N11—C1—N12118.8 (7)H14A—N14—H14B120.0
N12—C1—Se1120.1 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7119.9 (6)
H29A—N29—H29B120.0N27—C7—Se7121.7 (6)
C2—N22—H22A120.0N27—C7—N17118.3 (7)
C2—N22—H22B120.0N25—C5—Se5120.6 (5)
H22A—N22—H22B120.0N15—C5—Se5121.1 (5)
C6—N26—H26A120.0N15—C5—N25118.3 (7)
C6—N26—H26B120.0N28—C8—Se8120.0 (5)
H26A—N26—H26B120.0N18—C8—Se8122.2 (6)
C1—N11—H11A120.0N18—C8—N28117.8 (7)
C1—N11—H11B120.0N14—C4—Se4120.4 (6)
H11A—N11—H11B120.0N24—C4—Se4120.3 (6)
C1—N12—H12A120.0N24—C4—N14119.3 (7)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_250K) top
Crystal data top
CH4N2SeDx = 2.110 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6687 reflections
a = 15.23887 (11) Åθ = 3.3–72.2°
c = 12.99870 (13) ŵ = 11.30 mm1
V = 2614.18 (5) Å3T = 250 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
4004 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3972 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.037
Detector resolution: 10.5384 pixels mm-1θmax = 72.4°, θmin = 3.4°
ω scansh = 1818
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1816
Tmin = 0.195, Tmax = 1.000l = 1413
6882 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0593P)2 + 0.467P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max = 0.001
wR(F2) = 0.090Δρmax = 0.67 e Å3
S = 1.09Δρmin = 0.48 e Å3
4004 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00076 (6)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30629 (5)0.35125 (6)0.09713 (5)0.03035 (18)
Se20.39526 (6)0.36009 (6)0.75806 (5)0.03164 (19)
Se30.30491 (5)0.27051 (5)0.42653 (6)0.02982 (18)
Se40.63098 (6)0.60738 (6)0.70713 (5)0.0323 (2)
Se50.72097 (5)0.69372 (5)0.05091 (6)0.02999 (18)
Se60.63358 (5)0.70197 (6)0.38306 (5)0.03010 (18)
Se70.72844 (6)0.37656 (7)0.47447 (7)0.0407 (2)
Se80.29825 (6)0.70002 (5)0.66411 (7)0.0346 (2)
Se91.06983 (6)1.02797 (7)0.45938 (8)0.0415 (2)
C60.7490 (5)0.6889 (5)0.3919 (6)0.0325 (13)
C20.2570 (5)0.3180 (6)0.7562 (6)0.0370 (16)
C90.9343 (6)0.9964 (6)0.4541 (6)0.0381 (16)
C30.4141 (6)0.4037 (5)0.4176 (6)0.0379 (16)
C10.3858 (6)0.2897 (6)0.0944 (5)0.0336 (15)
N160.8041 (5)0.7002 (5)0.3094 (5)0.0443 (15)
H16A0.8567600.6934890.3138850.053*
H16B0.7873190.7141420.2510580.053*
N210.2099 (5)0.3164 (6)0.8408 (5)0.0490 (17)
H21A0.1469910.2995540.8387740.059*
H21B0.2418190.3322640.8984850.059*
N190.8901 (5)1.0070 (6)0.5355 (5)0.0495 (17)
H19A0.8280930.9931630.5322210.059*
H19B0.9230211.0278740.5923820.059*
N290.8826 (6)0.9647 (7)0.3693 (6)0.061 (2)
H29A0.8207090.9512770.3675880.073*
H29B0.9103750.9572520.3149690.073*
N220.2081 (6)0.2940 (9)0.6699 (6)0.082 (3)
H22A0.1451960.2772040.6685380.099*
H22B0.2385200.2948120.6138210.099*
N260.7764 (6)0.6675 (7)0.4802 (6)0.058 (2)
H26A0.8292900.6611350.4833740.069*
H26B0.7413630.6599740.5347990.069*
N110.4358 (5)0.2920 (5)0.0112 (5)0.0407 (14)
H11A0.4719980.2632640.0109480.049*
H11B0.4322290.3223620.0431600.049*
N120.3931 (6)0.2422 (6)0.1766 (5)0.0538 (19)
H12A0.4298480.2140100.1744350.065*
H12B0.3610940.2396190.2319980.065*
N280.3865 (7)0.5964 (7)0.7512 (6)0.065 (2)
H28A0.4220070.5667800.7505490.078*
H28B0.3570140.5981130.8069210.078*
N250.5264 (5)0.6265 (6)0.1267 (6)0.0491 (17)
H25A0.4612830.5939130.1238140.059*
H25B0.5566470.6596070.1813590.059*
N170.5412 (5)0.2423 (6)0.3865 (6)0.0548 (19)
H17A0.4769570.2005580.3868090.066*
H17B0.5744240.2568100.3296970.066*
N180.4244 (7)0.6343 (8)0.5834 (6)0.074 (3)
H18A0.4592480.6040740.5853890.089*
H18B0.4200420.6614060.5269730.089*
N230.4738 (5)0.4463 (5)0.4966 (6)0.0526 (17)
H23A0.5251480.5063700.4911470.063*
H23B0.4615810.4142100.5540470.063*
N140.6773 (7)0.7997 (5)0.6448 (6)0.064 (2)
H14A0.7036600.8642230.6504960.077*
H14B0.6425300.7689880.5910660.077*
N240.7431 (6)0.7956 (5)0.7990 (6)0.056 (2)
H24A0.7690890.8601460.8039280.067*
H24B0.7520040.7624370.8475560.067*
N270.5351 (5)0.2599 (6)0.5588 (6)0.061 (2)
H27A0.4710360.2178790.5563380.073*
H27B0.5637230.2856930.6166930.073*
N130.4335 (7)0.4534 (6)0.3309 (6)0.072 (3)
H13A0.4851270.5134180.3262440.086*
H13B0.3947860.4260510.2785810.086*
C70.5892 (6)0.2845 (6)0.4744 (6)0.0403 (16)
C50.5800 (5)0.6259 (5)0.0469 (5)0.0313 (14)
C80.3775 (6)0.6391 (6)0.6669 (6)0.0423 (17)
C40.6902 (6)0.7479 (6)0.7182 (6)0.0389 (16)
N150.5312 (5)0.5742 (6)0.0364 (5)0.0524 (19)
H15A0.4660810.5420160.0378190.063*
H15B0.5647810.5728560.0889950.063*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0309 (4)0.0312 (4)0.0320 (4)0.0179 (3)0.0009 (3)0.0001 (3)
Se20.0251 (3)0.0351 (4)0.0337 (4)0.0143 (3)0.0003 (3)0.0033 (3)
Se30.0302 (4)0.0244 (3)0.0327 (4)0.0120 (3)0.0010 (3)0.0008 (3)
Se40.0327 (4)0.0258 (3)0.0354 (5)0.0123 (3)0.0001 (3)0.0001 (3)
Se50.0255 (3)0.0291 (3)0.0346 (4)0.0131 (3)0.0015 (3)0.0004 (3)
Se60.0285 (3)0.0308 (3)0.0340 (4)0.0170 (3)0.0007 (3)0.0001 (3)
Se70.0284 (4)0.0371 (4)0.0410 (5)0.0047 (3)0.0022 (3)0.0006 (3)
Se80.0417 (4)0.0338 (4)0.0352 (5)0.0241 (3)0.0025 (3)0.0013 (3)
Se90.0286 (4)0.0493 (5)0.0477 (5)0.0203 (4)0.0049 (3)0.0110 (4)
C60.032 (3)0.032 (3)0.038 (4)0.020 (3)0.006 (3)0.003 (3)
C20.034 (4)0.048 (4)0.033 (4)0.023 (3)0.001 (3)0.002 (3)
C90.036 (3)0.037 (4)0.042 (5)0.018 (3)0.003 (3)0.005 (3)
C30.041 (4)0.032 (3)0.034 (4)0.013 (3)0.003 (3)0.003 (3)
C10.036 (4)0.036 (4)0.027 (4)0.017 (3)0.000 (3)0.002 (3)
N160.042 (3)0.060 (4)0.038 (4)0.031 (3)0.005 (3)0.005 (3)
N210.038 (3)0.073 (5)0.041 (4)0.032 (3)0.003 (3)0.002 (3)
N190.040 (3)0.082 (5)0.038 (4)0.039 (4)0.005 (3)0.003 (3)
N290.040 (4)0.098 (6)0.038 (4)0.030 (4)0.004 (3)0.019 (4)
N220.047 (4)0.177 (11)0.037 (4)0.066 (6)0.013 (3)0.024 (5)
N260.053 (4)0.099 (6)0.045 (4)0.056 (4)0.001 (3)0.006 (4)
N110.045 (3)0.058 (4)0.033 (3)0.036 (3)0.007 (3)0.007 (3)
N120.078 (5)0.082 (5)0.036 (4)0.066 (5)0.007 (3)0.012 (3)
N280.089 (6)0.097 (6)0.049 (5)0.077 (6)0.023 (4)0.031 (4)
N250.034 (3)0.061 (4)0.044 (4)0.019 (3)0.007 (3)0.009 (3)
N170.035 (3)0.060 (4)0.046 (4)0.006 (3)0.005 (3)0.009 (3)
N180.091 (6)0.146 (9)0.038 (4)0.100 (7)0.024 (4)0.032 (5)
N230.052 (4)0.036 (3)0.045 (4)0.004 (3)0.003 (3)0.002 (3)
N140.107 (7)0.036 (3)0.046 (4)0.034 (4)0.016 (4)0.003 (3)
N240.077 (5)0.029 (3)0.049 (4)0.017 (3)0.012 (4)0.001 (3)
N270.032 (3)0.082 (5)0.048 (4)0.013 (4)0.000 (3)0.006 (4)
N130.093 (6)0.036 (4)0.041 (4)0.002 (4)0.012 (4)0.002 (3)
C70.034 (4)0.040 (4)0.044 (4)0.016 (3)0.004 (3)0.008 (3)
C50.032 (3)0.031 (3)0.028 (3)0.014 (3)0.000 (3)0.002 (3)
C80.046 (4)0.060 (5)0.037 (4)0.038 (4)0.006 (3)0.005 (3)
C40.048 (4)0.034 (4)0.032 (4)0.018 (3)0.007 (3)0.001 (3)
N150.030 (3)0.074 (5)0.033 (4)0.012 (3)0.002 (3)0.013 (3)
Geometric parameters (Å, º) top
Se1—C11.867 (7)N11—H11B0.8600
Se2—C21.870 (7)N12—H12A0.8600
Se3—C31.877 (7)N12—H12B0.8600
Se4—C41.868 (7)N28—H28A0.8600
Se5—C51.862 (7)N28—H28B0.8600
Se6—C61.870 (6)N28—C81.316 (11)
Se7—C71.869 (7)N25—H25A0.8600
Se8—C81.856 (7)N25—H25B0.8600
Se9—C91.873 (7)N25—C51.323 (9)
C6—N161.319 (10)N17—H17A0.8600
C6—N261.318 (10)N17—H17B0.8600
C2—N211.307 (10)N17—C71.335 (11)
C2—N221.295 (11)N18—H18A0.8600
C9—N191.307 (10)N18—H18B0.8600
C9—N291.299 (11)N18—C81.322 (10)
C3—N231.309 (10)N23—H23A0.8600
C3—N131.306 (11)N23—H23B0.8600
C1—N111.313 (9)N14—H14A0.8600
C1—N121.326 (9)N14—H14B0.8600
N16—H16A0.8600N14—C41.313 (11)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.303 (11)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.310 (11)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.327 (10)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.5 (5)C8—N28—H28B120.0
N26—C6—Se6120.7 (5)H25A—N25—H25B120.0
N26—C6—N16118.8 (6)C5—N25—H25A120.0
N21—C2—Se2120.6 (6)C5—N25—H25B120.0
N22—C2—Se2119.9 (6)H17A—N17—H17B120.0
N22—C2—N21119.4 (7)C7—N17—H17A120.0
N19—C9—Se9120.6 (6)C7—N17—H17B120.0
N29—C9—Se9120.8 (6)H18A—N18—H18B120.0
N29—C9—N19118.6 (7)C8—N18—H18A120.0
N23—C3—Se3120.5 (6)C8—N18—H18B120.0
N13—C3—Se3120.1 (6)C3—N23—H23A120.0
N13—C3—N23119.3 (7)C3—N23—H23B120.0
N11—C1—Se1121.0 (5)H23A—N23—H23B120.0
N11—C1—N12118.3 (7)H14A—N14—H14B120.0
N12—C1—Se1120.7 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.4 (6)
H29A—N29—H29B120.0N27—C7—Se7122.0 (6)
C2—N22—H22A120.0N27—C7—N17117.6 (7)
C2—N22—H22B120.0N25—C5—Se5121.3 (5)
H22A—N22—H22B120.0N25—C5—N15118.7 (7)
C6—N26—H26A120.0N15—C5—Se5120.0 (5)
C6—N26—H26B120.0N28—C8—Se8121.3 (6)
H26A—N26—H26B120.0N28—C8—N18117.6 (7)
C1—N11—H11A120.0N18—C8—Se8121.1 (6)
C1—N11—H11B120.0N14—C4—Se4120.1 (6)
H11A—N11—H11B120.0N24—C4—Se4120.7 (6)
C1—N12—H12A120.0N24—C4—N14119.2 (7)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_270K) top
Crystal data top
CH4N2SeDx = 2.104 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 6632 reflections
a = 15.2541 (1) Åθ = 3.3–72.2°
c = 13.0096 (2) ŵ = 11.27 mm1
V = 2621.61 (5) Å3T = 270 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
4032 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source4001 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.036
Detector resolution: 10.5384 pixels mm-1θmax = 72.3°, θmin = 3.4°
ω scansh = 1818
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1816
Tmin = 0.395, Tmax = 1.000l = 1413
6907 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0626P)2 + 0.4992P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.033(Δ/σ)max = 0.001
wR(F2) = 0.090Δρmax = 0.58 e Å3
S = 1.04Δρmin = 0.46 e Å3
4032 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00074 (6)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30619 (5)0.35124 (6)0.09711 (5)0.03351 (18)
Se20.39488 (5)0.36016 (6)0.75804 (5)0.03475 (19)
Se30.30496 (5)0.27067 (5)0.42659 (6)0.03289 (17)
Se40.63092 (6)0.60740 (6)0.70710 (5)0.0356 (2)
Se50.72101 (5)0.69354 (5)0.05079 (5)0.03321 (18)
Se60.63372 (5)0.70194 (6)0.38297 (5)0.03327 (18)
Se70.72868 (6)0.37640 (6)0.47389 (7)0.0448 (2)
Se80.29817 (6)0.70010 (5)0.66440 (7)0.0382 (2)
Se91.06991 (6)1.02849 (7)0.46008 (8)0.0452 (2)
C60.7488 (5)0.6885 (5)0.3914 (6)0.0365 (14)
C20.2571 (5)0.3173 (6)0.7564 (6)0.0415 (16)
C90.9342 (5)0.9962 (6)0.4545 (6)0.0412 (16)
C30.4131 (6)0.4038 (5)0.4178 (5)0.0422 (16)
C10.3860 (5)0.2904 (5)0.0949 (5)0.0369 (15)
N160.8035 (5)0.6997 (5)0.3095 (5)0.0488 (15)
H16A0.8559170.6926780.3139240.059*
H16B0.7869540.7140140.2512960.059*
N210.2095 (5)0.3156 (6)0.8412 (5)0.0544 (17)
H21A0.1465220.2982390.8390220.065*
H21B0.2413720.3319270.8988030.065*
N190.8899 (5)1.0071 (6)0.5362 (5)0.0554 (18)
H19A0.8280750.9935580.5328200.066*
H19B0.9227601.0277990.5930650.066*
N290.8828 (5)0.9649 (7)0.3700 (6)0.067 (2)
H29A0.8210030.9517900.3682130.081*
H29B0.9103990.9573210.3156730.081*
N220.2076 (6)0.2924 (9)0.6700 (6)0.091 (4)
H22A0.1446660.2751360.6688260.109*
H22B0.2379410.2931680.6139270.109*
N260.7758 (6)0.6665 (7)0.4796 (5)0.064 (2)
H26A0.8285050.6597900.4825590.077*
H26B0.7408530.6588760.5340950.077*
N110.4359 (5)0.2926 (5)0.0112 (5)0.0458 (15)
H11A0.4716390.2633290.0106800.055*
H11B0.4327900.3233770.0428940.055*
N120.3929 (6)0.2421 (6)0.1766 (5)0.059 (2)
H12A0.4291740.2134600.1739100.071*
H12B0.3611440.2394280.2321430.071*
N280.3860 (7)0.5964 (7)0.7509 (6)0.072 (3)
H28A0.4214950.5668150.7503600.086*
H28B0.3562750.5978650.8065020.086*
N250.5268 (5)0.6267 (6)0.1267 (6)0.0534 (17)
H25A0.4617280.5945300.1239440.064*
H25B0.5572460.6597400.1812450.064*
N170.5417 (5)0.2431 (6)0.3861 (6)0.059 (2)
H17A0.4775210.2013910.3862250.071*
H17B0.5750120.2576370.3293730.071*
N180.4242 (7)0.6350 (8)0.5839 (6)0.082 (3)
H18A0.4591040.6048770.5857260.098*
H18B0.4198970.6623450.5277750.098*
N230.4729 (5)0.4467 (5)0.4967 (6)0.0576 (18)
H23A0.5241410.5066890.4910630.069*
H23B0.4607920.4147420.5541280.069*
N140.6778 (7)0.7997 (5)0.6447 (6)0.071 (2)
H14A0.7032980.8640690.6509030.085*
H14B0.6439570.7693060.5904580.085*
N240.7419 (6)0.7952 (5)0.7994 (6)0.062 (2)
H24A0.7669500.8596150.8045440.074*
H24B0.7508320.7623070.8480280.074*
N270.5356 (5)0.2608 (6)0.5583 (6)0.066 (2)
H27A0.4716010.2188330.5557300.080*
H27B0.5641150.2865730.6161450.080*
N130.4326 (7)0.4534 (6)0.3312 (6)0.078 (3)
H13A0.4840910.5133870.3264480.094*
H13B0.3939010.4260470.2788160.094*
C70.5896 (6)0.2853 (6)0.4742 (6)0.0442 (17)
C50.5799 (5)0.6255 (5)0.0470 (5)0.0350 (14)
C80.3774 (6)0.6392 (7)0.6671 (6)0.0465 (18)
C40.6905 (6)0.7477 (5)0.7182 (6)0.0420 (16)
N150.5311 (5)0.5739 (6)0.0364 (5)0.0575 (19)
H15A0.4659780.5421120.0378970.069*
H15B0.5645180.5723380.0888750.069*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0340 (4)0.0341 (4)0.0356 (4)0.0195 (3)0.0009 (3)0.0000 (3)
Se20.0279 (3)0.0381 (4)0.0372 (4)0.0157 (3)0.0005 (3)0.0037 (3)
Se30.0331 (4)0.0270 (3)0.0363 (4)0.0133 (3)0.0010 (3)0.0009 (3)
Se40.0358 (4)0.0282 (3)0.0391 (5)0.0133 (3)0.0000 (3)0.0002 (3)
Se50.0284 (3)0.0322 (3)0.0385 (4)0.0147 (3)0.0017 (3)0.0005 (3)
Se60.0314 (3)0.0339 (3)0.0378 (4)0.0188 (3)0.0006 (3)0.0003 (3)
