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Organic seleno­cyanates R–Se–CN can act as an amphoteric chalcogen bond (ChB) donor (through the Se atom) and acceptor (through the N atom lone pair). Co-crystallization of tri-s­ubstituted 1,3,5-tris­(seleno­cyanato­methyl)-2,4,6-tri­methyl­benzene (1) is investigated with different ditopic Lewis bases acting as chalcogen bond (ChB) acceptors to investigate the outcome of the competition, as ChB acceptor, between the nitro­gen lone pair of the SeCN group and other Lewis bases involving pyridinyl or carbonyl functions. In the presence of tetra­methyl­pyrazine (TMP), benzo­quinone (BQ) and para-di­nitro­benzene (pDNB) as ditopic Lewis bases, a recurrent oligomeric motif stabilized by six ChB interactions is observed, involving six SeCN groups and the ChB acceptor sites of TMP, BQ and pDNB in the 2:1 adducts (1)2·TMP, (1)2·BQ and (1)2·pDNB.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520618017778/aw5020sup1.cif
Contains datablocks global, 1TMP, 1BQ, pDNB

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520618017778/aw5020sup2.pdf
Details on DFT calculations

CCDC references: 1885519; 1885520; 1885521

Computing details top

For all structures, data collection: Bruker APEX2 (Bruker, 2014); cell refinement: Bruker APEX2 (Bruker, 2014); data reduction: Bruker APEX2 (Bruker, 2014); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014); molecular graphics: ORTEP for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX publication routines (Farrugia, 2012).

(1TMP) top
Crystal data top
C15H15N3Se3·0.5(C8H12N2)Z = 2
Mr = 542.28F(000) = 530
Triclinic, P1Dx = 1.743 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.797 (3) ÅCell parameters from 6066 reflections
b = 10.560 (3) Åθ = 2.9–26.0°
c = 10.656 (3) ŵ = 5.35 mm1
α = 87.528 (10)°T = 296 K
β = 69.844 (8)°Prism, colorless
γ = 87.528 (9)°0.13 × 0.04 × 0.02 mm
V = 1033.5 (5) Å3
Data collection top
APEXII, Bruker-AXS
diffractometer
2995 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.057
CCD rotation images, thick slices scansθmax = 27.4°, θmin = 1.9°
Absorption correction: multi-scan
[Sheldrick, G.M. (2014). SADABS Bruker AXS Inc., Madison, Wisconsin, USA]
h = 1211
Tmin = 0.774, Tmax = 0.899k = 1313
25685 measured reflectionsl = 1313
4706 independent reflections
Refinement top
Refinement on F2Primary atom site location: direct - structure invariant direct methods
Least-squares matrix: fullSecondary atom site location: direct - structure invariant direct methods
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.092H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0366P)2 + 0.8648P]
where P = (Fo2 + 2Fc2)/3
4706 reflections(Δ/σ)max = 0.001