Se70.0313 (4)0.0403 (4)0.0456 (5)0.0051 (3)0.0026 (3)0.0006 (3)
Se80.0457 (4)0.0372 (4)0.0395 (5)0.0266 (3)0.0027 (3)0.0015 (3)
Se90.0313 (4)0.0531 (5)0.0522 (5)0.0218 (4)0.0050 (3)0.0116 (4)
C60.036 (3)0.037 (3)0.042 (4)0.021 (3)0.008 (3)0.004 (3)
C20.039 (4)0.055 (4)0.035 (4)0.028 (3)0.000 (3)0.004 (3)
C90.035 (3)0.042 (4)0.045 (4)0.019 (3)0.003 (3)0.002 (3)
C30.048 (4)0.034 (3)0.035 (4)0.014 (3)0.004 (3)0.003 (3)
C10.036 (4)0.039 (4)0.034 (4)0.017 (3)0.001 (3)0.001 (3)
N160.044 (3)0.066 (4)0.045 (4)0.035 (3)0.005 (3)0.005 (3)
N210.043 (3)0.081 (5)0.044 (4)0.035 (4)0.005 (3)0.002 (3)
N190.045 (3)0.089 (5)0.044 (4)0.043 (4)0.006 (3)0.004 (3)
N290.041 (4)0.109 (6)0.043 (4)0.032 (4)0.006 (3)0.024 (4)
N220.054 (4)0.196 (12)0.040 (4)0.076 (6)0.012 (4)0.019 (6)
N260.065 (5)0.111 (7)0.045 (4)0.066 (5)0.002 (3)0.010 (4)
N110.051 (4)0.065 (4)0.039 (3)0.043 (3)0.009 (3)0.010 (3)
N120.087 (5)0.089 (5)0.039 (4)0.073 (5)0.008 (3)0.013 (3)
N280.101 (6)0.107 (7)0.052 (5)0.086 (6)0.022 (4)0.032 (5)
N250.037 (3)0.067 (4)0.048 (4)0.020 (3)0.006 (3)0.009 (3)
N170.038 (3)0.064 (4)0.051 (4)0.008 (3)0.003 (3)0.011 (3)
N180.099 (6)0.160 (9)0.044 (4)0.108 (7)0.028 (4)0.035 (5)
N230.056 (4)0.041 (3)0.051 (4)0.005 (3)0.005 (3)0.003 (3)
N140.118 (7)0.040 (3)0.051 (4)0.036 (4)0.020 (4)0.004 (3)
N240.086 (5)0.032 (3)0.055 (5)0.019 (3)0.013 (4)0.003 (3)
N270.035 (3)0.087 (6)0.052 (4)0.012 (3)0.002 (3)0.006 (4)
N130.096 (6)0.040 (4)0.047 (4)0.005 (4)0.012 (4)0.004 (3)
C70.036 (3)0.044 (4)0.049 (4)0.017 (3)0.005 (3)0.007 (3)
C50.033 (3)0.035 (3)0.033 (3)0.015 (3)0.002 (3)0.001 (3)
C80.048 (4)0.067 (5)0.039 (4)0.040 (4)0.007 (3)0.005 (3)
C40.054 (4)0.037 (3)0.032 (4)0.021 (3)0.006 (3)0.000 (3)
N150.035 (3)0.080 (5)0.039 (4)0.015 (3)0.002 (3)0.015 (3)
Geometric parameters (Å, º) top
Se1—C11.864 (7)N11—H11B0.8600
Se2—C21.864 (7)N12—H12A0.8600
Se3—C31.873 (7)N12—H12B0.8600
Se4—C41.866 (7)N28—H28A0.8600
Se5—C51.865 (7)N28—H28B0.8600
Se6—C61.869 (6)N28—C81.312 (11)
Se7—C71.866 (7)N25—H25A0.8600
Se8—C81.857 (7)N25—H25B0.8600
Se9—C91.874 (7)N25—C51.322 (9)
C6—N161.312 (10)N17—H17A0.8600
C6—N261.318 (9)N17—H17B0.8600
C2—N211.313 (10)N17—C71.339 (11)
C2—N221.300 (11)N18—H18A0.8600
C9—N191.313 (10)N18—H18B0.8600
C9—N291.296 (10)N18—C81.315 (10)
C3—N231.310 (10)N23—H23A0.8600
C3—N131.306 (11)N23—H23B0.8600
C1—N111.320 (9)N14—H14A0.8600
C1—N121.327 (9)N14—H14B0.8600
N16—H16A0.8600N14—C41.317 (11)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.299 (10)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.306 (11)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.329 (10)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.6 (5)C8—N28—H28B120.0
N16—C6—N26118.7 (6)H25A—N25—H25B120.0
N26—C6—Se6120.7 (5)C5—N25—H25A120.0
N21—C2—Se2120.8 (6)C5—N25—H25B120.0
N22—C2—Se2120.0 (6)H17A—N17—H17B120.0
N22—C2—N21119.1 (7)C7—N17—H17A120.0
N19—C9—Se9120.4 (6)C7—N17—H17B120.0
N29—C9—Se9121.0 (6)H18A—N18—H18B120.0
N29—C9—N19118.6 (7)C8—N18—H18A120.0
N23—C3—Se3120.6 (6)C8—N18—H18B120.0
N13—C3—Se3120.2 (6)C3—N23—H23A120.0
N13—C3—N23119.2 (7)C3—N23—H23B120.0
N11—C1—Se1120.8 (5)H23A—N23—H23B120.0
N11—C1—N12118.0 (6)H14A—N14—H14B120.0
N12—C1—Se1121.2 (5)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.0 (6)
H29A—N29—H29B120.0N27—C7—Se7122.3 (6)
C2—N22—H22A120.0N27—C7—N17117.7 (7)
C2—N22—H22B120.0N25—C5—Se5121.1 (5)
H22A—N22—H22B120.0N25—C5—N15118.9 (6)
C6—N26—H26A120.0N15—C5—Se5120.0 (5)
C6—N26—H26B120.0N28—C8—Se8121.2 (6)
H26A—N26—H26B120.0N28—C8—N18117.9 (7)
C1—N11—H11A120.0N18—C8—Se8120.9 (6)
C1—N11—H11B120.0N14—C4—Se4120.0 (6)
H11A—N11—H11B120.0N24—C4—Se4121.0 (6)
C1—N12—H12A120.0N24—C4—N14118.9 (7)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_290K) top
Crystal data top
CH4N2SeDx = 2.097 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 3720 reflections
a = 15.2714 (1) Åθ = 3.3–72.3°
c = 13.0219 (2) ŵ = 11.23 mm1
V = 2630.04 (5) Å3T = 290 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
2709 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source2649 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.030
Detector resolution: 10.5384 pixels mm-1θmax = 72.5°, θmin = 3.3°
ω scansh = 1215
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1811
Tmin = 0.279, Tmax = 1.000l = 1311
3810 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0775P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.035(Δ/σ)max < 0.001
wR(F2) = 0.102Δρmax = 0.46 e Å3
S = 1.06Δρmin = 0.45 e Å3
2709 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00075 (8)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30605 (7)0.35124 (8)0.09725 (8)0.0377 (3)
Se20.39435 (8)0.36028 (8)0.75790 (8)0.0392 (3)
Se30.30499 (8)0.27089 (7)0.42680 (8)0.0374 (3)
Se40.63085 (8)0.60744 (8)0.70707 (8)0.0403 (3)
Se50.72109 (7)0.69330 (7)0.05065 (8)0.0375 (3)
Se60.63390 (8)0.70196 (8)0.38297 (7)0.0376 (3)
Se70.72901 (8)0.37619 (9)0.47311 (10)0.0502 (3)
Se80.29809 (8)0.70028 (8)0.66470 (10)0.0435 (3)
Se91.07005 (8)1.02909 (9)0.46070 (11)0.0504 (3)
C60.7477 (7)0.6871 (7)0.3908 (8)0.041 (2)
C20.2565 (8)0.3166 (8)0.7571 (8)0.047 (3)
C90.9342 (7)0.9967 (8)0.4554 (9)0.047 (2)
C30.4136 (8)0.4044 (7)0.4174 (9)0.050 (3)
C10.3857 (7)0.2909 (7)0.0947 (8)0.043 (2)
N160.8034 (7)0.6989 (7)0.3088 (7)0.056 (2)
H16A0.8554720.6914940.3135050.067*
H16B0.7875200.7139380.2507040.067*
N210.2090 (7)0.3148 (8)0.8412 (7)0.058 (2)
H21A0.1456380.2957190.8391380.070*
H21B0.2410420.3327020.8986190.070*
N190.8895 (7)1.0064 (8)0.5363 (7)0.063 (3)
H19A0.8270860.9906180.5330800.076*
H19B0.9224901.0285940.5927970.076*
N290.8831 (7)0.9631 (10)0.3712 (8)0.077 (3)
H29A0.8206690.9476510.3692910.092*
H29B0.9114820.9562440.3171910.092*
N220.2071 (8)0.2894 (12)0.6712 (9)0.105 (5)
H22A0.1437540.2704120.6700680.126*
H22B0.2376160.2902330.6154220.126*
N260.7740 (8)0.6638 (9)0.4796 (8)0.076 (3)
H26A0.8263420.6566940.4828050.092*
H26B0.7385830.6557700.5338240.092*
N110.4346 (6)0.2919 (7)0.0104 (7)0.052 (2)
H11A0.4687670.2611230.0093930.062*
H11B0.4322540.3234730.0432730.062*
N120.3912 (9)0.2408 (8)0.1770 (7)0.067 (3)
H12A0.4258510.2105650.1740060.081*
H12B0.3600260.2389840.2326770.081*
N280.3853 (9)0.5961 (9)0.7511 (9)0.079 (4)
H28A0.4201350.5660210.7505120.095*
H28B0.3552750.5974940.8064510.095*
N250.5275 (7)0.6272 (8)0.1268 (8)0.060 (3)
H25A0.4625890.5955640.1239850.072*
H25B0.5580490.6598360.1815080.072*
N170.5419 (7)0.2429 (8)0.3856 (7)0.062 (3)
H17A0.4776690.2019680.3861890.074*
H17B0.5748980.2561740.3288260.074*
N180.4253 (9)0.6355 (11)0.5848 (8)0.092 (4)
H18A0.4594130.6046940.5872000.111*
H18B0.4221110.6633040.5285500.111*
N230.4721 (7)0.4479 (7)0.4957 (7)0.063 (3)
H23A0.5211090.5091310.4908090.076*
H23B0.4618140.4153630.5524820.076*
N140.6786 (9)0.7994 (7)0.6443 (8)0.080 (4)
H14A0.7047200.8637900.6500550.096*
H14B0.6447260.7689020.5902150.096*
N240.7411 (9)0.7942 (7)0.7989 (8)0.074 (3)
H24A0.7668450.8586390.8035020.089*
H24B0.7494210.7612940.8478570.089*
N270.5365 (7)0.2629 (8)0.5572 (8)0.078 (3)
H27A0.4723580.2217710.5556360.093*
H27B0.5658380.2894920.6145060.093*
N130.4304 (9)0.4550 (7)0.3317 (8)0.092 (5)
H13A0.4797050.5162400.3278210.110*
H13B0.3922380.4270520.2793250.110*
C70.5899 (8)0.2853 (8)0.4720 (9)0.051 (3)
C50.5810 (7)0.6258 (7)0.0465 (8)0.040 (2)
C80.3778 (8)0.6400 (9)0.6672 (10)0.056 (3)
C40.6904 (9)0.7472 (8)0.7188 (9)0.053 (3)
N150.5309 (6)0.5745 (8)0.0369 (7)0.068 (3)
H15A0.4659220.5433920.0378100.081*
H15B0.5636460.5723920.0896890.081*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0370 (5)0.0381 (5)0.0418 (6)0.0216 (5)0.0012 (4)0.0002 (4)
Se20.0300 (5)0.0413 (6)0.0448 (7)0.0167 (4)0.0000 (4)0.0038 (4)
Se30.0367 (5)0.0300 (5)0.0429 (6)0.0148 (4)0.0014 (4)0.0013 (4)
Se40.0396 (5)0.0315 (5)0.0460 (7)0.0148 (4)0.0001 (5)0.0004 (4)
Se50.0312 (5)0.0356 (5)0.0452 (6)0.0162 (4)0.0018 (4)0.0005 (4)
Se60.0352 (5)0.0373 (5)0.0442 (6)0.0210 (4)0.0006 (4)0.0001 (4)
Se70.0347 (6)0.0443 (6)0.0528 (8)0.0058 (4)0.0027 (5)0.0010 (5)
Se80.0509 (6)0.0412 (6)0.0467 (7)0.0293 (5)0.0035 (5)0.0020 (4)
Se90.0346 (5)0.0575 (7)0.0600 (8)0.0237 (5)0.0043 (5)0.0113 (6)
C60.042 (5)0.040 (5)0.048 (6)0.024 (4)0.005 (4)0.005 (4)
C20.041 (5)0.060 (6)0.045 (7)0.028 (5)0.005 (5)0.007 (5)
C90.035 (5)0.050 (6)0.057 (8)0.023 (4)0.001 (5)0.004 (5)
C30.053 (6)0.034 (5)0.052 (7)0.014 (5)0.001 (5)0.012 (5)
C10.038 (5)0.037 (5)0.051 (7)0.018 (4)0.001 (4)0.002 (4)
N160.051 (5)0.079 (6)0.049 (6)0.042 (5)0.005 (4)0.003 (4)
N210.046 (5)0.092 (7)0.045 (6)0.040 (5)0.004 (4)0.003 (5)
N190.050 (5)0.106 (8)0.051 (6)0.053 (5)0.008 (4)0.001 (5)
N290.048 (5)0.127 (10)0.053 (8)0.042 (6)0.006 (5)0.028 (6)
N220.058 (6)0.231 (17)0.044 (7)0.086 (9)0.011 (6)0.016 (9)
N260.074 (7)0.138 (10)0.055 (7)0.081 (7)0.009 (5)0.023 (6)
N110.056 (5)0.073 (6)0.047 (6)0.048 (5)0.006 (4)0.005 (4)
N120.094 (8)0.100 (8)0.048 (6)0.079 (7)0.009 (5)0.015 (5)
N280.111 (9)0.125 (10)0.059 (7)0.101 (8)0.027 (6)0.029 (7)
N250.039 (4)0.081 (7)0.048 (6)0.021 (5)0.004 (4)0.013 (5)
N170.041 (5)0.079 (7)0.037 (6)0.009 (5)0.004 (4)0.008 (5)
N180.098 (9)0.184 (14)0.056 (7)0.116 (10)0.021 (6)0.027 (8)
N230.061 (5)0.045 (5)0.053 (6)0.003 (4)0.013 (5)0.007 (4)
N140.138 (11)0.040 (5)0.058 (6)0.042 (6)0.027 (7)0.005 (4)
N240.106 (9)0.034 (4)0.065 (8)0.023 (5)0.027 (7)0.004 (4)
N270.040 (5)0.104 (9)0.053 (7)0.010 (5)0.004 (4)0.005 (6)
N130.127 (11)0.038 (5)0.043 (7)0.009 (6)0.013 (6)0.004 (4)
C70.037 (5)0.046 (6)0.061 (8)0.013 (4)0.001 (5)0.001 (5)
C50.031 (4)0.034 (4)0.051 (7)0.015 (4)0.003 (4)0.002 (4)
C80.047 (6)0.077 (8)0.060 (8)0.044 (6)0.006 (5)0.007 (6)
C40.054 (6)0.043 (6)0.061 (8)0.024 (5)0.002 (5)0.004 (5)
N150.033 (4)0.092 (7)0.052 (7)0.011 (5)0.005 (4)0.016 (5)
Geometric parameters (Å, º) top
Se1—C11.857 (10)N11—H11B0.8600
Se2—C21.863 (10)N12—H12A0.8600
Se3—C31.882 (10)N12—H12B0.8600
Se4—C41.861 (11)N28—H28A0.8600
Se5—C51.854 (9)N28—H28B0.8600
Se6—C61.865 (9)N28—C81.316 (15)
Se7—C71.869 (10)N25—H25A0.8600
Se8—C81.857 (10)N25—H25B0.8600
Se9—C91.878 (9)N25—C51.333 (13)
C6—N161.319 (13)N17—H17A0.8600
C6—N261.330 (12)N17—H17B0.8600
C2—N211.307 (13)N17—C71.321 (14)
C2—N221.296 (15)N18—H18A0.8600
C9—N191.303 (13)N18—H18B0.8600
C9—N291.294 (14)N18—C81.316 (15)
C3—N231.298 (13)N23—H23A0.8600
C3—N131.307 (14)N23—H23B0.8600
C1—N111.323 (13)N14—H14A0.8600
C1—N121.344 (13)N14—H14B0.8600
N16—H16A0.8600N14—C41.324 (15)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.283 (15)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.317 (15)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.334 (13)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6121.0 (7)C8—N28—H28B120.0
N16—C6—N26118.7 (8)H25A—N25—H25B120.0
N26—C6—Se6120.3 (7)C5—N25—H25A120.0
N21—C2—Se2121.3 (8)C5—N25—H25B120.0
N22—C2—Se2119.5 (8)H17A—N17—H17B120.0
N22—C2—N21119.2 (10)C7—N17—H17A120.0
N19—C9—Se9120.9 (8)C7—N17—H17B120.0
N29—C9—Se9120.3 (8)H18A—N18—H18B120.0
N29—C9—N19118.9 (9)C8—N18—H18A120.0
N23—C3—Se3120.7 (8)C8—N18—H18B120.0
N23—C3—N13119.1 (9)C3—N23—H23A120.0
N13—C3—Se3120.1 (8)C3—N23—H23B120.0
N11—C1—Se1121.0 (8)H23A—N23—H23B120.0
N11—C1—N12118.2 (9)H14A—N14—H14B120.0
N12—C1—Se1120.7 (8)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7121.1 (8)
H29A—N29—H29B120.0N27—C7—Se7120.8 (8)
C2—N22—H22A120.0N27—C7—N17118.1 (9)
C2—N22—H22B120.0N25—C5—Se5120.9 (7)
H22A—N22—H22B120.0N15—C5—Se5120.9 (7)
C6—N26—H26A120.0N15—C5—N25118.2 (8)
C6—N26—H26B120.0N28—C8—Se8120.8 (8)
H26A—N26—H26B120.0N28—C8—N18117.3 (9)
C1—N11—H11A120.0N18—C8—Se8121.8 (9)
C1—N11—H11B120.0N14—C4—Se4119.7 (9)
H11A—N11—H11B120.0N24—C4—Se4121.4 (9)
C1—N12—H12A120.0N24—C4—N14119.0 (10)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_293K) top
Crystal data top
CH4N2SeDx = 2.113 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3420 reflections
a = 15.2757 (6) Åθ = 3.4–28.8°
c = 13.0230 (5) ŵ = 9.48 mm1
V = 2631.7 (2) Å3T = 293 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
7257 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5372 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
Detector resolution: 16.1544 pixels mm-1θmax = 29.1°, θmin = 3.1°
ω scansh = 1820
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.550, Tmax = 1.000l = 1716
18848 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + 51.6018P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.081(Δ/σ)max < 0.001
wR(F2) = 0.143Δρmax = 1.74 e Å3
S = 1.09Δρmin = 2.14 e Å3
7257 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00068 (4)
1 restraintAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30586 (19)0.35118 (18)0.09687 (17)0.0324 (5)
Se20.39446 (19)0.3609 (2)0.75598 (17)0.0349 (6)
Se30.30425 (19)0.27047 (18)0.42822 (19)0.0330 (5)
Se40.6316 (2)0.6083 (2)0.70798 (17)0.0413 (7)
Se50.72099 (19)0.6936 (2)0.05018 (19)0.0358 (6)
Se60.63414 (18)0.7016 (2)0.38280 (17)0.0319 (5)
Se70.7307 (2)0.3744 (2)0.47012 (19)0.0502 (3)
Se80.29956 (19)0.70090 (19)0.6651 (2)0.0389 (6)
Se91.0696 (2)1.0306 (2)0.4653 (2)0.0504 (3)
C60.7471 (17)0.6824 (17)0.3878 (16)0.033 (5)
C20.257 (3)0.321 (3)0.762 (2)0.076 (11)
C90.923 (3)0.985 (2)0.461 (2)0.047 (2)
C30.413 (2)0.4015 (17)0.4161 (16)0.042 (6)
C10.3823 (19)0.287 (2)0.0930 (16)0.069 (7)
N160.8026 (14)0.6950 (16)0.3098 (15)0.049 (5)
H16A0.8533670.6855070.3150470.058*
H16B0.7892580.7129140.2519840.058*
N210.2095 (18)0.315 (3)0.8419 (16)0.058 (2)
H21A0.1454770.2927440.8390900.070*
H21B0.2406850.3339440.8996900.070*
N190.889 (2)0.998 (2)0.537 (2)0.063 (3)
H19A0.8329660.9980360.5347090.076*
H19B0.9207011.0077520.5941640.076*
N290.8880 (16)0.970 (2)0.3758 (18)0.077 (3)
H29A0.8316570.9690090.3656860.092*
H29B0.9189230.9615680.3252490.092*
N220.205 (3)0.290 (4)0.670 (2)0.069 (7)
H22A0.1406410.2677320.6694810.083*
H22B0.2357840.2929620.6142100.083*
N260.7657 (18)0.655 (2)0.4783 (15)0.065 (7)
H26A0.8160760.6448330.4851050.078*
H26B0.7272620.6466030.5299300.078*
N110.4329 (14)0.2940 (15)0.0085 (13)0.041 (5)
H11A0.4714620.2679630.0062280.049*
H11B0.4274150.3246110.0444180.049*
N120.3902 (18)0.241 (2)0.1738 (14)0.067 (3)
H12A0.4286470.2143680.1720020.081*
H12B0.3570210.2362060.2287100.081*
N280.393 (2)0.6031 (19)0.7539 (15)0.079 (4)
H28A0.4317400.5773780.7498180.095*
H28B0.3660260.6035370.8117420.095*
N250.5269 (14)0.6214 (16)0.1298 (14)0.069 (7)
H25A0.4622460.5942410.1262880.083*
H25B0.5578820.6485910.1861700.083*
N170.5407 (15)0.2465 (18)0.391 (2)0.062 (3)
H17A0.4756880.2142970.3911540.074*
H17B0.5731880.2515000.3355700.074*
N180.425 (2)0.636 (3)0.5816 (15)0.069 (7)
H18A0.4623310.6084090.5847750.083*
H18B0.4173800.6589420.5242450.083*
N230.4734 (18)0.4482 (18)0.4943 (17)0.069 (7)
H23A0.5199560.5104720.4886040.083*
H23B0.4662580.4164000.5509700.083*
N140.680 (3)0.797 (2)0.6445 (19)0.122 (15)
H14A0.7013680.8611110.6454170.146*
H14B0.6476450.7617370.5918450.146*
N240.739 (3)0.793 (2)0.7993 (19)0.100 (11)
H24A0.7642950.8562820.8100390.121*
H24B0.7448340.7553120.8452290.121*
N270.539 (2)0.278 (3)0.555 (2)0.128 (16)
H27A0.4738990.2456280.5535260.154*
H27B0.5701450.3047350.6114720.154*
N130.430 (2)0.4571 (17)0.3313 (17)0.069 (7)
H13A0.4773940.5191160.3302580.083*
H13B0.3924650.4308390.2777980.083*
C70.589 (2)0.287 (2)0.4737 (19)0.054 (7)
C50.5826 (14)0.6213 (16)0.0422 (15)0.027 (4)
C80.375 (3)0.642 (3)0.672 (2)0.078 (11)
C40.696 (2)0.756 (3)0.7201 (16)0.053 (3)
N150.5294 (16)0.5787 (18)0.0392 (16)0.068 (3)
H15A0.4647900.5528180.0376860.081*
H15B0.5585890.5761770.0946170.081*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0355 (13)0.0303 (12)0.0329 (11)0.0175 (11)0.0026 (10)0.0031 (10)
Se20.0303 (13)0.0375 (13)0.0375 (13)0.0175 (11)0.0049 (10)0.0024 (10)
Se30.0339 (13)0.0278 (12)0.0317 (10)0.0112 (11)0.0043 (10)0.0005 (10)
Se40.0430 (14)0.0356 (14)0.0414 (15)0.0168 (12)0.0050 (11)0.0042 (10)
Se50.0315 (12)0.0408 (13)0.0378 (13)0.0200 (11)0.0022 (10)0.0052 (10)
Se60.0348 (12)0.0347 (12)0.0326 (12)0.0222 (10)0.0023 (10)0.0028 (9)
Se70.0347 (6)0.0443 (6)0.0528 (8)0.0058 (4)0.0027 (5)0.0010 (5)
Se80.0499 (15)0.0416 (14)0.0355 (13)0.0304 (12)0.0065 (11)0.0028 (11)
Se90.0346 (5)0.0575 (7)0.0600 (8)0.0237 (5)0.0043 (5)0.0113 (6)
C60.035 (11)0.040 (12)0.037 (11)0.029 (11)0.001 (9)0.001 (9)
C20.12 (3)0.11 (3)0.043 (15)0.09 (2)0.048 (18)0.044 (17)
C90.035 (5)0.050 (6)0.057 (8)0.023 (4)0.001 (5)0.004 (5)
C30.064 (16)0.033 (12)0.021 (10)0.018 (11)0.005 (10)0.003 (9)
C10.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
N160.031 (10)0.080 (16)0.049 (12)0.037 (11)0.003 (9)0.000 (11)
N210.046 (5)0.092 (7)0.045 (6)0.040 (5)0.004 (4)0.003 (5)
N190.050 (5)0.106 (8)0.051 (6)0.053 (5)0.008 (4)0.001 (5)
N290.048 (5)0.127 (10)0.053 (8)0.042 (6)0.006 (5)0.028 (6)
N220.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
N260.082 (17)0.13 (2)0.036 (11)0.088 (17)0.006 (11)0.012 (13)
N110.051 (12)0.056 (12)0.026 (9)0.036 (11)0.002 (8)0.006 (9)
N120.094 (8)0.100 (8)0.048 (6)0.079 (7)0.009 (5)0.015 (5)
N280.111 (9)0.125 (10)0.059 (7)0.101 (8)0.027 (6)0.029 (7)
N250.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
N170.041 (5)0.079 (7)0.037 (6)0.009 (5)0.004 (4)0.008 (5)
N180.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
N230.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
N140.24 (4)0.055 (17)0.047 (15)0.06 (2)0.03 (2)0.021 (13)
N240.16 (3)0.067 (19)0.058 (17)0.05 (2)0.021 (19)0.002 (14)
N270.056 (18)0.26 (5)0.059 (18)0.07 (2)0.017 (14)0.04 (2)
N130.067 (16)0.059 (15)0.047 (13)0.006 (13)0.000 (12)0.016 (11)
C70.053 (16)0.10 (2)0.046 (14)0.062 (17)0.006 (12)0.003 (15)
C50.017 (9)0.034 (11)0.029 (10)0.011 (9)0.014 (8)0.004 (9)
C80.12 (3)0.15 (3)0.038 (14)0.12 (3)0.005 (16)0.010 (17)
C40.054 (6)0.043 (6)0.061 (8)0.024 (5)0.002 (5)0.004 (5)
N150.033 (4)0.092 (7)0.052 (7)0.011 (5)0.005 (4)0.016 (5)
Geometric parameters (Å, º) top
Se1—C11.86 (2)N11—H11B0.8600
Se2—C21.87 (3)N12—H12A0.8600
Se3—C31.86 (2)N12—H12B0.8600
Se4—C41.96 (3)N28—H28A0.8600
Se5—C51.835 (19)N28—H28B0.8600
Se6—C61.89 (2)N28—C81.32 (3)
Se7—C71.90 (3)N25—H25A0.8600
Se8—C81.79 (2)N25—H25B0.8600
Se9—C91.98 (3)N25—C51.42 (2)
C6—N161.27 (3)N17—H17A0.8600
C6—N261.33 (3)N17—H17B0.8600
C2—N211.26 (4)N17—C71.27 (3)
C2—N221.38 (3)N18—H18A0.8600
C9—N191.18 (4)N18—H18B0.8600
C9—N291.20 (3)N18—C81.43 (3)
C3—N231.32 (3)N23—H23A0.8600
C3—N131.34 (3)N23—H23B0.8600
C1—N111.32 (3)N14—H14A0.8600
C1—N121.31 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.26 (3)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.20 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.27 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.30 (3)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6122.7 (16)C8—N28—H28B120.0
N16—C6—N26121 (2)H25A—N25—H25B120.0
N26—C6—Se6115.9 (16)C5—N25—H25A120.0
N21—C2—Se2125 (2)C5—N25—H25B120.0
N21—C2—N22118 (3)H17A—N17—H17B120.0
N22—C2—Se2117 (2)C7—N17—H17A120.0
N19—C9—Se9116 (2)C7—N17—H17B120.0
N19—C9—N29127 (3)H18A—N18—H18B120.0
N29—C9—Se9115 (3)C8—N18—H18A120.0
N23—C3—Se3121.5 (17)C8—N18—H18B120.0
N23—C3—N13116 (2)C3—N23—H23A120.0
N13—C3—Se3122.6 (17)C3—N23—H23B120.0
N11—C1—Se1118.4 (19)H23A—N23—H23B120.0
N12—C1—Se1121.0 (15)H14A—N14—H14B120.0
N12—C1—N11120 (2)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120 (2)
H29A—N29—H29B120.0N17—C7—N27119 (3)
C2—N22—H22A120.0N27—C7—Se7121 (2)
C2—N22—H22B120.0N25—C5—Se5117.6 (15)
H22A—N22—H22B120.0N15—C5—Se5126.4 (16)
C6—N26—H26A120.0N15—C5—N25115.5 (19)
C6—N26—H26B120.0N28—C8—Se8127 (2)
H26A—N26—H26B120.0N28—C8—N18114 (2)
C1—N11—H11A120.0N18—C8—Se8119.8 (19)
C1—N11—H11B120.0N14—C4—Se4114 (2)
H11A—N11—H11B120.0N24—C4—Se4117 (2)
C1—N12—H12A120.0N24—C4—N14129 (4)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_303K) top
Crystal data top
CH4N2SeDx = 2.094 Mg m3
Mr = 123.02Cu Kα radiation, λ = 1.54184 Å
Trigonal, P31Cell parameters from 7386 reflections
a = 15.2813 (2) Åθ = 3.3–72.1°
c = 13.0272 (2) ŵ = 11.21 mm1
V = 2634.52 (8) Å3T = 303 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
SuperNova, Single source at offset/far, Atlas
diffractometer
3791 independent reflections
Radiation source: micro-focus sealed X-ray tube, SuperNova (Cu) X-ray Source3754 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.033
Detector resolution: 10.5384 pixels mm-1θmax = 72.2°, θmin = 3.3°
ω scansh = 1615
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1418
Tmin = 0.240, Tmax = 1.000l = 1115
7938 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0478P)2 + 0.205P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.027(Δ/σ)max = 0.001
wR(F2) = 0.075Δρmax = 0.40 e Å3
S = 1.07Δρmin = 0.39 e Å3
3791 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00070 (4)
1 restraintAbsolute structure: Classical Flack method preferred over Parsons because s.u. lower.
Primary atom site location: dualAbsolute structure parameter: 0.00 (5)
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30604 (5)0.35121 (5)0.09707 (4)0.03728 (17)
Se20.39423 (5)0.36028 (6)0.75801 (4)0.03868 (18)
Se30.30511 (5)0.27099 (5)0.42668 (5)0.03677 (17)
Se40.63095 (6)0.60745 (5)0.70716 (4)0.03992 (19)
Se50.72119 (5)0.69323 (5)0.05051 (5)0.03714 (17)
Se60.63403 (5)0.70198 (6)0.38293 (4)0.03698 (17)
Se70.72897 (5)0.37623 (6)0.47290 (6)0.0502 (2)
Se80.29803 (5)0.70017 (5)0.66503 (6)0.0428 (2)
Se91.06999 (5)1.02926 (6)0.46099 (7)0.0499 (2)
C60.7469 (5)0.6862 (5)0.3912 (5)0.0411 (14)
C20.2569 (5)0.3160 (5)0.7567 (5)0.0442 (16)
C90.9356 (5)0.9955 (5)0.4554 (5)0.0469 (16)
C30.4115 (5)0.4038 (5)0.4176 (5)0.0477 (17)
C10.3863 (5)0.2907 (5)0.0951 (4)0.0382 (15)
N160.8029 (4)0.6983 (5)0.3093 (4)0.0532 (15)
H16A0.8552580.6913620.3142350.064*
H16B0.7870360.7130740.2511240.064*
N210.2082 (4)0.3136 (5)0.8413 (4)0.0584 (17)
H21A0.1447800.2938680.8389210.070*
H21B0.2399730.3318060.8988730.070*
N190.8897 (5)1.0067 (5)0.5369 (4)0.0656 (19)
H19A0.8281240.9936150.5322250.079*
H19B0.9214911.0271270.5941850.079*
N290.8837 (5)0.9645 (6)0.3710 (5)0.080 (2)
H29A0.8222880.9521510.3695050.096*
H29B0.9107190.9562540.3166840.096*
N220.2063 (5)0.2879 (8)0.6709 (5)0.109 (4)
H22A0.1428970.2684040.6703840.130*
H22B0.2363850.2887520.6147440.130*
N260.7742 (5)0.6635 (6)0.4792 (4)0.074 (2)
H26A0.8269530.6570220.4817060.089*
H26B0.7392250.6551290.5337430.089*
N110.4347 (4)0.2923 (5)0.0105 (4)0.0520 (15)
H11A0.4695320.2622990.0089100.062*
H11B0.4313340.3234690.0430770.062*
N120.3924 (5)0.2426 (5)0.1763 (4)0.0652 (19)
H12A0.4274940.2128650.1736980.078*
H12B0.3612270.2409580.2318720.078*
N280.3863 (6)0.5973 (6)0.7520 (5)0.080 (2)
H28A0.4210850.5671610.7507390.096*
H28B0.3570410.5988510.8078000.096*
N250.5278 (4)0.6266 (5)0.1270 (4)0.0575 (17)
H25A0.4629050.5952060.1243440.069*
H25B0.5585140.6590060.1816910.069*
N170.5424 (5)0.2433 (5)0.3861 (5)0.0674 (19)
H17A0.4781630.2026960.3864160.081*
H17B0.5756140.2561970.3294740.081*
N180.4252 (6)0.6362 (7)0.5837 (5)0.100 (3)
H18A0.4591860.6052840.5859130.120*
H18B0.4216950.6637980.5275140.120*
N230.4716 (5)0.4480 (5)0.4966 (4)0.0661 (18)
H23A0.5220390.5083180.4905870.079*
H23B0.4603140.4164970.5540630.079*
N140.6792 (6)0.7995 (5)0.6442 (5)0.084 (2)
H14A0.7052070.8638190.6508470.101*
H14B0.6463790.7699130.5893670.101*
N240.7394 (5)0.7934 (4)0.8000 (5)0.070 (2)
H24A0.7649460.8577310.8053710.084*
H24B0.7468030.7599100.8489190.084*
N270.5366 (5)0.2640 (6)0.5568 (5)0.080 (2)
H27A0.4724060.2231810.5549120.096*
H27B0.5656280.2906410.6141370.096*
N130.4313 (6)0.4542 (5)0.3319 (5)0.094 (3)
H13A0.4822460.5143990.3281340.112*
H13B0.3933160.4271770.2791740.112*
C70.5900 (5)0.2858 (5)0.4724 (5)0.0473 (16)
C50.5807 (5)0.6251 (5)0.0467 (5)0.0398 (14)
C80.3778 (6)0.6415 (6)0.6678 (5)0.0540 (18)
C40.6894 (6)0.7467 (5)0.7177 (5)0.0467 (17)
N150.5312 (4)0.5745 (5)0.0363 (4)0.0659 (19)
H15A0.4662560.5436100.0373570.079*
H15B0.5639900.5725590.0890350.079*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0388 (4)0.0388 (4)0.0380 (3)0.0222 (3)0.0006 (3)0.0003 (3)
Se20.0325 (4)0.0428 (4)0.0397 (4)0.0180 (3)0.0006 (3)0.0040 (3)
Se30.0383 (4)0.0314 (4)0.0384 (3)0.0158 (3)0.0008 (3)0.0006 (3)
Se40.0414 (4)0.0330 (4)0.0413 (4)0.0155 (3)0.0000 (3)0.0002 (3)
Se50.0328 (4)0.0379 (4)0.0403 (3)0.0173 (3)0.0019 (3)0.0007 (3)
Se60.0359 (4)0.0393 (4)0.0396 (4)0.0217 (3)0.0010 (3)0.0001 (3)
Se70.0362 (4)0.0458 (4)0.0500 (5)0.0066 (3)0.0027 (3)0.0006 (3)
Se80.0521 (5)0.0429 (4)0.0424 (4)0.0304 (4)0.0026 (3)0.0017 (3)
Se90.0358 (4)0.0588 (5)0.0552 (4)0.0237 (4)0.0047 (3)0.0122 (4)
C60.040 (4)0.043 (4)0.045 (3)0.025 (3)0.002 (3)0.004 (3)
C20.036 (4)0.060 (5)0.040 (3)0.026 (3)0.002 (3)0.002 (3)
C90.043 (4)0.047 (4)0.051 (4)0.022 (3)0.001 (3)0.002 (3)
C30.058 (4)0.040 (4)0.035 (3)0.017 (3)0.001 (3)0.003 (3)
C10.042 (4)0.044 (4)0.031 (3)0.023 (3)0.001 (2)0.004 (3)
N160.044 (3)0.077 (4)0.047 (3)0.037 (3)0.005 (3)0.006 (3)
N210.043 (3)0.100 (5)0.034 (3)0.037 (4)0.002 (2)0.005 (3)
N190.055 (4)0.113 (6)0.046 (3)0.056 (4)0.001 (3)0.007 (3)
N290.045 (4)0.130 (7)0.056 (4)0.036 (4)0.005 (3)0.027 (4)
N220.051 (4)0.243 (11)0.041 (4)0.079 (6)0.012 (3)0.023 (5)
N260.078 (5)0.141 (7)0.044 (3)0.085 (5)0.002 (3)0.012 (4)
N110.060 (4)0.069 (4)0.043 (3)0.045 (3)0.009 (3)0.007 (3)
N120.093 (5)0.103 (5)0.041 (3)0.081 (5)0.011 (3)0.016 (3)
N280.117 (6)0.124 (7)0.050 (4)0.099 (6)0.020 (4)0.028 (4)
N250.042 (3)0.077 (4)0.041 (3)0.021 (3)0.006 (3)0.009 (3)
N170.040 (3)0.077 (5)0.056 (4)0.007 (3)0.002 (3)0.010 (3)
N180.121 (7)0.204 (9)0.048 (4)0.137 (7)0.021 (4)0.024 (5)
N230.062 (4)0.056 (4)0.047 (3)0.004 (3)0.009 (3)0.002 (3)
N140.156 (8)0.043 (4)0.053 (4)0.050 (4)0.023 (4)0.002 (3)
N240.108 (6)0.032 (3)0.053 (4)0.022 (3)0.013 (4)0.004 (3)
N270.038 (4)0.115 (6)0.060 (4)0.018 (4)0.001 (3)0.002 (4)
N130.123 (7)0.044 (4)0.050 (4)0.005 (4)0.014 (4)0.007 (3)