240 parametersΔρmax = 0.70 e Å3
0 restraintsΔρmin = 0.52 e Å3
0 constraints
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
C11.1028 (4)0.0541 (3)0.6188 (4)0.0294 (9)
C21.0005 (4)0.1473 (3)0.6089 (4)0.0301 (9)
C30.8647 (4)0.1574 (3)0.7117 (4)0.0307 (9)
C40.8305 (4)0.0742 (4)0.8242 (4)0.0316 (9)
C50.9339 (4)0.0186 (3)0.8325 (4)0.0313 (9)
C61.0712 (4)0.0283 (4)0.7316 (4)0.0312 (9)
C71.2445 (4)0.0403 (4)0.5037 (4)0.0389 (10)
H7A1.22340.04360.42110.047*
H7B1.28740.04280.51150.047*
C81.0357 (4)0.2374 (4)0.4879 (4)0.0434 (10)
H8A1.13490.26210.46260.065*
H8B0.97230.31120.50950.065*
H8C1.0220.19570.41490.065*
C90.7544 (4)0.2563 (4)0.7001 (4)0.0392 (10)
H9A0.65810.22820.75330.047*
H9B0.75920.26330.60760.047*
C100.6826 (4)0.0883 (4)0.9335 (4)0.0482 (11)
H10A0.67740.02931.00590.072*
H10B0.60770.07140.8980.072*
H10C0.66940.17310.96540.072*
C110.8979 (4)0.1095 (4)0.9517 (4)0.0373 (10)
H11A0.81770.07331.02410.045*
H11B0.98120.11840.98110.045*
C121.1824 (4)0.1278 (4)0.7429 (4)0.0433 (11)
H12A1.14680.17060.82880.065*
H12B1.27190.08790.73320.065*
H12C1.19930.18820.67390.065*
C131.3945 (4)0.1482 (4)0.6551 (5)0.0438 (11)
C140.8745 (5)0.3741 (4)0.8774 (5)0.0471 (11)
C150.7040 (5)0.2280 (4)0.8454 (4)0.0477 (12)
C161.3556 (4)0.5056 (4)0.5626 (5)0.0463 (11)
C171.4503 (5)0.4974 (4)0.6338 (5)0.0495 (12)
C181.1947 (5)0.5059 (5)0.6306 (5)0.0645 (14)
H18A1.1480.51430.56490.097*
H18B1.1650.57580.68980.097*
H18C1.16770.42780.68110.097*
C191.3974 (6)0.4993 (6)0.7839 (5)0.0805 (17)
H19A1.35230.42060.82030.121*
H19B1.32790.56810.81390.121*
H19C1.47820.51040.81330.121*
N11.4041 (5)0.1377 (5)0.7626 (5)0.0769 (14)
N20.9312 (5)0.3468 (4)0.9517 (5)0.0692 (12)
N30.6192 (5)0.2007 (4)0.7970 (4)0.0652 (12)
N41.4053 (4)0.5085 (3)0.4280 (4)0.0502 (10)
Se11.39051 (5)0.16930 (4)0.49006 (5)0.04673 (15)
Se20.78128 (5)0.42823 (4)0.75911 (5)0.05066 (15)
Se30.84421 (5)0.28103 (4)0.91729 (4)0.04628 (14)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0269 (19)0.027 (2)0.035 (2)0.0007 (16)0.0106 (16)0.0056 (17)
C20.030 (2)0.031 (2)0.031 (2)0.0081 (17)0.0104 (16)0.0018 (17)
C30.029 (2)0.026 (2)0.040 (2)0.0029 (16)0.0154 (17)0.0015 (18)
C40.0302 (19)0.030 (2)0.034 (2)0.0069 (17)0.0090 (16)0.0066 (18)
C50.037 (2)0.026 (2)0.033 (2)0.0069 (17)0.0137 (17)0.0004 (17)
C60.030 (2)0.028 (2)0.038 (2)0.0050 (16)0.0148 (17)0.0021 (18)
C70.037 (2)0.033 (2)0.042 (2)0.0030 (18)0.0080 (19)0.0043 (19)
C80.044 (2)0.046 (3)0.040 (2)0.001 (2)0.015 (2)0.008 (2)
C90.034 (2)0.040 (2)0.047 (3)0.0018 (18)0.0184 (19)0.001 (2)
C100.039 (2)0.049 (3)0.044 (3)0.001 (2)0.000 (2)0.006 (2)
C110.047 (2)0.030 (2)0.036 (2)0.0021 (18)0.0155 (19)0.0030 (18)
C120.039 (2)0.038 (2)0.051 (3)0.0006 (19)0.014 (2)0.007 (2)
C130.030 (2)0.043 (3)0.057 (3)0.0063 (19)0.011 (2)0.006 (2)