C70.037 (4)0.045 (4)0.054 (4)0.016 (3)0.003 (3)0.002 (3)
C50.036 (3)0.045 (4)0.035 (3)0.017 (3)0.003 (3)0.002 (3)
C80.059 (5)0.076 (5)0.043 (4)0.046 (4)0.005 (3)0.007 (3)
C40.053 (4)0.045 (4)0.042 (4)0.024 (3)0.004 (3)0.002 (3)
N150.037 (3)0.092 (5)0.046 (3)0.015 (3)0.006 (3)0.014 (3)
Geometric parameters (Å, º) top
Se1—C11.869 (6)N11—H11B0.8600
Se2—C21.855 (7)N12—H12A0.8600
Se3—C31.865 (7)N12—H12B0.8600
Se4—C41.856 (7)N28—H28A0.8600
Se5—C51.860 (6)N28—H28B0.8600
Se6—C61.860 (6)N28—C81.328 (9)
Se7—C71.866 (7)N25—H25A0.8600
Se8—C81.840 (7)N25—H25B0.8600
Se9—C91.852 (7)N25—C51.330 (8)
C6—N161.322 (8)N17—H17A0.8600
C6—N261.324 (8)N17—H17B0.8600
C2—N211.320 (8)N17—C71.320 (9)
C2—N221.304 (8)N18—H18A0.8600
C9—N191.330 (8)N18—H18B0.8600
C9—N291.299 (9)N18—C81.337 (9)
C3—N231.318 (8)N23—H23A0.8600
C3—N131.302 (8)N23—H23B0.8600
C1—N111.320 (8)N14—H14A0.8600
C1—N121.318 (8)N14—H14B0.8600
N16—H16A0.8600N14—C41.311 (9)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.302 (9)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.310 (9)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.324 (8)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.9 (5)C8—N28—H28B120.0
N16—C6—N26117.9 (6)H25A—N25—H25B120.0
N26—C6—Se6121.3 (5)C5—N25—H25A120.0
N21—C2—Se2121.4 (5)C5—N25—H25B120.0
N22—C2—Se2120.3 (5)H17A—N17—H17B120.0
N22—C2—N21118.3 (6)C7—N17—H17A120.0
N19—C9—Se9121.1 (5)C7—N17—H17B120.0
N29—C9—Se9121.7 (5)H18A—N18—H18B120.0
N29—C9—N19117.2 (6)C8—N18—H18A120.0
N23—C3—Se3120.9 (5)C8—N18—H18B120.0
N13—C3—Se3121.1 (5)C3—N23—H23A120.0
N13—C3—N23118.0 (6)C3—N23—H23B120.0
N11—C1—Se1120.1 (5)H23A—N23—H23B120.0
N12—C1—Se1120.8 (5)H14A—N14—H14B120.0
N12—C1—N11119.1 (6)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7120.7 (5)
H29A—N29—H29B120.0N27—C7—Se7121.3 (5)
C2—N22—H22A120.0N27—C7—N17118.0 (6)
C2—N22—H22B120.0N25—C5—Se5120.7 (5)
H22A—N22—H22B120.0N15—C5—Se5120.7 (5)
C6—N26—H26A120.0N15—C5—N25118.5 (6)
C6—N26—H26B120.0N28—C8—Se8121.4 (5)
H26A—N26—H26B120.0N28—C8—N18116.9 (7)
C1—N11—H11A120.0N18—C8—Se8121.6 (5)
C1—N11—H11B120.0N14—C4—Se4121.0 (5)
H11A—N11—H11B120.0N24—C4—Se4120.2 (5)
C1—N12—H12A120.0N24—C4—N14118.8 (7)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_313K) top
Crystal data top
CH4N2SeDx = 2.089 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3411 reflections
a = 15.2940 (5) Åθ = 3.5–26.4°
c = 13.0350 (4) ŵ = 9.37 mm1
V = 2640.48 (19) Å3T = 313 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8231 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5822 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.338, Tmax = 0.626l = 1717
28408 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + 46.5028P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.081(Δ/σ)max < 0.001
wR(F2) = 0.144Δρmax = 1.74 e Å3
S = 1.08Δρmin = 1.92 e Å3
8231 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00066 (4)
50 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30575 (18)0.35152 (18)0.09653 (16)0.0364 (5)
Se20.39364 (19)0.36082 (19)0.75568 (17)0.0383 (6)
Se30.30445 (18)0.27075 (17)0.42849 (18)0.0357 (5)
Se40.6315 (2)0.6085 (2)0.70793 (17)0.0431 (7)
Se50.72106 (18)0.69334 (19)0.04976 (19)0.0391 (6)
Se60.63415 (18)0.70144 (19)0.38296 (16)0.0344 (5)
Se70.73130 (19)0.3741 (2)0.46978 (19)0.0514 (8)
Se80.29963 (19)0.70130 (18)0.6658 (2)0.0430 (6)
Se91.06951 (19)1.0313 (2)0.4656 (2)0.0530 (7)
C60.7462 (15)0.6804 (16)0.3873 (17)0.038 (5)
C20.257 (3)0.319 (3)0.763 (2)0.085 (12)
C90.927 (2)0.9906 (15)0.462 (2)0.057 (7)
C30.4123 (18)0.4009 (17)0.4179 (17)0.045 (5)
C10.3836 (18)0.2889 (19)0.0948 (15)0.041 (6)
N160.8019 (13)0.6924 (16)0.3086 (14)0.049 (5)
H16A0.8529610.6835170.3140980.059*
H16B0.7880280.7091910.2504430.059*
N210.2082 (19)0.3108 (19)0.8405 (18)0.076 (7)
H21A0.1437950.2851620.8367110.092*
H21B0.2382240.3305260.8987380.092*
N190.8872 (18)0.996 (2)0.5380 (19)0.090 (9)
H19A0.8258400.9833230.5357390.108*
H19B0.9194981.0119260.5952760.108*
N290.8860 (18)0.9683 (18)0.3800 (18)0.075 (7)
H29A0.8246580.9553010.3741740.090*
H29B0.9180440.9655020.3270450.090*
N220.206 (3)0.286 (3)0.667 (3)0.122 (11)
H22A0.1412990.2605740.6640090.146*
H22B0.2392290.2916950.6118700.146*
N260.7657 (17)0.655 (2)0.4775 (14)0.071 (7)
H26A0.8165180.6454520.4843940.085*
H26B0.7277110.6469610.5292720.085*
N110.4324 (13)0.2923 (14)0.0086 (12)0.041 (4)
H11A0.4670800.2621660.0055620.049*
H11B0.4291190.3245720.0439570.049*
N120.3895 (18)0.2403 (19)0.1722 (13)0.070 (7)
H12A0.4244760.2105840.1680930.084*
H12B0.3584890.2375220.2282440.084*
N280.394 (2)0.605 (2)0.7554 (14)0.080 (2)
H28A0.4390920.5875510.7534900.096*
H28B0.3629350.6010090.8119180.096*
N250.5284 (13)0.6225 (15)0.1298 (14)0.053 (5)
H25A0.4637650.5949550.1275020.064*
H25B0.5603470.6507190.1853870.064*
N170.5430 (14)0.2477 (16)0.3900 (17)0.072 (8)
H17A0.4781370.2142110.3885500.086*
H17B0.5769300.2543910.3350280.086*
N180.4273 (18)0.642 (2)0.5838 (18)0.077 (7)
H18A0.4717360.6234370.5868660.092*
H18B0.4164150.6633750.5268000.092*
N230.4735 (16)0.4472 (17)0.4967 (16)0.071 (7)
H23A0.5216280.5086360.4905250.085*
H23B0.4648260.4157590.5538050.085*
N140.680 (2)0.799 (2)0.643 (2)0.114 (10)
H14A0.7072210.8639500.6430070.137*
H14B0.6441970.7648900.5912720.137*
N240.742 (2)0.794 (2)0.800 (2)0.098 (9)
H24A0.7725290.8583020.8080960.118*
H24B0.7456910.7564580.8474770.118*
N270.542 (2)0.279 (2)0.556 (2)0.092 (8)
H27A0.4766380.2461000.5575010.110*
H27B0.5747670.3067510.6116450.110*
N130.431 (2)0.4557 (19)0.3309 (18)0.084 (7)
H13A0.4802910.5168910.3288460.100*
H13B0.3937450.4292600.2776960.100*
C70.589 (2)0.287 (3)0.4730 (18)0.0473 (16)
C50.5821 (14)0.6215 (16)0.0423 (14)0.030 (4)
C80.372 (2)0.638 (3)0.6729 (19)0.073 (9)
C40.692 (2)0.754 (3)0.7195 (17)0.069 (10)
N150.5296 (15)0.5784 (17)0.0369 (15)0.066 (7)
H15A0.4650890.5519990.0350690.079*
H15B0.5587080.5757210.0923010.079*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0398 (13)0.0358 (12)0.0356 (11)0.0204 (11)0.0043 (9)0.0021 (10)
Se20.0335 (13)0.0410 (13)0.0410 (13)0.0189 (11)0.0041 (10)0.0012 (10)
Se30.0368 (13)0.0303 (11)0.0339 (10)0.0122 (10)0.0023 (9)0.0000 (10)
Se40.0441 (14)0.0394 (14)0.0429 (15)0.0188 (12)0.0040 (10)0.0024 (10)
Se50.0342 (12)0.0427 (13)0.0425 (12)0.0207 (11)0.0039 (10)0.0059 (10)
Se60.0366 (12)0.0386 (12)0.0356 (12)0.0246 (10)0.0001 (9)0.0018 (9)
Se70.0367 (14)0.0453 (15)0.0500 (16)0.0039 (11)0.0023 (11)0.0083 (11)
Se80.0541 (15)0.0426 (14)0.0430 (14)0.0321 (12)0.0076 (11)0.0046 (10)
Se90.0403 (14)0.0562 (17)0.0569 (16)0.0201 (13)0.0014 (12)0.0061 (12)
C60.029 (10)0.043 (12)0.050 (13)0.023 (10)0.001 (9)0.001 (10)
C20.15 (3)0.12 (3)0.045 (15)0.11 (3)0.041 (19)0.048 (17)
C90.09 (2)0.046 (14)0.049 (15)0.042 (15)0.020 (14)0.006 (12)
C30.051 (14)0.041 (13)0.036 (11)0.016 (11)0.005 (10)0.008 (10)
C10.043 (13)0.065 (16)0.022 (10)0.032 (12)0.015 (8)0.001 (10)
N160.034 (10)0.093 (16)0.045 (10)0.049 (11)0.001 (8)0.005 (10)
N210.064 (10)0.099 (12)0.063 (10)0.038 (8)0.001 (8)0.003 (9)
N190.068 (16)0.16 (3)0.062 (15)0.073 (19)0.017 (12)0.041 (17)
N290.058 (10)0.090 (11)0.066 (11)0.028 (8)0.018 (8)0.004 (8)
N220.111 (14)0.141 (15)0.116 (15)0.065 (11)0.000 (10)0.003 (10)
N260.089 (16)0.15 (2)0.037 (10)0.105 (18)0.006 (10)0.018 (13)
N110.052 (11)0.062 (12)0.022 (8)0.039 (10)0.001 (8)0.007 (8)
N120.104 (18)0.14 (2)0.019 (9)0.102 (18)0.020 (10)0.024 (11)
N280.117 (6)0.124 (7)0.050 (4)0.098 (6)0.020 (4)0.028 (4)
N250.022 (9)0.077 (15)0.046 (11)0.014 (9)0.014 (8)0.014 (10)
N170.023 (10)0.077 (16)0.059 (14)0.019 (10)0.009 (9)0.034 (11)
N180.078 (10)0.106 (11)0.071 (11)0.064 (9)0.002 (8)0.009 (8)
N230.063 (15)0.061 (14)0.047 (12)0.000 (12)0.002 (11)0.013 (10)
N140.128 (14)0.097 (13)0.103 (13)0.046 (10)0.009 (10)0.002 (10)
N240.107 (13)0.093 (12)0.091 (12)0.046 (9)0.006 (9)0.008 (9)
N270.077 (11)0.108 (13)0.080 (12)0.039 (9)0.003 (9)0.004 (9)
N130.090 (11)0.065 (10)0.064 (10)0.014 (8)0.002 (9)0.002 (8)
C70.038 (4)0.045 (4)0.054 (4)0.017 (3)0.003 (3)0.002 (3)
C50.025 (9)0.048 (12)0.023 (9)0.022 (9)0.007 (7)0.002 (8)
C80.11 (2)0.14 (3)0.037 (13)0.11 (2)0.005 (14)0.005 (15)
C40.08 (2)0.14 (3)0.022 (12)0.08 (2)0.016 (12)0.011 (14)
N150.042 (12)0.081 (16)0.048 (12)0.010 (11)0.008 (9)0.035 (11)
Geometric parameters (Å, º) top
Se1—C11.86 (2)N11—H11B0.8600
Se2—C21.86 (4)N12—H12A0.8600
Se3—C31.85 (2)N12—H12B0.8600
Se4—C41.94 (4)N28—H28A0.8600
Se5—C51.844 (19)N28—H28B0.8600
Se6—C61.89 (2)N28—C81.30 (3)
Se7—C71.91 (3)N25—H25A0.8600
Se8—C81.80 (2)N25—H25B0.8600
Se9—C91.94 (3)N25—C51.41 (2)
C6—N161.29 (3)N17—H17A0.8600
C6—N261.32 (3)N17—H17B0.8600
C2—N211.23 (4)N17—C71.26 (3)
C2—N221.43 (4)N18—H18A0.8600
C9—N191.18 (3)N18—H18B0.8600
C9—N291.21 (3)N18—C81.42 (3)
C3—N231.33 (3)N23—H23A0.8600
C3—N131.35 (3)N23—H23B0.8600
C1—N111.34 (2)N14—H14A0.8600
C1—N121.28 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.28 (4)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.26 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.28 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.27 (3)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6122.9 (16)C8—N28—H28B120.0
N16—C6—N26121.2 (19)H25A—N25—H25B120.0
N26—C6—Se6115.9 (16)C5—N25—H25A120.0
N21—C2—Se2127 (2)C5—N25—H25B120.0
N21—C2—N22119 (3)H17A—N17—H17B120.0
N22—C2—Se2114 (2)C7—N17—H17A120.0
N19—C9—Se9120 (2)C7—N17—H17B120.0
N19—C9—N29123 (3)H18A—N18—H18B120.0
N29—C9—Se9117 (2)C8—N18—H18A120.0
N23—C3—Se3121.8 (17)C8—N18—H18B120.0
N23—C3—N13116 (2)C3—N23—H23A120.0
N13—C3—Se3121.9 (19)C3—N23—H23B120.0
N11—C1—Se1118.6 (16)H23A—N23—H23B120.0
N12—C1—Se1122.4 (15)H14A—N14—H14B120.0
N12—C1—N11119 (2)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7118.7 (19)
H29A—N29—H29B120.0N17—C7—N27122 (3)
C2—N22—H22A120.0N27—C7—Se7119 (2)
C2—N22—H22B120.0N25—C5—Se5117.1 (14)
H22A—N22—H22B120.0N15—C5—Se5126.3 (15)
C6—N26—H26A120.0N15—C5—N25116.3 (18)
C6—N26—H26B120.0N28—C8—Se8126.6 (19)
H26A—N26—H26B120.0N28—C8—N18116 (2)
C1—N11—H11A120.0N18—C8—Se8116.6 (19)
C1—N11—H11B120.0N14—C4—Se4116 (2)
H11A—N11—H11B120.0N24—C4—Se4116 (2)
C1—N12—H12A120.0N24—C4—N14127 (4)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_323K) top
Crystal data top
CH4N2SeDx = 2.090 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3345 reflections
a = 15.3052 (6) Åθ = 4.1–26.3°
c = 13.0398 (4) ŵ = 9.38 mm1
V = 2645.33 (2) Å3T = 323 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8247 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5710 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 1919
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 2020
Tmin = 0.338, Tmax = 0.626l = 1717
28481 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + 85.4123P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.098(Δ/σ)max < 0.001
wR(F2) = 0.179Δρmax = 0.74 e Å3
S = 1.05Δρmin = 1.92 e Å3
8247 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00066 (4)
107 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.3053 (2)0.3519 (2)0.0959 (2)0.0369 (6)
Se20.3930 (2)0.3607 (2)0.7550 (2)0.0387 (7)
Se30.3043 (2)0.2703 (2)0.4291 (2)0.0373 (6)
Se40.6316 (3)0.6087 (3)0.7087 (2)0.0470 (8)
Se50.7210 (2)0.6931 (3)0.0485 (3)0.0443 (7)
Se60.6343 (2)0.7008 (2)0.38294 (19)0.0351 (6)
Se70.7328 (2)0.3724 (2)0.4684 (2)0.0533 (10)
Se80.3002 (2)0.7020 (2)0.6669 (3)0.0457 (8)
Se91.0691 (2)1.0326 (3)0.4680 (2)0.0542 (9)
C60.7425 (19)0.674 (2)0.389 (2)0.038 (6)
C20.256 (3)0.319 (2)0.761 (4)0.093 (13)
C90.917 (3)0.983 (2)0.464 (2)0.056 (9)
C30.412 (2)0.400 (2)0.4197 (19)0.041 (6)
C10.381 (2)0.289 (2)0.0974 (19)0.034 (6)
N160.7991 (16)0.689 (2)0.3087 (16)0.079 (11)
H16A0.8511960.6818310.3134930.095*
H16B0.7844720.7059650.2510870.095*
N210.206 (3)0.312 (3)0.840 (3)0.113 (13)
H21A0.1423040.2898120.8356350.135*
H21B0.2356080.3292020.8987330.135*
N190.886 (2)0.989 (2)0.539 (3)0.082 (9)
H19A0.8278570.9854890.5412920.098*
H19B0.9193000.9974350.5945620.098*
N290.887 (2)0.972 (2)0.383 (2)0.069 (8)
H29A0.8293730.9668390.3716820.083*
H29B0.9219720.9687300.3333080.083*
N220.205 (4)0.290 (4)0.663 (4)0.158 (19)
H22A0.1413140.2679380.6599020.190*
H22B0.2386040.2946880.6088290.190*
N260.762 (2)0.649 (3)0.4763 (17)0.079 (11)
H26A0.8139050.6413860.4829830.095*
H26B0.7237290.6398410.5280930.095*
N110.4297 (16)0.2925 (17)0.0070 (14)0.039 (5)
H11A0.4637700.2618330.0025150.047*
H11B0.4259030.3252080.0447530.047*
N120.388 (2)0.241 (2)0.1705 (16)0.075 (10)
H12A0.4226510.2112580.1642620.090*
H12B0.3585620.2382040.2275930.090*
N280.3984 (18)0.6086 (17)0.7583 (18)0.046 (5)
H28A0.4392970.5857080.7529430.055*
H28B0.3714410.6072640.8165870.055*
N250.5271 (17)0.6212 (18)0.1311 (18)0.050 (6)
H25A0.4629350.5966630.1264610.060*
H25B0.5574920.6465140.1881190.060*
N170.544 (2)0.246 (2)0.397 (2)0.070 (8)
H17A0.4798350.2104890.4007260.084*
H17B0.5748190.2495880.3404750.084*
N180.429 (2)0.643 (2)0.584 (2)0.076 (8)
H18A0.4681150.6176880.5894570.092*
H18B0.4214900.6647160.5263170.092*
N230.475 (2)0.449 (2)0.4976 (19)0.081 (10)
H23A0.5222240.5104770.4900600.097*
H23B0.4692050.4182210.5547870.097*
N140.676 (3)0.803 (4)0.641 (3)0.135 (16)
H14A0.7020580.8670510.6444860.162*
H14B0.6403510.7698510.5892540.162*
N240.746 (3)0.793 (3)0.802 (3)0.114 (13)
H24A0.7753570.8567650.8126780.137*
H24B0.7519550.7540600.8454490.137*
N270.543 (3)0.286 (3)0.559 (3)0.107 (12)
H27A0.4786080.2494330.5606530.129*
H27B0.5757630.3177260.6131950.129*
N130.430 (3)0.456 (3)0.335 (2)0.092 (10)
H13A0.4782610.5175880.3340030.110*
H13B0.3922670.4307480.2814670.110*
C70.593 (2)0.2929 (19)0.473 (2)0.049 (7)
C50.5829 (15)0.6199 (16)0.0443 (16)0.022 (4)
C80.376 (2)0.648 (2)0.673 (3)0.076 (10)
C40.693 (3)0.754 (3)0.716 (3)0.085 (13)
N150.531 (2)0.580 (2)0.0373 (19)0.066 (8)
H15A0.4667320.5572600.0368550.079*
H15B0.5600290.5773810.0924070.079*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0425 (17)0.0332 (14)0.0357 (13)0.0194 (13)0.0068 (11)0.0023 (12)
Se20.0347 (15)0.0390 (15)0.0426 (16)0.0186 (13)0.0074 (12)0.0039 (12)
Se30.0375 (15)0.0317 (14)0.0348 (13)0.0116 (13)0.0018 (11)0.0001 (12)
Se40.0482 (18)0.0455 (19)0.0443 (19)0.0212 (15)0.0043 (13)0.0012 (13)
Se50.0395 (16)0.0482 (17)0.0478 (16)0.0239 (14)0.0082 (13)0.0122 (13)
Se60.0387 (15)0.0406 (15)0.0376 (15)0.0285 (13)0.0019 (11)0.0012 (11)
Se70.0370 (17)0.0479 (18)0.054 (2)0.0054 (13)0.0027 (14)0.0118 (14)
Se80.058 (2)0.0460 (17)0.0454 (17)0.0347 (15)0.0084 (14)0.0060 (13)
Se90.0412 (17)0.055 (2)0.057 (2)0.0164 (15)0.0022 (14)0.0023 (15)
C60.031 (13)0.044 (15)0.045 (14)0.024 (12)0.002 (11)0.002 (11)
C20.094 (14)0.094 (14)0.092 (14)0.048 (8)0.001 (6)0.003 (6)
C90.10 (3)0.032 (14)0.043 (16)0.041 (17)0.019 (17)0.000 (12)
C30.050 (16)0.037 (14)0.028 (12)0.016 (12)0.009 (11)0.008 (10)
C10.032 (7)0.038 (7)0.031 (7)0.016 (5)0.007 (5)0.004 (5)
N160.11 (2)0.18 (3)0.032 (12)0.13 (3)0.007 (13)0.022 (16)
N210.112 (13)0.114 (13)0.112 (13)0.056 (7)0.000 (3)0.000 (3)
N190.079 (12)0.091 (13)0.079 (13)0.045 (10)0.005 (9)0.013 (10)
N290.057 (11)0.080 (12)0.064 (11)0.028 (9)0.019 (9)0.002 (9)
N220.158 (19)0.159 (19)0.158 (19)0.080 (10)0.000 (3)0.000 (3)
N260.11 (2)0.18 (3)0.032 (12)0.13 (3)0.007 (13)0.022 (16)
N110.045 (13)0.062 (14)0.021 (10)0.034 (12)0.012 (9)0.014 (9)
N120.13 (3)0.14 (3)0.018 (11)0.11 (2)0.016 (13)0.016 (14)
N280.057 (10)0.053 (10)0.034 (8)0.033 (8)0.005 (7)0.013 (7)
N250.035 (9)0.063 (10)0.050 (10)0.022 (8)0.016 (7)0.006 (8)
N170.062 (11)0.064 (11)0.070 (11)0.021 (9)0.004 (9)0.013 (9)
N180.080 (12)0.096 (13)0.074 (12)0.060 (10)0.001 (9)0.010 (9)
N230.09 (2)0.070 (19)0.034 (13)0.000 (16)0.006 (13)0.025 (13)
N140.145 (19)0.126 (19)0.129 (19)0.063 (12)0.004 (11)0.001 (11)
N240.118 (16)0.114 (16)0.109 (16)0.057 (11)0.002 (10)0.005 (10)
N270.099 (15)0.118 (16)0.098 (15)0.049 (11)0.002 (10)0.006 (10)
N130.097 (14)0.080 (13)0.074 (13)0.025 (9)0.003 (10)0.000 (10)
C70.049 (8)0.054 (8)0.050 (8)0.030 (6)0.002 (5)0.003 (5)
C50.019 (10)0.026 (11)0.023 (10)0.013 (9)0.009 (8)0.001 (8)
C80.076 (11)0.080 (11)0.077 (12)0.042 (7)0.001 (5)0.001 (5)
C40.086 (14)0.087 (14)0.085 (14)0.045 (8)0.002 (6)0.001 (6)
N150.051 (15)0.081 (19)0.044 (14)0.016 (14)0.018 (12)0.041 (14)
Geometric parameters (Å, º) top
Se1—C11.84 (3)N11—H11B0.8600
Se2—C21.87 (4)N12—H12A0.8600
Se3—C31.84 (3)N12—H12B0.8600
Se4—C41.94 (5)N28—H28A0.8600
Se5—C51.83 (2)N28—H28B0.8600
Se6—C61.89 (2)N28—C81.38 (4)
Se7—C71.85 (3)N25—H25A0.8600
Se8—C81.73 (4)N25—H25B0.8600
Se9—C92.06 (4)N25—C51.42 (3)
C6—N161.30 (3)N17—H17A0.8600
C6—N261.29 (3)N17—H17B0.8600
C2—N211.25 (5)N17—C71.23 (4)
C2—N221.44 (6)N18—H18A0.8600
C9—N191.11 (4)N18—H18B0.8600
C9—N291.13 (4)N18—C81.44 (5)
C3—N231.35 (4)N23—H23A0.8600
C3—N131.34 (4)N23—H23B0.8600
C1—N111.38 (3)N14—H14A0.8600
C1—N121.24 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.33 (5)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.33 (5)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.34 (4)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.28 (3)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6120.7 (19)C8—N28—H28B120.0
N26—C6—Se6117.4 (19)H25A—N25—H25B120.0
N26—C6—N16122 (2)C5—N25—H25A120.0
N21—C2—Se2127 (4)C5—N25—H25B120.0
N21—C2—N22119 (4)H17A—N17—H17B120.0
N22—C2—Se2114 (4)C7—N17—H17A120.0
N19—C9—Se9114 (3)C7—N17—H17B120.0
N19—C9—N29132 (4)H18A—N18—H18B120.0
N29—C9—Se9112 (3)C8—N18—H18A120.0
N23—C3—Se3124 (2)C8—N18—H18B120.0
N13—C3—Se3122 (2)C3—N23—H23A120.0
N13—C3—N23114 (3)C3—N23—H23B120.0
N11—C1—Se1116.1 (19)H23A—N23—H23B120.0
N12—C1—Se1125 (2)H14A—N14—H14B120.0
N12—C1—N11118 (2)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7122 (3)
H29A—N29—H29B120.0N17—C7—N27118 (3)
C2—N22—H22A120.0N27—C7—Se7120 (3)
C2—N22—H22B120.0N25—C5—Se5119.0 (17)
H22A—N22—H22B120.0N15—C5—Se5124.5 (18)
C6—N26—H26A120.0N15—C5—N25115 (2)
C6—N26—H26B120.0N28—C8—Se8128 (3)
H26A—N26—H26B120.0N28—C8—N18111 (3)
C1—N11—H11A120.0N18—C8—Se8121 (3)
C1—N11—H11B120.0N14—C4—Se4119 (4)
H11A—N11—H11B120.0N14—C4—N24128 (5)
C1—N12—H12A120.0N24—C4—Se4113 (3)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_333K) top
Crystal data top
CH4N2SeDx = 2.086 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3264 reflections
a = 15.3150 (6) Åθ = 4.1–25.9°
c = 13.0481 (5) ŵ = 9.36 mm1
V = 2650.4 (2) Å3T = 333 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8258 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5566 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.338, Tmax = 0.626l = 1717
28577 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0127P)2 + 41.939P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.078(Δ/σ)max < 0.001
wR(F2) = 0.149Δρmax = 0.56 e Å3
S = 1.06Δρmin = 1.90 e Å3
8258 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00065 (5)
80 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30573 (18)0.35167 (17)0.09650 (16)0.0385 (5)
Se20.39302 (19)0.36063 (19)0.75571 (17)0.0406 (6)
Se30.30470 (18)0.27103 (17)0.42838 (18)0.0385 (5)
Se40.6316 (2)0.6084 (2)0.70808 (16)0.0464 (7)
Se50.72130 (18)0.69301 (19)0.04964 (19)0.0428 (6)
Se60.63446 (18)0.7016 (2)0.38266 (16)0.0384 (5)
Se70.73160 (19)0.3737 (2)0.46959 (18)0.0544 (8)
Se80.29941 (19)0.70144 (18)0.6668 (2)0.0476 (7)
Se91.06956 (19)1.0320 (2)0.4659 (2)0.0556 (7)
C60.7429 (15)0.6773 (18)0.3881 (16)0.044 (5)
C20.261 (3)0.322 (3)0.761 (3)0.083 (9)
C90.927 (2)0.9885 (19)0.4623 (18)0.055 (6)
C30.4113 (17)0.4023 (16)0.4178 (16)0.045 (5)
C10.3820 (16)0.2900 (17)0.0935 (14)0.037 (5)
N160.7999 (13)0.6908 (15)0.3090 (13)0.052 (5)
H16A0.8522860.6842850.3150720.062*
H16B0.7853330.7063570.2506530.062*
N210.2063 (19)0.3071 (19)0.8399 (18)0.083 (7)
H21A0.1417150.2761390.8343380.100*
H21B0.2340680.3276280.8989970.100*
N190.8871 (18)0.996 (2)0.5379 (18)0.096 (10)
H19A0.8275060.9886070.5342970.116*
H19B0.9179341.0097910.5958430.116*
N290.8860 (18)0.9697 (19)0.3793 (18)0.081 (7)
H29A0.8264100.9615380.3734440.097*
H29B0.9164160.9644680.3262910.097*
N220.205 (2)0.285 (2)0.669 (2)0.118 (10)
H22A0.1401020.2543980.6697890.142*
H22B0.2360190.2918980.6116870.142*
N260.7650 (16)0.6538 (16)0.4769 (15)0.061 (5)
H26A0.8172870.6471690.4830530.074*
H26B0.7271710.6448290.5291770.074*
N110.4337 (13)0.2924 (14)0.0084 (12)0.044 (4)
H11A0.4689270.2629390.0081510.053*
H11B0.4312870.3235330.0455150.053*
N120.3899 (17)0.2410 (18)0.1719 (13)0.072 (7)
H12A0.4262820.2128770.1672910.087*
H12B0.3586440.2368910.2280990.087*
N280.3925 (17)0.6042 (16)0.7555 (16)0.064 (6)
H28A0.4375760.5863550.7545310.077*
H28B0.3601530.5990050.8111410.077*
N250.5293 (13)0.6226 (16)0.1302 (14)0.060 (6)
H25A0.4647020.5945760.1279040.072*
H25B0.5610370.6509800.1857850.072*
N170.5441 (15)0.2473 (15)0.3887 (16)0.063 (6)
H17A0.4793920.2109940.3888220.076*
H17B0.5771730.2551310.3329450.076*
N180.4294 (18)0.645 (2)0.5855 (18)0.084 (7)
H18A0.4734960.6260380.5893510.100*
H18B0.4201720.6674900.5285010.100*
N230.4715 (16)0.4480 (17)0.4970 (16)0.076 (7)
H23A0.5197570.5093140.4914160.091*
H23B0.4622610.4162180.5539640.091*
N140.678 (3)0.799 (3)0.643 (3)0.132 (12)
H14A0.7019500.8629550.6449210.158*
H14B0.6433310.7649690.5902920.158*
N240.741 (2)0.793 (2)0.801 (2)0.105 (9)
H24A0.7684740.8571470.8096100.126*
H24B0.7471030.7563820.8467820.126*
N270.543 (2)0.279 (2)0.557 (2)0.099 (9)
H27A0.4782420.2430700.5579680.119*
H27B0.5755290.3081260.6116520.119*
N130.4291 (19)0.4550 (19)0.3320 (18)0.089 (7)
H13A0.4780570.5161860.3292690.107*
H13B0.3916150.4279160.2791090.107*
C70.5913 (18)0.2899 (16)0.4718 (18)0.054 (6)
C50.5831 (13)0.6220 (15)0.0431 (14)0.031 (4)
C80.373 (2)0.640 (3)0.6716 (18)0.076 (9)
C40.692 (2)0.753 (2)0.7186 (16)0.070 (9)
N150.5301 (14)0.5779 (17)0.0372 (15)0.072 (7)
H15A0.4655580.5510030.0354130.086*
H15B0.5592470.5753410.0925560.086*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0423 (14)0.0377 (12)0.0381 (11)0.0220 (11)0.0040 (9)0.0019 (10)
Se20.0352 (13)0.0437 (13)0.0440 (13)0.0205 (11)0.0030 (10)0.0015 (10)
Se30.0407 (13)0.0316 (11)0.0378 (10)0.0141 (11)0.0026 (10)0.0002 (10)
Se40.0486 (14)0.0405 (14)0.0457 (15)0.0190 (12)0.0057 (11)0.0030 (10)
Se50.0371 (13)0.0471 (14)0.0451 (13)0.0217 (11)0.0029 (10)0.0057 (10)
Se60.0412 (13)0.0439 (13)0.0390 (12)0.0280 (11)0.0012 (10)0.0026 (9)
Se70.0375 (14)0.0496 (15)0.0528 (16)0.0042 (11)0.0009 (11)0.0084 (11)
Se80.0585 (16)0.0488 (14)0.0483 (14)0.0364 (13)0.0077 (11)0.0053 (11)
Se90.0408 (14)0.0602 (17)0.0590 (16)0.0202 (13)0.0002 (12)0.0064 (12)
C60.032 (11)0.069 (16)0.045 (12)0.037 (12)0.003 (9)0.003 (11)
C20.085 (10)0.085 (10)0.081 (10)0.043 (6)0.001 (5)0.004 (5)
C90.081 (18)0.052 (14)0.048 (14)0.046 (14)0.007 (13)0.011 (11)
C30.055 (14)0.034 (11)0.033 (10)0.012 (10)0.003 (10)0.007 (9)
C10.033 (11)0.054 (13)0.026 (10)0.023 (10)0.011 (8)0.000 (9)
N160.041 (10)0.097 (16)0.041 (10)0.052 (11)0.007 (8)0.012 (10)
N210.069 (10)0.104 (12)0.069 (10)0.038 (8)0.002 (8)0.003 (9)
N190.071 (16)0.17 (3)0.069 (16)0.072 (18)0.023 (13)0.053 (17)
N290.066 (10)0.097 (11)0.070 (11)0.033 (8)0.017 (8)0.001 (8)
N220.107 (13)0.141 (14)0.112 (14)0.065 (10)0.002 (10)0.006 (10)
N260.063 (9)0.086 (10)0.058 (9)0.054 (8)0.002 (7)0.005 (8)
N110.054 (11)0.063 (12)0.027 (8)0.038 (10)0.003 (8)0.008 (8)
N120.107 (18)0.14 (2)0.021 (9)0.103 (18)0.014 (10)0.016 (11)
N280.076 (10)0.081 (10)0.052 (9)0.051 (8)0.008 (8)0.008 (8)
N250.026 (9)0.098 (16)0.046 (11)0.023 (10)0.016 (8)0.010 (11)
N170.048 (9)0.063 (10)0.055 (9)0.010 (7)0.000 (7)0.013 (8)
N180.085 (11)0.112 (12)0.076 (11)0.066 (9)0.005 (8)0.010 (9)
N230.069 (15)0.061 (14)0.051 (12)0.001 (11)0.008 (11)0.019 (10)
N140.133 (12)0.131 (12)0.131 (12)0.065 (6)0.001 (3)0.000 (3)
N240.114 (13)0.100 (13)0.097 (13)0.051 (9)0.004 (9)0.008 (9)
N270.083 (12)0.116 (13)0.086 (12)0.040 (9)0.004 (9)0.005 (9)
N130.098 (12)0.069 (10)0.067 (10)0.016 (8)0.001 (9)0.002 (8)
C70.051 (7)0.061 (8)0.055 (8)0.033 (5)0.000 (5)0.001 (5)
C50.023 (9)0.047 (12)0.026 (9)0.020 (9)0.011 (7)0.001 (8)
C80.09 (2)0.16 (3)0.034 (12)0.10 (2)0.012 (12)0.029 (15)
C40.10 (2)0.12 (2)0.029 (12)0.09 (2)0.029 (13)0.023 (14)
N150.040 (11)0.090 (16)0.056 (12)0.010 (11)0.014 (9)0.045 (12)
Geometric parameters (Å, º) top
Se1—C11.83 (2)N11—H11B0.8600
Se2—C21.81 (3)N12—H12A0.8600
Se3—C31.86 (2)N12—H12B0.8600
Se4—C41.93 (3)N28—H28A0.8600
Se5—C51.835 (18)N28—H28B0.8600
Se6—C61.876 (19)N28—C81.32 (3)
Se7—C71.87 (2)N25—H25A0.8600
Se8—C81.80 (2)N25—H25B0.8600
Se9—C91.94 (3)N25—C51.41 (2)
C6—N161.30 (3)N17—H17A0.8600
C6—N261.31 (3)N17—H17B0.8600
C2—N211.27 (4)N17—C71.29 (3)
C2—N221.42 (4)N18—H18A0.8600
C9—N191.20 (3)N18—H18B0.8600
C9—N291.21 (3)N18—C81.39 (3)
C3—N231.33 (3)N23—H23A0.8600
C3—N131.33 (3)N23—H23B0.8600
C1—N111.35 (2)N14—H14A0.8600
C1—N121.31 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.30 (4)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.27 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.30 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.29 (2)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6122.0 (15)C8—N28—H28B120.0
N16—C6—N26120.1 (19)H25A—N25—H25B120.0
N26—C6—Se6117.8 (15)C5—N25—H25A120.0
N21—C2—Se2128 (3)C5—N25—H25B120.0
N21—C2—N22114 (3)H17A—N17—H17B120.0
N22—C2—Se2116 (2)C7—N17—H17A120.0
N19—C9—Se9119 (2)C7—N17—H17B120.0
N19—C9—N29122 (3)H18A—N18—H18B120.0
N29—C9—Se9118 (2)C8—N18—H18A120.0
N23—C3—Se3121.0 (16)C8—N18—H18B120.0
N13—C3—Se3121.6 (18)C3—N23—H23A120.0
N13—C3—N23117 (2)C3—N23—H23B120.0
N11—C1—Se1121.2 (15)H23A—N23—H23B120.0
N12—C1—Se1122.9 (14)H14A—N14—H14B120.0
N12—C1—N11115.9 (18)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7119.7 (19)
H29A—N29—H29B120.0N17—C7—N27121 (3)
C2—N22—H22A120.0N27—C7—Se7119 (2)
C2—N22—H22B120.0N25—C5—Se5117.6 (14)
H22A—N22—H22B120.0N15—C5—Se5125.8 (14)