C140.055 (3)0.034 (3)0.057 (3)0.002 (2)0.025 (2)0.005 (2)
C150.051 (3)0.047 (3)0.038 (3)0.016 (2)0.003 (2)0.004 (2)
C160.035 (2)0.032 (2)0.064 (3)0.0003 (18)0.008 (2)0.007 (2)
C170.043 (3)0.045 (3)0.056 (3)0.002 (2)0.012 (2)0.008 (2)
C180.040 (3)0.065 (3)0.080 (4)0.001 (2)0.009 (2)0.002 (3)
C190.060 (3)0.109 (5)0.064 (4)0.004 (3)0.012 (3)0.006 (3)
N10.068 (3)0.098 (4)0.069 (3)0.028 (3)0.025 (3)0.003 (3)
N20.093 (3)0.053 (3)0.080 (3)0.002 (2)0.053 (3)0.001 (2)
N30.059 (3)0.079 (3)0.060 (3)0.008 (2)0.024 (2)0.003 (2)
N40.040 (2)0.044 (2)0.059 (3)0.0024 (17)0.0091 (19)0.0069 (19)
Se10.0380 (2)0.0469 (3)0.0507 (3)0.0098 (2)0.0092 (2)0.0056 (2)
Se20.0595 (3)0.0351 (3)0.0643 (3)0.0101 (2)0.0309 (2)0.0058 (2)
Se30.0597 (3)0.0320 (2)0.0470 (3)0.0110 (2)0.0179 (2)0.0059 (2)
Geometric parameters (Å, º) top
C1—C21.402 (5)C11—Se31.991 (4)
C1—C61.405 (5)C11—H11A0.97
C1—C71.509 (5)C11—H11B0.97
C2—C31.405 (5)C12—H12A0.96
C2—C81.517 (5)C12—H12B0.96
C3—C41.407 (5)C12—H12C0.96
C3—C91.502 (5)C13—N11.181 (6)
C4—C51.401 (5)C13—Se11.777 (5)
C4—C101.520 (5)C14—N21.134 (5)
C5—C61.406 (5)C14—Se21.854 (5)
C5—C111.508 (5)C15—N31.141 (6)
C6—C121.513 (5)C15—Se31.847 (6)
C7—Se11.983 (4)C16—N41.346 (6)
C7—H7A0.97C16—C171.385 (6)
C7—H7B0.97C16—C181.490 (6)
C8—H8A0.96C17—N4i1.339 (5)
C8—H8B0.96C17—C191.502 (7)
C8—H8C0.96C18—H18A0.96
C9—Se22.004 (4)C18—H18B0.96
C9—H9A0.97C18—H18C0.96
C9—H9B0.97C19—H19A0.96
C10—H10A0.96C19—H19B0.96
C10—H10B0.96C19—H19C0.96
C10—H10C0.96N4—C17i1.339 (5)
C2—C1—C6120.4 (3)H10A—C10—H10C109.5
C2—C1—C7118.8 (3)H10B—C10—H10C109.5
C6—C1—C7120.8 (3)C5—C11—Se3114.4 (3)
C1—C2—C3119.8 (3)C5—C11—H11A108.7
C1—C2—C8120.3 (3)Se3—C11—H11A108.7
C3—C2—C8119.9 (3)C5—C11—H11B108.7
C2—C3—C4120.5 (3)Se3—C11—H11B108.7
C2—C3—C9119.7 (3)H11A—C11—H11B107.6
C4—C3—C9119.9 (3)C6—C12—H12A109.5
C5—C4—C3119.1 (3)C6—C12—H12B109.5
C5—C4—C10122.0 (4)H12A—C12—H12B109.5
C3—C4—C10118.9 (3)C6—C12—H12C109.5
C4—C5—C6121.1 (3)H12A—C12—H12C109.5
C4—C5—C11119.6 (3)H12B—C12—H12C109.5
C6—C5—C11119.3 (3)N1—C13—Se1176.3 (4)
C1—C6—C5119.2 (3)N2—C14—Se2176.7 (4)
C1—C6—C12120.3 (3)N3—C15—Se3176.5 (4)
C5—C6—C12120.5 (3)N4—C16—C17121.2 (4)
C1—C7—Se1115.6 (3)N4—C16—C18116.9 (4)
C1—C7—H7A108.4C17—C16—C18121.8 (4)
Se1—C7—H7A108.4N4i—C17—C16121.5 (4)
C1—C7—H7B108.4N4i—C17—C19116.4 (4)
Se1—C7—H7B108.4C16—C17—C19122.1 (4)
H7A—C7—H7B107.4C16—C18—H18A109.5
C2—C8—H8A109.5C16—C18—H18B109.5
C2—C8—H8B109.5H18A—C18—H18B109.5
H8A—C8—H8B109.5C16—C18—H18C109.5
C2—C8—H8C109.5H18A—C18—H18C109.5
H8A—C8—H8C109.5H18B—C18—H18C109.5
H8B—C8—H8C109.5C17—C19—H19A109.5
C3—C9—Se2114.2 (3)C17—C19—H19B109.5
C3—C9—H9A108.7H19A—C19—H19B109.5
Se2—C9—H9A108.7C17—C19—H19C109.5
C3—C9—H9B108.7H19A—C19—H19C109.5