C6—N26—H26A120.0N15—C5—N25116.2 (17)
C6—N26—H26B120.0N28—C8—Se8125.0 (19)
H26A—N26—H26B120.0N28—C8—N18116 (2)
C1—N11—H11A120.0N18—C8—Se8118.2 (18)
C1—N11—H11B120.0N14—C4—Se4117 (2)
H11A—N11—H11B120.0N24—C4—Se4116 (2)
C1—N12—H12A120.0N24—C4—N14127 (3)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_343K) top
Crystal data top
CH4N2SeDx = 2.082 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3181 reflections
a = 15.3269 (7) Åθ = 4.1–25.9°
c = 13.0553 (5) ŵ = 9.34 mm1
V = 2655.99 (3) Å3T = 343 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8276 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5485 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.597, Tmax = 1.000l = 1717
28565 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0071P)2 + 37.1154P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.078(Δ/σ)max < 0.001
wR(F2) = 0.139Δρmax = 1.37 e Å3
S = 1.06Δρmin = 1.65 e Å3
8276 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00064 (4)
75 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30538 (18)0.35148 (17)0.09639 (16)0.0409 (5)
Se20.39240 (19)0.36049 (19)0.75586 (17)0.0425 (6)
Se30.30475 (18)0.27110 (17)0.42829 (18)0.0403 (5)
Se40.6315 (2)0.6082 (2)0.70829 (16)0.0485 (7)
Se50.72138 (18)0.69267 (19)0.04962 (19)0.0442 (6)
Se60.63445 (18)0.7013 (2)0.38280 (16)0.0407 (5)
Se70.73181 (18)0.3736 (2)0.46903 (18)0.0566 (8)
Se80.29944 (19)0.70143 (18)0.6671 (2)0.0490 (7)
Se91.06962 (19)1.0322 (2)0.46571 (19)0.0578 (7)
C60.7431 (16)0.6772 (17)0.3872 (16)0.046 (5)
C20.258 (2)0.3173 (17)0.761 (2)0.076 (8)
C90.927 (2)0.9877 (18)0.4618 (18)0.060 (7)
C30.4095 (17)0.4019 (16)0.4191 (16)0.048 (5)
C10.3828 (16)0.2889 (18)0.0943 (14)0.041 (5)
N160.8000 (13)0.6904 (15)0.3092 (13)0.058 (5)
H16A0.8519830.6833590.3155310.069*
H16B0.7859370.7062580.2507340.069*
N210.2061 (19)0.3101 (18)0.8387 (18)0.089 (7)
H21A0.1420500.2845920.8328890.107*
H21B0.2345890.3307060.8974320.107*
N190.8875 (17)0.998 (2)0.5369 (18)0.097 (9)
H19A0.8284670.9910890.5327990.116*
H19B0.9182761.0114280.5948390.116*
N290.8866 (17)0.9684 (18)0.3788 (17)0.082 (7)
H29A0.8275630.9612780.3720150.098*
H29B0.9169370.9617110.3266060.098*
N220.203 (2)0.281 (2)0.668 (2)0.122 (10)
H22A0.1392090.2562650.6676940.147*
H22B0.2345900.2837220.6124720.147*
N260.7640 (15)0.6531 (16)0.4761 (15)0.065 (5)
H26A0.8159240.6460230.4827450.078*
H26B0.7258770.6444000.5279130.078*
N110.4334 (13)0.2924 (13)0.0089 (12)0.046 (4)
H11A0.4685000.2628210.0073290.055*
H11B0.4305740.3241380.0441320.055*
N120.3888 (17)0.2406 (18)0.1723 (12)0.076 (7)
H12A0.4243860.2116570.1688920.091*
H12B0.3570640.2373440.2278700.091*
N280.3913 (17)0.6025 (16)0.7555 (17)0.073 (6)
H28A0.4316290.5788810.7519680.087*
H28B0.3614240.5995650.8122490.087*
N250.5306 (12)0.6224 (15)0.1301 (13)0.060 (6)
H25A0.4660400.5949620.1280440.071*
H25B0.5625200.6503010.1857200.071*
N170.5432 (16)0.2471 (16)0.3893 (17)0.070 (6)
H17A0.4783810.2143270.3876930.084*
H17B0.5769240.2524400.3347000.084*
N180.4286 (17)0.6435 (19)0.5858 (18)0.085 (7)
H18A0.4674630.6181110.5893650.102*
H18B0.4227550.6685750.5290040.102*
N230.4708 (16)0.4478 (16)0.4974 (15)0.080 (7)
H23A0.5196980.5086210.4908660.096*
H23B0.4616760.4166460.5546930.096*
N140.682 (2)0.799 (2)0.643 (2)0.127 (11)
H14A0.7097550.8633580.6447940.152*
H14B0.6487730.7663800.5892860.152*
N240.741 (2)0.794 (2)0.802 (2)0.111 (9)
H24A0.7696840.8580170.8084700.133*
H24B0.7442300.7575970.8502960.133*
N270.543 (2)0.282 (2)0.556 (2)0.107 (9)
H27A0.4779260.2503030.5579600.129*
H27B0.5769380.3109930.6100340.129*
N130.4288 (19)0.4556 (18)0.3322 (17)0.089 (7)
H13A0.4786850.5162410.3295160.107*
H13B0.3912690.4291950.2792150.107*
C70.588 (2)0.287 (3)0.4712 (18)0.078 (10)
C50.5831 (14)0.6217 (15)0.0438 (14)0.037 (4)
C80.3749 (16)0.6440 (17)0.6724 (18)0.083 (10)
C40.692 (2)0.751 (2)0.7186 (16)0.070 (9)
N150.5305 (15)0.5786 (17)0.0368 (15)0.077 (7)
H15A0.4660880.5521650.0353650.092*
H15B0.5598570.5763900.0921220.092*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0455 (14)0.0395 (12)0.0402 (11)0.0230 (11)0.0044 (10)0.0028 (10)
Se20.0363 (13)0.0463 (13)0.0453 (13)0.0211 (11)0.0038 (10)0.0014 (10)
Se30.0422 (13)0.0325 (11)0.0405 (10)0.0142 (11)0.0037 (10)0.0007 (10)
Se40.0497 (14)0.0428 (14)0.0488 (15)0.0200 (12)0.0048 (11)0.0037 (10)
Se50.0389 (13)0.0474 (13)0.0477 (13)0.0226 (11)0.0031 (10)0.0058 (10)
Se60.0438 (13)0.0464 (13)0.0409 (12)0.0293 (11)0.0009 (10)0.0019 (9)
Se70.0396 (14)0.0516 (15)0.0557 (16)0.0054 (11)0.0010 (11)0.0084 (11)
Se80.0607 (16)0.0494 (14)0.0494 (14)0.0368 (13)0.0066 (11)0.0046 (11)
Se90.0435 (14)0.0611 (17)0.0623 (16)0.0213 (13)0.0007 (12)0.0060 (12)
C60.039 (11)0.065 (15)0.052 (13)0.039 (12)0.004 (9)0.008 (11)
C20.078 (9)0.078 (9)0.074 (9)0.040 (6)0.000 (5)0.004 (5)
C90.09 (2)0.049 (14)0.048 (14)0.039 (15)0.007 (13)0.013 (11)
C30.058 (14)0.039 (12)0.035 (10)0.015 (10)0.002 (10)0.004 (9)
C10.035 (11)0.065 (15)0.029 (10)0.029 (11)0.016 (8)0.000 (9)
N160.048 (11)0.104 (16)0.048 (11)0.058 (12)0.006 (9)0.013 (10)
N210.074 (10)0.112 (12)0.074 (10)0.041 (9)0.007 (8)0.001 (9)
N190.073 (16)0.17 (3)0.072 (16)0.077 (18)0.023 (13)0.046 (17)
N290.067 (10)0.097 (11)0.068 (10)0.031 (8)0.016 (8)0.000 (8)
N220.110 (13)0.147 (14)0.115 (14)0.068 (10)0.003 (10)0.006 (10)
N260.063 (9)0.092 (10)0.068 (10)0.058 (8)0.000 (7)0.006 (8)
N110.057 (11)0.062 (12)0.031 (9)0.039 (10)0.001 (8)0.006 (8)
N120.111 (18)0.15 (2)0.019 (8)0.108 (18)0.011 (10)0.018 (11)
N280.085 (10)0.086 (10)0.062 (9)0.054 (8)0.008 (8)0.010 (8)
N250.020 (8)0.100 (16)0.045 (10)0.020 (9)0.010 (7)0.015 (10)
N170.053 (9)0.073 (10)0.061 (9)0.016 (7)0.000 (8)0.013 (8)
N180.088 (11)0.114 (11)0.078 (11)0.069 (9)0.006 (8)0.009 (8)
N230.073 (15)0.059 (13)0.055 (12)0.005 (11)0.007 (11)0.022 (10)
N140.141 (14)0.111 (14)0.115 (14)0.052 (10)0.011 (10)0.004 (10)
N240.122 (13)0.103 (13)0.103 (13)0.053 (10)0.005 (9)0.008 (9)
N270.094 (12)0.123 (13)0.093 (12)0.045 (9)0.006 (9)0.002 (9)
N130.097 (11)0.071 (10)0.066 (10)0.016 (8)0.003 (9)0.000 (8)
C70.10 (2)0.17 (3)0.039 (13)0.12 (2)0.005 (13)0.000 (16)
C50.031 (10)0.048 (12)0.030 (9)0.018 (9)0.012 (8)0.001 (9)
C80.11 (2)0.17 (3)0.043 (13)0.12 (2)0.015 (13)0.028 (16)
C40.10 (2)0.12 (2)0.030 (12)0.08 (2)0.027 (13)0.016 (13)
N150.048 (12)0.094 (17)0.054 (12)0.010 (12)0.014 (10)0.042 (12)
Geometric parameters (Å, º) top
Se1—C11.86 (2)N11—H11B0.8600
Se2—C21.82 (3)N12—H12A0.8600
Se3—C31.84 (2)N12—H12B0.8600
Se4—C41.91 (3)N28—H28A0.8600
Se5—C51.837 (19)N28—H28B0.8600
Se6—C61.878 (19)N28—C81.34 (3)
Se7—C71.92 (3)N25—H25A0.8600
Se8—C81.77 (2)N25—H25B0.8600
Se9—C91.94 (3)N25—C51.39 (2)
C6—N161.29 (3)N17—H17A0.8600
C6—N261.30 (3)N17—H17B0.8600
C2—N211.26 (3)N17—C71.26 (3)
C2—N221.42 (4)N18—H18A0.8600
C9—N191.20 (3)N18—H18B0.8600
C9—N291.21 (3)N18—C81.40 (3)
C3—N231.33 (3)N23—H23A0.8600
C3—N131.34 (3)N23—H23B0.8600
C1—N111.34 (2)N14—H14A0.8600
C1—N121.29 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.28 (3)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.30 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.29 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.29 (3)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6122.8 (15)C8—N28—H28B120.0
N16—C6—N26120.3 (19)H25A—N25—H25B120.0
N26—C6—Se6116.8 (16)C5—N25—H25A120.0
N21—C2—Se2128 (2)C5—N25—H25B120.0
N21—C2—N22115 (3)H17A—N17—H17B120.0
N22—C2—Se2116 (2)C7—N17—H17A120.0
N19—C9—Se9119 (2)C7—N17—H17B120.0
N19—C9—N29122 (3)H18A—N18—H18B120.0
N29—C9—Se9117 (2)C8—N18—H18A120.0
N23—C3—Se3121.8 (17)C8—N18—H18B120.0
N23—C3—N13116 (2)C3—N23—H23A120.0
N13—C3—Se3121.7 (17)C3—N23—H23B120.0
N11—C1—Se1119.7 (15)H23A—N23—H23B120.0
N12—C1—Se1122.0 (14)H14A—N14—H14B120.0
N12—C1—N11118.3 (19)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7119.2 (19)
H29A—N29—H29B120.0N17—C7—N27123 (3)
C2—N22—H22A120.0N27—C7—Se7117 (2)
C2—N22—H22B120.0N25—C5—Se5117.6 (14)
H22A—N22—H22B120.0N15—C5—Se5125.3 (15)
C6—N26—H26A120.0N15—C5—N25116.7 (18)
C6—N26—H26B120.0N28—C8—Se8126.2 (19)
H26A—N26—H26B120.0N28—C8—N18114 (2)
C1—N11—H11A120.0N18—C8—Se8120.2 (18)
C1—N11—H11B120.0N14—C4—Se4118 (2)
H11A—N11—H11B120.0N14—C4—N24124 (3)
C1—N12—H12A120.0N24—C4—Se4118 (2)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_353K) top
Crystal data top
CH4N2SeDx = 2.077 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3095 reflections
a = 15.3389 (7) Åθ = 4.0–25.8°
c = 13.0642 (6) ŵ = 9.32 mm1
V = 2662.0 (3) Å3T = 353 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8281 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5333 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.043
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.340, Tmax = 0.628l = 1717
28618 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0138P)2 + 32.3626P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.076(Δ/σ)max < 0.001
wR(F2) = 0.145Δρmax = 1.27 e Å3
S = 1.05Δρmin = 1.49 e Å3
8281 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00066 (5)
61 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30519 (18)0.35152 (17)0.09625 (16)0.0424 (5)
Se20.39231 (19)0.36053 (19)0.75577 (17)0.0450 (6)
Se30.30503 (17)0.27123 (16)0.42827 (17)0.0423 (5)
Se40.6315 (2)0.6084 (2)0.70836 (16)0.0500 (7)
Se50.72141 (18)0.69250 (19)0.04920 (19)0.0468 (6)
Se60.63476 (18)0.7013 (2)0.38302 (15)0.0425 (5)
Se70.73220 (18)0.37340 (19)0.46866 (18)0.0593 (8)
Se80.29918 (18)0.70140 (17)0.6675 (2)0.0512 (7)
Se91.06954 (18)1.0325 (2)0.46576 (19)0.0598 (7)
C60.7430 (16)0.6762 (17)0.3871 (16)0.048 (5)
C20.258 (3)0.319 (3)0.7625 (19)0.095 (11)
C90.927 (2)0.9883 (18)0.4594 (19)0.063 (7)
C30.4080 (16)0.4014 (15)0.4191 (15)0.048 (5)
C10.3817 (16)0.2868 (18)0.0954 (14)0.045 (5)
N160.7993 (13)0.6898 (15)0.3100 (13)0.059 (5)
H16A0.8514070.6830400.3162480.071*
H16B0.7851370.7057180.2517090.071*
N210.2050 (18)0.3091 (18)0.8400 (17)0.090 (7)
H21A0.1405180.2790660.8347320.108*
H21B0.2332920.3323110.8982650.108*
N190.8880 (16)0.997 (2)0.5372 (18)0.095 (8)
H19A0.8284450.9885690.5350230.115*
H19B0.9201011.0102740.5942890.115*
N290.8863 (18)0.9695 (19)0.3793 (19)0.093 (8)
H29A0.8266230.9610340.3740610.111*
H29B0.9162380.9642660.3259550.111*
N220.201 (2)0.277 (2)0.669 (2)0.133 (11)
H22A0.1368290.2479270.6702510.160*
H22B0.2324480.2808670.6133090.160*
N260.7630 (16)0.6522 (19)0.4758 (14)0.073 (6)
H26A0.8148700.6451840.4831010.087*
H26B0.7243620.6432680.5271630.087*
N110.4327 (13)0.2927 (13)0.0082 (11)0.048 (4)
H11A0.4692340.2647940.0052730.058*
H11B0.4283500.3244020.0441050.058*
N120.3883 (17)0.2405 (18)0.1713 (13)0.085 (8)
H12A0.4249580.2127070.1680300.102*
H12B0.3561830.2365780.2266040.102*
N280.3943 (17)0.6057 (16)0.7574 (17)0.075 (6)
H28A0.4416340.5911300.7556540.090*
H28B0.3616820.5983690.8132560.090*
N250.5304 (12)0.6229 (15)0.1302 (13)0.066 (6)
H25A0.4659800.5961160.1291670.079*
H25B0.5634500.6515460.1849860.079*
N170.5442 (15)0.2486 (16)0.3873 (16)0.075 (6)
H17A0.4794750.2173940.3850610.089*
H17B0.5781120.2531700.3332130.089*
N180.4314 (17)0.6472 (18)0.5886 (17)0.087 (7)
H18A0.4770600.6306420.5950660.104*
H18B0.4227670.6683260.5305790.104*
N230.4703 (16)0.4485 (16)0.4975 (15)0.084 (7)
H23A0.5187900.5093830.4904250.101*
H23B0.4617280.4178760.5549730.101*
N140.685 (2)0.801 (2)0.641 (2)0.135 (11)
H14A0.7144190.8651520.6438170.161*
H14B0.6508090.7695330.5872210.161*
N240.741 (2)0.793 (2)0.802 (2)0.114 (9)
H24A0.7712520.8575820.8064330.137*
H24B0.7435760.7579210.8517600.137*
N270.542 (2)0.283 (2)0.5547 (19)0.108 (9)
H27A0.4775400.2527530.5556010.129*
H27B0.5758190.3108500.6094850.129*
N130.4285 (19)0.4562 (18)0.3336 (17)0.097 (8)
H13A0.4784570.5168580.3322060.117*
H13B0.3916810.4308960.2800880.117*
C70.589 (2)0.288 (3)0.4702 (17)0.077 (9)
C50.5812 (13)0.6200 (15)0.0431 (15)0.037 (4)
C80.371 (2)0.640 (2)0.6726 (17)0.075 (8)
C40.690 (2)0.748 (2)0.7195 (18)0.074 (8)
N150.5299 (13)0.5773 (16)0.0357 (14)0.075 (7)
H15A0.4655170.5511270.0345080.090*
H15B0.5592690.5743990.0905840.090*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0472 (14)0.0419 (12)0.0412 (11)0.0247 (11)0.0035 (9)0.0026 (10)
Se20.0391 (13)0.0474 (13)0.0489 (13)0.0220 (11)0.0037 (10)0.0008 (10)
Se30.0441 (13)0.0342 (11)0.0422 (10)0.0148 (11)0.0034 (10)0.0001 (10)
Se40.0517 (14)0.0439 (14)0.0502 (15)0.0209 (12)0.0052 (11)0.0042 (10)
Se50.0401 (13)0.0504 (14)0.0512 (13)0.0235 (11)0.0023 (10)0.0064 (10)
Se60.0451 (13)0.0488 (13)0.0423 (12)0.0301 (11)0.0004 (10)0.0017 (9)
Se70.0417 (14)0.0553 (15)0.0576 (16)0.0066 (11)0.0008 (11)0.0068 (11)
Se80.0616 (16)0.0508 (14)0.0531 (14)0.0372 (12)0.0064 (11)0.0044 (11)
Se90.0441 (14)0.0631 (17)0.0651 (16)0.0215 (13)0.0007 (12)0.0069 (12)
C60.041 (11)0.069 (15)0.054 (13)0.042 (12)0.007 (10)0.011 (11)
C20.13 (3)0.14 (3)0.040 (14)0.09 (2)0.027 (16)0.043 (17)
C90.09 (2)0.051 (14)0.055 (15)0.043 (15)0.001 (14)0.013 (12)
C30.049 (13)0.036 (11)0.037 (10)0.005 (10)0.003 (9)0.000 (9)
C10.040 (12)0.066 (15)0.026 (10)0.024 (11)0.017 (8)0.004 (9)
N160.048 (11)0.104 (16)0.050 (10)0.057 (12)0.003 (9)0.002 (10)
N210.077 (10)0.114 (12)0.072 (10)0.042 (8)0.008 (8)0.003 (9)
N190.066 (15)0.15 (3)0.087 (17)0.070 (17)0.033 (13)0.046 (17)
N290.076 (11)0.108 (12)0.085 (11)0.039 (9)0.017 (9)0.001 (9)
N220.124 (14)0.153 (15)0.124 (14)0.070 (10)0.002 (10)0.006 (10)
N260.070 (9)0.101 (10)0.076 (10)0.065 (8)0.003 (7)0.007 (8)
N110.060 (11)0.063 (11)0.035 (9)0.041 (10)0.006 (8)0.011 (8)
N120.114 (19)0.17 (2)0.026 (9)0.109 (18)0.015 (10)0.028 (12)
N280.086 (10)0.087 (10)0.062 (9)0.052 (8)0.011 (8)0.011 (8)
N250.016 (8)0.102 (16)0.057 (11)0.013 (9)0.015 (8)0.018 (11)
N170.057 (9)0.079 (10)0.061 (9)0.013 (7)0.004 (8)0.016 (8)
N180.090 (11)0.113 (11)0.077 (10)0.066 (9)0.005 (8)0.013 (8)
N230.077 (15)0.063 (14)0.062 (13)0.002 (12)0.008 (11)0.017 (10)
N140.150 (14)0.117 (14)0.123 (14)0.056 (10)0.008 (10)0.005 (10)
N240.126 (13)0.108 (13)0.103 (13)0.053 (9)0.004 (9)0.009 (9)
N270.092 (12)0.124 (13)0.093 (12)0.043 (9)0.002 (9)0.004 (9)
N130.102 (12)0.080 (11)0.077 (11)0.022 (8)0.003 (9)0.002 (9)
C70.081 (18)0.16 (3)0.042 (13)0.10 (2)0.002 (12)0.011 (15)
C50.028 (9)0.048 (12)0.041 (10)0.023 (9)0.008 (8)0.007 (9)
C80.094 (19)0.15 (3)0.041 (12)0.10 (2)0.012 (12)0.024 (14)
C40.11 (2)0.09 (2)0.042 (14)0.067 (19)0.010 (14)0.005 (13)
N150.038 (10)0.100 (16)0.053 (12)0.009 (11)0.013 (9)0.036 (11)
Geometric parameters (Å, º) top
Se1—C11.88 (2)N11—H11B0.8600
Se2—C21.83 (3)N12—H12A0.8600
Se3—C31.828 (19)N12—H12B0.8600
Se4—C41.87 (3)N28—H28A0.8600
Se5—C51.864 (18)N28—H28B0.8600
Se6—C61.882 (18)N28—C81.35 (3)
Se7—C71.91 (3)N25—H25A0.8600
Se8—C81.78 (2)N25—H25B0.8600
Se9—C91.94 (3)N25—C51.39 (2)
C6—N161.27 (2)N17—H17A0.8600
C6—N261.30 (2)N17—H17B0.8600
C2—N211.26 (3)N17—C71.26 (3)
C2—N221.44 (4)N18—H18A0.8600
C9—N191.22 (3)N18—H18B0.8600
C9—N291.18 (3)N18—C81.40 (3)
C3—N231.34 (3)N23—H23A0.8600
C3—N131.34 (3)N23—H23B0.8600
C1—N111.36 (2)N14—H14A0.8600
C1—N121.25 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.33 (3)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.30 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.30 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.26 (2)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6122.6 (15)C8—N28—H28B120.0
N16—C6—N26121.0 (18)H25A—N25—H25B120.0
N26—C6—Se6116.2 (15)C5—N25—H25A120.0
N21—C2—Se2129 (2)C5—N25—H25B120.0
N21—C2—N22115 (3)H17A—N17—H17B120.0
N22—C2—Se2116 (2)C7—N17—H17A120.0
N19—C9—Se9117 (2)C7—N17—H17B120.0
N29—C9—Se9119 (2)H18A—N18—H18B120.0
N29—C9—N19123 (3)C8—N18—H18A120.0
N23—C3—Se3122.2 (16)C8—N18—H18B120.0
N13—C3—Se3123.0 (17)C3—N23—H23A120.0
N13—C3—N23115 (2)C3—N23—H23B120.0
N11—C1—Se1117.4 (15)H23A—N23—H23B120.0
N12—C1—Se1122.9 (15)H14A—N14—H14B120.0
N12—C1—N11120 (2)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7119.0 (19)
H29A—N29—H29B120.0N17—C7—N27123 (3)
C2—N22—H22A120.0N27—C7—Se7117 (2)
C2—N22—H22B120.0N25—C5—Se5116.3 (14)
H22A—N22—H22B120.0N15—C5—Se5125.3 (15)
C6—N26—H26A120.0N15—C5—N25118.0 (17)
C6—N26—H26B120.0N28—C8—Se8126.3 (18)
H26A—N26—H26B120.0N28—C8—N18113 (2)
C1—N11—H11A120.0N18—C8—Se8119.2 (17)
C1—N11—H11B120.0N14—C4—Se4119 (2)
H11A—N11—H11B120.0N24—C4—Se4119 (2)
C1—N12—H12A120.0N24—C4—N14122 (3)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_363K) top
Crystal data top
CH4N2SeDx = 2.073 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 3032 reflections
a = 15.3505 (7) Åθ = 4.0–25.0°
c = 13.0706 (6) ŵ = 9.30 mm1
V = 2667.3 (3) Å3T = 363 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8308 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source5097 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.044
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.341, Tmax = 0.628l = 1717
28681 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0234P)2 + 30.3829P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.075(Δ/σ)max < 0.001
wR(F2) = 0.158Δρmax = 1.24 e Å3
S = 1.04Δρmin = 1.49 e Å3
8308 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00066 (6)
74 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30541 (18)0.35177 (17)0.09620 (16)0.0441 (5)
Se20.39192 (18)0.36061 (19)0.75568 (16)0.0462 (6)
Se30.30515 (17)0.27170 (17)0.42827 (17)0.0440 (5)
Se40.6315 (2)0.6083 (2)0.70831 (16)0.0517 (7)
Se50.72151 (18)0.69260 (19)0.04925 (19)0.0488 (6)
Se60.63483 (18)0.7015 (2)0.38288 (15)0.0447 (6)
Se70.73238 (18)0.37327 (19)0.46856 (18)0.0602 (8)
Se80.29926 (18)0.70166 (18)0.6681 (2)0.0541 (7)
Se91.06947 (18)1.0326 (2)0.46569 (19)0.0621 (7)
C60.7412 (16)0.6750 (17)0.3864 (16)0.051 (5)
C20.256 (2)0.317 (2)0.762 (2)0.080 (8)
C90.927 (2)0.9884 (18)0.4593 (18)0.063 (7)
C30.4088 (16)0.4028 (15)0.4190 (16)0.050 (5)
C10.3827 (17)0.2879 (18)0.0943 (14)0.047 (5)
N160.7993 (14)0.6882 (15)0.3098 (13)0.062 (5)
H16A0.8507360.6806380.3174340.075*
H16B0.7866000.7045920.2510750.075*
N210.2054 (18)0.3085 (18)0.8391 (17)0.091 (7)
H21A0.1409940.2802100.8347250.110*
H21B0.2347300.3309560.8969950.110*
N190.8879 (17)0.997 (2)0.5357 (19)0.099 (8)
H19A0.8282880.9891500.5328910.118*
H19B0.9196441.0115890.5929680.118*
N290.8865 (18)0.9690 (19)0.3798 (19)0.097 (8)
H29A0.8268450.9604270.3743930.116*
H29B0.9164110.9632590.3268370.116*
N220.202 (2)0.278 (2)0.668 (2)0.138 (11)
H22A0.1373800.2499330.6670560.165*
H22B0.2339970.2819120.6126210.165*
N260.7613 (15)0.6499 (16)0.4760 (15)0.073 (6)
H26A0.8129560.6424790.4830280.087*
H26B0.7228750.6409550.5275400.087*
N110.4330 (13)0.2922 (14)0.0083 (11)0.054 (5)
H11A0.4685810.2633030.0060030.064*
H11B0.4294240.3238910.0443670.064*
N120.3887 (17)0.2410 (19)0.1710 (13)0.089 (8)
H12A0.4245430.2123920.1678610.107*
H12B0.3569060.2377690.2263600.107*
N280.3897 (18)0.6022 (17)0.7574 (18)0.083 (6)
H28A0.4306670.5794360.7544890.099*
H28B0.3583790.5978850.8134050.099*
N250.5304 (12)0.6228 (15)0.1308 (13)0.065 (6)
H25A0.4660780.5960080.1289390.079*
H25B0.5627590.6507510.1860510.079*
N170.5443 (15)0.2508 (15)0.3863 (16)0.073 (6)
H17A0.4796360.2190020.3841770.088*
H17B0.5782130.2559560.3319720.088*
N180.4305 (17)0.6466 (18)0.5882 (17)0.089 (7)
H18A0.4698640.6219680.5922130.107*
H18B0.4254230.6723460.5315930.107*
N230.4687 (16)0.4486 (16)0.4974 (15)0.091 (8)
H23A0.5171520.5096120.4912160.109*
H23B0.4592240.4175690.5546830.109*
N140.686 (2)0.799 (3)0.641 (2)0.146 (12)
H14A0.7169300.8635050.6418300.175*
H14B0.6519600.7668610.5875780.175*
N240.741 (2)0.792 (2)0.8028 (19)0.110 (9)
H24A0.7732280.8569360.8077570.132*
H24B0.7419010.7563300.8527070.132*
N270.543 (2)0.285 (2)0.5553 (19)0.112 (9)
H27A0.4781690.2538110.5559730.135*
H27B0.5759980.3124400.6103510.135*
N130.4295 (19)0.4571 (18)0.3335 (17)0.100 (8)
H13A0.4790790.5178170.3320980.120*
H13B0.3931240.4313510.2797900.120*
C70.5905 (18)0.291 (2)0.4711 (17)0.069 (8)
C50.5823 (14)0.6209 (16)0.0443 (14)0.041 (5)
C80.3744 (16)0.6447 (17)0.6739 (18)0.090 (10)
C40.691 (2)0.749 (2)0.7195 (17)0.076 (9)
N150.5307 (14)0.5784 (17)0.0361 (15)0.085 (7)
H15A0.4664250.5523520.0352540.102*
H15B0.5604030.5759180.0908840.102*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0489 (14)0.0440 (13)0.0433 (11)0.0263 (11)0.0029 (10)0.0034 (10)
Se20.0394 (13)0.0501 (14)0.0493 (13)0.0225 (11)0.0036 (10)0.0010 (10)
Se30.0457 (13)0.0370 (12)0.0427 (11)0.0159 (11)0.0036 (10)0.0005 (10)
Se40.0534 (14)0.0456 (14)0.0513 (15)0.0211 (12)0.0053 (11)0.0041 (10)
Se50.0424 (13)0.0516 (14)0.0532 (13)0.0241 (11)0.0016 (10)0.0050 (10)
Se60.0483 (13)0.0499 (13)0.0462 (13)0.0323 (11)0.0005 (10)0.0024 (10)
Se70.0426 (14)0.0557 (15)0.0598 (16)0.0076 (11)0.0003 (11)0.0066 (11)
Se80.0649 (16)0.0537 (14)0.0568 (15)0.0394 (13)0.0071 (12)0.0056 (11)
Se90.0457 (14)0.0659 (17)0.0665 (16)0.0218 (13)0.0003 (12)0.0073 (12)
C60.054 (13)0.076 (16)0.048 (12)0.051 (13)0.006 (10)0.011 (11)
C20.081 (9)0.084 (9)0.077 (9)0.042 (6)0.000 (5)0.005 (5)
C90.10 (2)0.058 (15)0.043 (13)0.052 (16)0.002 (13)0.005 (11)
C30.055 (13)0.033 (11)0.042 (11)0.008 (10)0.000 (10)0.007 (9)
C10.049 (13)0.067 (15)0.025 (10)0.030 (12)0.016 (9)0.004 (9)
N160.058 (12)0.106 (16)0.045 (10)0.058 (12)0.004 (9)0.006 (10)
N210.074 (10)0.116 (12)0.074 (10)0.040 (8)0.010 (8)0.001 (9)
N190.075 (16)0.15 (2)0.086 (17)0.066 (17)0.031 (13)0.042 (16)
N290.083 (11)0.112 (12)0.087 (11)0.042 (9)0.014 (9)0.002 (9)
N220.127 (14)0.161 (15)0.128 (14)0.074 (10)0.001 (10)0.007 (10)
N260.070 (9)0.101 (10)0.076 (10)0.065 (8)0.003 (7)0.007 (8)
N110.066 (12)0.077 (13)0.034 (9)0.047 (11)0.006 (8)0.015 (8)
N120.13 (2)0.17 (2)0.034 (10)0.12 (2)0.010 (11)0.018 (13)
N280.095 (11)0.093 (11)0.072 (10)0.055 (8)0.009 (8)0.012 (8)
N250.024 (8)0.097 (15)0.060 (12)0.018 (9)0.007 (8)0.019 (11)
N170.054 (9)0.079 (10)0.062 (9)0.016 (7)0.002 (7)0.017 (8)
N180.092 (11)0.117 (11)0.081 (10)0.070 (9)0.005 (8)0.011 (8)
N230.076 (15)0.073 (15)0.060 (13)0.010 (12)0.012 (11)0.021 (11)
N140.158 (15)0.129 (15)0.137 (15)0.063 (10)0.006 (10)0.003 (10)
N240.121 (12)0.101 (12)0.099 (12)0.050 (9)0.005 (9)0.009 (9)
N270.096 (12)0.129 (13)0.097 (12)0.046 (9)0.001 (9)0.001 (9)
N130.108 (12)0.080 (11)0.078 (11)0.021 (8)0.001 (9)0.005 (9)
C70.056 (14)0.15 (3)0.046 (12)0.080 (17)0.010 (11)0.016 (14)
C50.034 (10)0.055 (13)0.034 (10)0.022 (10)0.010 (8)0.003 (9)
C80.12 (2)0.17 (3)0.046 (14)0.12 (2)0.014 (14)0.020 (16)
C40.11 (2)0.10 (2)0.039 (14)0.07 (2)0.014 (13)0.013 (13)
N150.049 (12)0.102 (17)0.065 (13)0.009 (12)0.018 (10)0.046 (12)
Geometric parameters (Å, º) top
Se1—C11.88 (2)N11—H11B0.8600
Se2—C21.85 (3)N12—H12A0.8600
Se3—C31.842 (19)N12—H12B0.8600
Se4—C41.89 (3)N28—H28A0.8600
Se5—C51.852 (19)N28—H28B0.8600
Se6—C61.869 (19)N28—C81.35 (3)
Se7—C71.89 (2)N25—H25A0.8600
Se8—C81.76 (2)N25—H25B0.8600
Se9—C91.94 (3)N25—C51.39 (2)
C6—N161.29 (2)N17—H17A0.8600
C6—N261.32 (3)N17—H17B0.8600
C2—N211.24 (3)N17—C71.29 (3)
C2—N221.43 (4)N18—H18A0.8600
C9—N191.21 (3)N18—H18B0.8600
C9—N291.17 (3)N18—C81.40 (3)
C3—N231.32 (3)N23—H23A0.8600
C3—N131.33 (3)N23—H23B0.8600
C1—N111.35 (2)N14—H14A0.8600
C1—N121.26 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.31 (4)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.31 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.30 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.28 (2)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6124.0 (15)C8—N28—H28B120.0
N16—C6—N26119.4 (19)H25A—N25—H25B120.0
N26—C6—Se6116.3 (15)C5—N25—H25A120.0
N21—C2—Se2127 (2)C5—N25—H25B120.0
N21—C2—N22117 (3)H17A—N17—H17B120.0
N22—C2—Se2115 (2)C7—N17—H17A120.0
N19—C9—Se9117 (2)C7—N17—H17B120.0
N29—C9—Se9119 (2)H18A—N18—H18B120.0
N29—C9—N19122 (3)C8—N18—H18A120.0
N23—C3—Se3121.5 (16)C8—N18—H18B120.0
N23—C3—N13116 (2)C3—N23—H23A120.0
N13—C3—Se3122.9 (17)C3—N23—H23B120.0
N11—C1—Se1118.7 (15)H23A—N23—H23B120.0
N12—C1—Se1122.1 (15)H14A—N14—H14B120.0
N12—C1—N11119 (2)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7118.5 (18)
H29A—N29—H29B120.0N17—C7—N27122 (2)
C2—N22—H22A120.0N27—C7—Se7119 (2)
C2—N22—H22B120.0N25—C5—Se5117.5 (14)
H22A—N22—H22B120.0N15—C5—Se5124.5 (15)
C6—N26—H26A120.0N15—C5—N25117.6 (18)
C6—N26—H26B120.0N28—C8—Se8126.1 (19)
H26A—N26—H26B120.0N28—C8—N18114 (2)
C1—N11—H11A120.0N18—C8—Se8120.1 (19)
C1—N11—H11B120.0N14—C4—Se4118 (2)
H11A—N11—H11B120.0N14—C4—N24124 (3)
C1—N12—H12A120.0N24—C4—Se4118 (2)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_alpha_Selenourea_373K) top
Crystal data top
CH4N2SeDx = 2.064 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P31Cell parameters from 2933 reflections
a = 15.3619 (8) Åθ = 4.0–24.5°
c = 13.0768 (6) ŵ = 9.26 mm1
V = 2672.5 (3) Å3T = 373 K
Z = 27Plate, orange
F(000) = 15660.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
8325 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source4942 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.045
Detector resolution: 16.1544 pixels mm-1θmax = 29.0°, θmin = 3.1°
ω scansh = 2020
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1919
Tmin = 0.342, Tmax = 0.629l = 1717
28736 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0297P)2 + 28.6035P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.075(Δ/σ)max < 0.001
wR(F2) = 0.167Δρmax = 1.21 e Å3
S = 1.03Δρmin = 1.40 e Å3
8325 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
326 parametersExtinction coefficient: 0.00064 (7)
93 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.30529 (18)0.35184 (17)0.09602 (16)0.0456 (6)
Se20.39180 (19)0.36075 (19)0.75585 (17)0.0478 (6)
Se30.30531 (18)0.27176 (17)0.42809 (18)0.0462 (5)
Se40.6316 (2)0.6082 (2)0.70857 (16)0.0539 (7)
Se50.72160 (18)0.6925 (2)0.04891 (19)0.0515 (6)
Se60.63529 (18)0.7017 (2)0.38309 (15)0.0464 (6)
Se70.73244 (18)0.37281 (19)0.46814 (19)0.0631 (8)
Se80.29910 (19)0.70171 (18)0.6689 (2)0.0570 (7)