Se2—C9—H9B108.7H19B—C19—H19C109.5
H9A—C9—H9B107.6C17i—N4—C16117.3 (4)
C4—C10—H10A109.5C13—Se1—C797.41 (18)
C4—C10—H10B109.5C14—Se2—C997.04 (18)
H10A—C10—H10B109.5C15—Se3—C1196.98 (18)
C4—C10—H10C109.5
C6—C1—C2—C30.8 (5)C2—C1—C6—C12179.2 (4)
C7—C1—C2—C3176.6 (3)C7—C1—C6—C123.3 (5)
C6—C1—C2—C8179.1 (3)C4—C5—C6—C12.1 (5)
C7—C1—C2—C83.4 (5)C11—C5—C6—C1178.1 (3)
C1—C2—C3—C40.2 (5)C4—C5—C6—C12179.1 (4)
C8—C2—C3—C4179.8 (3)C11—C5—C6—C120.7 (5)
C1—C2—C3—C9179.2 (3)C2—C1—C7—Se177.1 (4)
C8—C2—C3—C90.8 (5)C6—C1—C7—Se1105.4 (4)
C2—C3—C4—C50.1 (5)C2—C3—C9—Se283.7 (4)
C9—C3—C4—C5179.1 (3)C4—C3—C9—Se297.3 (4)
C2—C3—C4—C10179.9 (3)C4—C5—C11—Se3101.7 (4)
C9—C3—C4—C101.1 (5)C6—C5—C11—Se378.4 (4)
C3—C4—C5—C61.0 (5)N4—C16—C17—N4i0.2 (7)
C10—C4—C5—C6178.7 (4)C18—C16—C17—N4i177.0 (4)
C3—C4—C5—C11179.1 (3)N4—C16—C17—C19177.5 (5)
C10—C4—C5—C111.1 (6)C18—C16—C17—C195.3 (7)
C2—C1—C6—C52.0 (5)C17—C16—N4—C17i0.2 (7)
C7—C1—C6—C5175.4 (3)C18—C16—N4—C17i177.1 (4)
Symmetry code: (i) x+3, y+1, z+1.
(1BQ) top
Crystal data top
C15H15N3Se3·0.5(C6H4O2)Z = 2
Mr = 528.23F(000) = 512
Triclinic, P1Dx = 1.781 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 10.008 (2) ÅCell parameters from 3951 reflections
b = 10.4345 (19) Åθ = 2.7–24.6°
c = 10.760 (2) ŵ = 5.61 mm1
α = 93.538 (5)°T = 296 K
β = 117.528 (5)°Needle, yellow
γ = 95.282 (5)°0.28 × 0.02 × 0.01 mm
V = 985.3 (3) Å3
Data collection top
APEXII, Bruker-AXS
diffractometer
4486 independent reflections
Radiation source: fine-focus sealed tube2412 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.088
CCD rotation images, thick slices scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
[Sheldrick, G.M. (2014). SADABS Bruker AXS Inc., Madison, Wisconsin, USA]
h = 1212
Tmin = 0.874, Tmax = 0.945k = 139
24136 measured reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: direct - structure invariant direct methods
Least-squares matrix: fullSecondary atom site location: direct - structure invariant direct methods
R[F2 > 2σ(F2)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.140H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0523P)2 + 1.8613P]
where P = (Fo2 + 2Fc2)/3
4486 reflections(Δ/σ)max < 0.001
229 parametersΔρmax = 0.82 e Å3
0 restraintsΔρmin = 0.66 e Å3
0 constraints
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
C10.2459 (7)0.1361 (5)0.1014 (6)0.0321 (14)
C20.3681 (6)0.0463 (5)0.1990 (6)0.0340 (14)
C30.3457 (7)0.0362 (5)0.2937 (6)0.0338 (14)
C40.2058 (7)0.0294 (5)0.2918 (6)0.0348 (14)
C50.0830 (6)0.0576 (5)0.1908 (6)0.0349 (14)
C60.1044 (6)0.1417 (5)0.0958 (6)0.0351 (14)
C70.2677 (7)0.2239 (6)0.0014 (7)0.0436 (16)
H7A0.36080.190.00240.052*
H7B0.18420.22210.0950.052*
C80.5219 (7)0.0412 (7)0.2045 (7)0.0507 (17)
H8A0.51810.00530.12310.076*
H8B0.54880.12720.20540.076*
H8C0.59660.01210.28850.076*
C90.4780 (7)0.1338 (5)0.4028 (7)0.0404 (15)
H9A0.57260.10830.41180.048*
H9B0.48020.13110.49370.048*
C100.1824 (8)0.1204 (6)0.3930 (7)0.0491 (17)
H10A0.27920.15480.47130.074*
H10B0.12080.07390.42680.074*
H10C0.13240.19020.34520.074*
C110.0713 (7)0.0630 (6)0.1813 (7)0.0437 (16)
H11A0.14610.06760.08270.052*
H11B0.07580.0170.22920.052*
C120.0276 (7)0.2393 (6)0.0105 (7)0.0502 (18)
H12A0.00140.2770.07850.075*
H12B0.11570.19640.05770.075*
H12C0.04940.30610.03750.075*
C130.4240 (9)0.3722 (7)0.2222 (9)0.066 (2)
C140.4365 (8)0.2799 (6)0.1744 (9)0.0514 (18)
C150.0408 (8)0.1809 (7)0.4401 (9)0.0529 (19)
C160.0120 (9)0.5398 (7)0.3680 (8)0.060 (2)
C170.1339 (9)0.5270 (7)0.4971 (9)0.067 (2)
H170.21980.54590.49080.08*
C180.1471 (8)0.4896 (6)0.6225 (8)0.056 (2)
H180.24090.4820.70320.067*
N10.5095 (9)0.3534 (6)0.3385 (8)0.091 (3)
N20.4193 (7)0.2576 (7)0.0607 (8)0.0695 (18)
N30.1399 (8)0.1689 (6)0.5479 (8)0.073 (2)
O10.0224 (7)0.5746 (6)0.2513 (7)0.0907 (19)
Se10.27892 (10)0.40669 (7)0.03883 (8)0.0644 (3)
Se20.46601 (8)0.31386 (6)0.35479 (8)0.0526 (2)
Se30.12835 (8)0.21052 (7)0.26265 (8)0.0524 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.040 (4)0.030 (3)0.030 (3)0.006 (3)0.019 (3)0.009 (3)
C20.031 (3)0.034 (3)0.038 (3)0.010 (3)0.015 (3)0.013 (3)
C30.038 (4)0.023 (3)0.034 (3)0.003 (2)0.010 (3)0.007 (3)
C40.036 (4)0.035 (3)0.036 (3)0.007 (3)0.017 (3)0.008 (3)
C50.033 (3)0.036 (3)0.041 (4)0.011 (3)0.020 (3)0.010 (3)
C60.033 (4)0.035 (3)0.030 (3)0.002 (3)0.009 (3)0.006 (3)
C70.048 (4)0.039 (3)0.041 (4)0.007 (3)0.019 (3)0.002 (3)
C80.041 (4)0.053 (4)0.058 (4)0.001 (3)0.026 (3)0.007 (3)
C90.038 (4)0.032 (3)0.042 (4)0.007 (3)0.011 (3)0.008 (3)
C100.052 (4)0.051 (4)0.044 (4)0.002 (3)0.026 (3)0.007 (3)
C110.043 (4)0.038 (3)0.054 (4)0.009 (3)0.025 (3)0.010 (3)
C120.032 (4)0.054 (4)0.056 (4)0.003 (3)0.014 (3)0.003 (3)
C130.062 (5)0.043 (4)0.070 (6)0.006 (4)0.010 (5)0.009 (4)
C140.055 (5)0.044 (4)0.060 (5)0.010 (3)0.029 (4)0.017 (4)
C150.042 (4)0.057 (4)0.074 (6)0.008 (3)0.038 (4)0.023 (4)
C160.063 (5)0.042 (4)0.055 (5)0.003 (3)0.013 (4)0.005 (4)
C170.055 (5)0.057 (5)0.075 (6)0.002 (4)0.024 (5)0.008 (4)
C180.038 (4)0.045 (4)0.058 (5)0.002 (3)0.003 (4)0.000 (4)
N10.102 (6)0.059 (4)0.066 (5)0.011 (4)0.001 (4)0.016 (4)
N20.062 (4)0.081 (5)0.076 (5)0.016 (3)0.038 (4)0.027 (4)
N30.048 (4)0.073 (5)0.074 (5)0.006 (3)0.008 (4)0.018 (4)
O10.092 (4)0.099 (5)0.069 (4)0.008 (3)0.031 (4)0.015 (4)
Se10.0763 (6)0.0383 (4)0.0574 (5)0.0103 (3)0.0144 (4)0.0032 (3)
Se20.0525 (5)0.0330 (4)0.0600 (5)0.0034 (3)0.0178 (4)0.0046 (3)
Se30.0416 (4)0.0567 (4)0.0604 (5)0.0011 (3)0.0259 (4)0.0125 (3)
Geometric parameters (Å, º) top
C1—C61.385 (8)C10—H10B0.96