Se91.06962 (19)1.0330 (2)0.46573 (19)0.0633 (7)
C60.7413 (16)0.6731 (18)0.3865 (16)0.052 (5)
C20.258 (2)0.317 (2)0.759 (2)0.086 (9)
C90.928 (2)0.9888 (19)0.4607 (19)0.062 (6)
C30.4078 (15)0.4034 (15)0.4183 (15)0.050 (5)
C10.3821 (17)0.2896 (17)0.0939 (14)0.046 (5)
N160.7986 (14)0.6867 (15)0.3102 (13)0.064 (5)
H16A0.8506590.6800770.3174160.077*
H16B0.7852330.7025570.2515310.077*
N210.2033 (17)0.3068 (18)0.8382 (17)0.091 (7)
H21A0.1391060.2781790.8319760.109*
H21B0.2309410.3286390.8969220.109*
N190.8867 (17)0.998 (2)0.5366 (19)0.102 (9)
H19A0.8271260.9896540.5320530.123*
H19B0.9171721.0126170.5945930.123*
N290.8857 (18)0.9686 (19)0.381 (2)0.099 (8)
H29A0.8261820.9603000.3762190.119*
H29B0.9146560.9621520.3272860.119*
N220.202 (2)0.277 (2)0.669 (2)0.120 (9)
H22A0.1377030.2498940.6701200.144*
H22B0.2321390.2804460.6121420.144*
N260.7611 (16)0.6488 (17)0.4767 (16)0.079 (6)
H26A0.8129390.6419970.4845740.095*
H26B0.7220820.6397120.5277320.095*
N110.4327 (13)0.2925 (14)0.0081 (12)0.056 (5)
H11A0.4675530.2627370.0067660.067*
H11B0.4300290.3239690.0450720.067*
N120.3893 (15)0.2411 (16)0.1708 (16)0.075 (6)
H12A0.4249830.2125240.1660930.090*
H12B0.3583190.2374260.2268840.090*
N280.3922 (18)0.6041 (17)0.7576 (18)0.084 (6)
H28A0.4331710.5814530.7528900.101*
H28B0.3627190.6001480.8147420.101*
N250.5305 (13)0.6234 (15)0.1319 (13)0.069 (6)
H25A0.4663050.5978280.1303880.083*
H25B0.5633400.6510260.1869530.083*
N170.5450 (16)0.2494 (16)0.3852 (16)0.082 (6)
H17A0.4803950.2173560.3822960.098*
H17B0.5796220.2550700.3314120.098*
N180.4298 (17)0.6455 (18)0.5895 (17)0.092 (7)
H18A0.4684230.6201640.5951830.111*
H18B0.4252250.6699970.5319210.111*
N230.4687 (17)0.4490 (18)0.4974 (17)0.089 (7)
H23A0.5180530.5093830.4910480.107*
H23B0.4585120.4179660.5547780.107*
N140.684 (2)0.796 (2)0.642 (2)0.143 (11)
H14A0.7124670.8604920.6437630.172*
H14B0.6514760.7636140.5885920.172*
N240.738 (2)0.792 (2)0.8034 (19)0.132 (12)
H24A0.7681840.8564000.8092620.158*
H24B0.7401000.7561870.8529820.158*
N270.543 (2)0.284 (2)0.557 (2)0.120 (9)
H27A0.4782320.2531440.5584860.144*
H27B0.5767580.3122130.6113570.144*
N130.4284 (19)0.4559 (19)0.3328 (18)0.108 (8)
H13A0.4786960.5161480.3304160.129*
H13B0.3913840.4298980.2796120.129*
C70.5900 (17)0.2893 (18)0.4706 (17)0.057 (6)
C50.5820 (14)0.6199 (15)0.0437 (14)0.041 (5)
C80.3741 (16)0.6467 (15)0.6741 (19)0.068 (6)
C40.690 (2)0.749 (2)0.7188 (17)0.079 (9)
N150.5299 (15)0.5780 (17)0.0362 (15)0.089 (8)
H15A0.4657670.5532300.0350270.107*
H15B0.5588230.5746490.0910840.107*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0503 (14)0.0451 (13)0.0460 (12)0.0272 (12)0.0047 (10)0.0018 (10)
Se20.0418 (13)0.0505 (14)0.0512 (13)0.0233 (12)0.0040 (10)0.0008 (10)
Se30.0476 (13)0.0381 (12)0.0462 (11)0.0165 (11)0.0034 (10)0.0006 (11)
Se40.0560 (15)0.0483 (15)0.0530 (16)0.0227 (12)0.0058 (11)0.0041 (10)
Se50.0443 (13)0.0560 (15)0.0550 (13)0.0258 (12)0.0024 (11)0.0065 (11)
Se60.0501 (14)0.0530 (14)0.0468 (13)0.0338 (12)0.0007 (10)0.0003 (10)
Se70.0427 (14)0.0584 (16)0.0652 (17)0.0080 (11)0.0016 (12)0.0067 (12)
Se80.0693 (17)0.0582 (15)0.0585 (15)0.0431 (14)0.0077 (12)0.0059 (11)
Se90.0468 (14)0.0666 (17)0.0685 (16)0.0224 (13)0.0002 (12)0.0066 (12)
C60.040 (12)0.081 (17)0.050 (12)0.042 (12)0.001 (9)0.002 (11)
C20.087 (10)0.088 (10)0.083 (10)0.045 (6)0.000 (5)0.005 (5)
C90.090 (19)0.062 (15)0.056 (14)0.053 (15)0.001 (13)0.010 (12)
C30.043 (12)0.039 (11)0.040 (10)0.000 (9)0.002 (9)0.007 (9)
C10.058 (14)0.064 (14)0.026 (9)0.038 (12)0.018 (9)0.005 (9)
N160.056 (12)0.107 (16)0.041 (10)0.050 (12)0.002 (9)0.007 (10)
N210.073 (10)0.113 (12)0.076 (10)0.038 (8)0.002 (8)0.005 (9)
N190.078 (16)0.15 (3)0.087 (17)0.064 (17)0.030 (13)0.045 (17)
N290.080 (11)0.114 (12)0.091 (12)0.039 (9)0.013 (9)0.004 (9)
N220.106 (13)0.144 (14)0.110 (13)0.064 (10)0.000 (9)0.004 (10)
N260.077 (10)0.105 (11)0.084 (10)0.067 (8)0.001 (8)0.003 (8)
N110.067 (12)0.071 (12)0.040 (9)0.042 (11)0.005 (8)0.009 (9)
N120.080 (10)0.092 (10)0.068 (9)0.055 (8)0.000 (8)0.008 (8)
N280.096 (11)0.095 (11)0.075 (10)0.058 (8)0.008 (8)0.009 (8)
N250.033 (9)0.107 (17)0.052 (11)0.024 (10)0.019 (8)0.007 (11)
N170.066 (10)0.089 (11)0.066 (10)0.021 (8)0.003 (8)0.016 (8)
N180.097 (11)0.118 (11)0.085 (11)0.070 (9)0.003 (8)0.011 (8)
N230.086 (11)0.085 (11)0.074 (10)0.025 (8)0.004 (8)0.011 (8)
N140.157 (15)0.127 (14)0.133 (14)0.061 (10)0.006 (10)0.002 (10)
N240.21 (3)0.10 (2)0.076 (18)0.07 (2)0.01 (2)0.019 (16)
N270.102 (12)0.138 (13)0.110 (13)0.052 (9)0.001 (9)0.001 (10)
N130.114 (12)0.090 (11)0.085 (11)0.026 (9)0.005 (9)0.002 (9)
C70.053 (7)0.065 (7)0.057 (7)0.032 (5)0.001 (5)0.001 (5)
C50.034 (10)0.052 (12)0.033 (9)0.018 (9)0.012 (8)0.003 (9)
C80.068 (8)0.074 (8)0.068 (8)0.040 (6)0.001 (5)0.004 (5)
C40.12 (3)0.12 (2)0.035 (13)0.09 (2)0.016 (14)0.011 (14)
N150.051 (12)0.107 (18)0.067 (13)0.008 (12)0.021 (10)0.046 (12)
Geometric parameters (Å, º) top
Se1—C11.85 (2)N11—H11B0.8600
Se2—C21.81 (3)N12—H12A0.8600
Se3—C31.844 (19)N12—H12B0.8600
Se4—C41.88 (3)N28—H28A0.8600
Se5—C51.859 (18)N28—H28B0.8600
Se6—C61.888 (19)N28—C81.37 (3)
Se7—C71.90 (2)N25—H25A0.8600
Se8—C81.74 (2)N25—H25B0.8600
Se9—C91.93 (3)N25—C51.41 (2)
C6—N161.28 (2)N17—H17A0.8600
C6—N261.32 (3)N17—H17B0.8600
C2—N211.30 (3)N17—C71.29 (3)
C2—N221.41 (4)N18—H18A0.8600
C9—N191.22 (3)N18—H18B0.8600
C9—N291.19 (3)N18—C81.40 (3)
C3—N231.33 (3)N23—H23A0.8600
C3—N131.32 (3)N23—H23B0.8600
C1—N111.35 (2)N14—H14A0.8600
C1—N121.29 (3)N14—H14B0.8600
N16—H16A0.8600N14—C41.27 (3)
N16—H16B0.8600N24—H24A0.8600
N21—H21A0.8600N24—H24B0.8600
N21—H21B0.8600N24—C41.31 (3)
N19—H19A0.8600N27—H27A0.8600
N19—H19B0.8600N27—H27B0.8600
N29—H29A0.8600N27—C71.32 (3)
N29—H29B0.8600N13—H13A0.8600
N22—H22A0.8600N13—H13B0.8600
N22—H22B0.8600C5—N151.28 (2)
N26—H26A0.8600N15—H15A0.8600
N26—H26B0.8600N15—H15B0.8600
N11—H11A0.8600
N16—C6—Se6123.2 (16)C8—N28—H28B120.0
N16—C6—N26120.5 (19)H25A—N25—H25B120.0
N26—C6—Se6115.8 (16)C5—N25—H25A120.0
N21—C2—Se2128 (2)C5—N25—H25B120.0
N21—C2—N22113 (3)H17A—N17—H17B120.0
N22—C2—Se2118 (2)C7—N17—H17A120.0
N19—C9—Se9119 (2)C7—N17—H17B120.0
N29—C9—Se9120 (2)H18A—N18—H18B120.0
N29—C9—N19120 (3)C8—N18—H18A120.0
N23—C3—Se3120.8 (17)C8—N18—H18B120.0
N13—C3—Se3122.7 (18)C3—N23—H23A120.0
N13—C3—N23116 (2)C3—N23—H23B120.0
N11—C1—Se1120.0 (15)H23A—N23—H23B120.0
N12—C1—Se1123.1 (15)H14A—N14—H14B120.0
N12—C1—N11116.9 (19)C4—N14—H14A120.0
C6—N16—H16A120.0C4—N14—H14B120.0
C6—N16—H16B120.0H24A—N24—H24B120.0
H16A—N16—H16B120.0C4—N24—H24A120.0
C2—N21—H21A120.0C4—N24—H24B120.0
C2—N21—H21B120.0H27A—N27—H27B120.0
H21A—N21—H21B120.0C7—N27—H27A120.0
C9—N19—H19A120.0C7—N27—H27B120.0
C9—N19—H19B120.0C3—N13—H13A120.0
H19A—N19—H19B120.0C3—N13—H13B120.0
C9—N29—H29A120.0H13A—N13—H13B120.0
C9—N29—H29B120.0N17—C7—Se7117.8 (18)
H29A—N29—H29B120.0N17—C7—N27124 (2)
C2—N22—H22A120.0N27—C7—Se7117.7 (19)
C2—N22—H22B120.0N25—C5—Se5116.6 (14)
H22A—N22—H22B120.0N15—C5—Se5125.3 (15)
C6—N26—H26A120.0N15—C5—N25117.6 (18)
C6—N26—H26B120.0N28—C8—Se8127 (2)
H26A—N26—H26B120.0N28—C8—N18111 (2)
C1—N11—H11A120.0N18—C8—Se8122 (2)
C1—N11—H11B120.0N14—C4—Se4118 (2)
H11A—N11—H11B120.0N14—C4—N24124 (3)
C1—N12—H12A120.0N24—C4—Se4118 (2)
C1—N12—H12B120.0C5—N15—H15A120.0
H12A—N12—H12B120.0C5—N15—H15B120.0
H28A—N28—H28B120.0H15A—N15—H15B120.0
C8—N28—H28A120.0
Selenourea (phase_gamma_Selenourea_383K) top
Crystal data top
CH4N2SeDx = 2.072 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P3121Cell parameters from 1753 reflections
a = 8.8551 (4) Åθ = 4.1–25.8°
c = 13.0694 (7) ŵ = 9.29 mm1
V = 887.51 (9) Å3T = 383 K
Z = 9Plate, orange
F(000) = 5220.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
1414 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source1204 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 16.1544 pixels mm-1θmax = 28.9°, θmin = 3.1°
ω scansh = 1111
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1111
Tmin = 0.533, Tmax = 1.000l = 1716
6352 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0252P)2 + 0.2031P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.029(Δ/σ)max < 0.001
wR(F2) = 0.059Δρmax = 0.50 e Å3
S = 1.06Δρmin = 0.27 e Å3
1414 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
57 parametersExtinction coefficient: 0.0035 (5)
0 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.0000000.07237 (7)0.6666670.0472 (2)
Se20.44459 (6)0.76440 (7)0.29093 (4)0.0550 (2)
N110.0398 (9)0.1921 (7)0.5830 (4)0.100 (2)
H11A0.0395100.2893930.5835790.120*
H11B0.0659940.1311810.5278970.120*
N220.2111 (8)0.4352 (7)0.2192 (4)0.106 (2)
H22A0.1249590.3303940.2239460.127*
H22B0.2692260.4703930.1630390.127*
C10.0000000.1366 (8)0.6666670.054 (2)
N210.1637 (9)0.4845 (8)0.3811 (4)0.128 (3)
H21A0.0779280.3792260.3846050.154*
H21B0.1900660.5524230.4332110.154*
C20.2537 (8)0.5409 (8)0.2970 (4)0.0657 (17)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0564 (6)0.0425 (3)0.0472 (3)0.0282 (3)0.0021 (4)0.00106 (18)
Se20.0454 (3)0.0467 (3)0.0624 (3)0.0151 (3)0.0002 (2)0.0014 (2)
N110.198 (7)0.074 (4)0.058 (3)0.091 (4)0.028 (4)0.004 (3)
N220.123 (5)0.060 (3)0.069 (3)0.003 (3)0.000 (3)0.011 (3)
C10.068 (6)0.051 (3)0.048 (4)0.034 (3)0.002 (4)0.001 (2)
N210.109 (5)0.093 (5)0.073 (4)0.031 (4)0.025 (4)0.005 (3)
C20.066 (4)0.051 (3)0.054 (3)0.009 (3)0.000 (3)0.002 (3)
Geometric parameters (Å, º) top
Se1—C11.851 (8)N22—H22B0.8600
Se2—C21.854 (6)N22—C21.304 (7)
N11—H11A0.8600N21—H21A0.8600
N11—H11B0.8600N21—H21B0.8600
N11—C11.316 (6)N21—C21.302 (7)
N22—H22A0.8600
H11A—N11—H11B120.0N11i—C1—N11119.0 (7)
C1—N11—H11A120.0H21A—N21—H21B120.0
C1—N11—H11B120.0C2—N21—H21A120.0
H22A—N22—H22B120.0C2—N21—H21B120.0
C2—N22—H22A120.0N22—C2—Se2121.0 (4)
C2—N22—H22B120.0N21—C2—Se2120.2 (4)
N11—C1—Se1120.5 (3)N21—C2—N22118.8 (6)
N11i—C1—Se1120.5 (3)
Symmetry code: (i) x, x+y, z+4/3.
Selenourea (phase_gamma_Selenourea_393K) top
Crystal data top
CH4N2SeDx = 2.069 Mg m3
Mr = 123.02Mo Kα radiation, λ = 0.71073 Å
Trigonal, P3121Cell parameters from 1699 reflections
a = 8.8607 (4) Åθ = 4.1–25.0°
c = 13.0716 (7) ŵ = 9.28 mm1
V = 888.78 (9) Å3T = 393 K
Z = 9Plate, orange
F(000) = 5220.25 × 0.10 × 0.05 mm
Data collection top
Xcalibur, Eos
diffractometer
1422 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source1182 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 16.1544 pixels mm-1θmax = 28.9°, θmin = 3.1°
ω scansh = 1111
Absorption correction: multi-scan
CrysAlisPro 1.171.40.67a (Rigaku Oxford Diffraction, 2019) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1111
Tmin = 0.523, Tmax = 1.000l = 1716
6391 measured reflections
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0256P)2 + 0.223P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.029(Δ/σ)max < 0.001
wR(F2) = 0.059Δρmax = 0.51 e Å3
S = 1.02Δρmin = 0.31 e Å3
1422 reflectionsExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
57 parametersExtinction coefficient: 0.0041 (5)
0 restraintsAbsolute structure: Refined as a perfect inversion twin.
Primary atom site location: dualAbsolute structure parameter: 0.5
Hydrogen site location: inferred from neighbouring sites
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component perfect inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.0000000.07230 (7)0.6666670.0487 (2)
Se20.44461 (7)0.76430 (7)0.29075 (4)0.0571 (2)
N110.0389 (9)0.1924 (7)0.5832 (4)0.103 (2)
H11A0.0386050.2895500.5838250.123*
H11B0.0646280.1317490.5279720.123*
N220.2109 (8)0.4352 (7)0.2193 (4)0.108 (2)
H22A0.1248580.3303900.2244460.130*
H22B0.2685620.4698890.1630760.130*
C10.0000000.1365 (9)0.6666670.056 (2)
N210.1634 (9)0.4842 (8)0.3809 (4)0.131 (3)
H21A0.0780540.3788050.3838500.158*
H21B0.1888370.5514430.4332420.158*
C20.2540 (8)0.5419 (8)0.2973 (4)0.0676 (18)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0581 (6)0.0439 (3)0.0487 (3)0.0290 (3)0.0021 (4)0.00107 (19)
Se20.0468 (3)0.0486 (3)0.0651 (3)0.0157 (3)0.0000 (2)0.0014 (2)
N110.202 (7)0.076 (4)0.060 (3)0.092 (5)0.025 (4)0.004 (3)
N220.124 (5)0.061 (3)0.073 (3)0.005 (3)0.002 (3)0.010 (3)
C10.066 (6)0.055 (4)0.050 (4)0.033 (3)0.002 (4)0.001 (2)
N210.118 (5)0.091 (4)0.076 (4)0.030 (4)0.027 (4)0.005 (3)
C20.069 (4)0.050 (3)0.058 (3)0.010 (3)0.002 (3)0.001 (3)
Geometric parameters (Å, º) top
Se1—C11.850 (8)N22—H22B0.8600
Se2—C21.848 (6)N22—C21.311 (7)
N11—H11A0.8600N21—H21A0.8600
N11—H11B0.8600N21—H21B0.8600
N11—C11.313 (6)N21—C21.300 (7)
N22—H22A0.8600
H11A—N11—H11B120.0N11i—C1—N11118.9 (7)
C1—N11—H11A120.0H21A—N21—H21B120.0
C1—N11—H11B120.0C2—N21—H21A120.0
H22A—N22—H22B120.0C2—N21—H21B120.0
C2—N22—H22A120.0N22—C2—Se2121.0 (4)
C2—N22—H22B120.0N21—C2—Se2120.9 (4)
N11—C1—Se1120.5 (4)N21—C2—N22118.0 (6)
N11i—C1—Se1120.5 (4)
Symmetry code: (i) x, x+y, z+4/3.
 

Follow Acta Cryst. B
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds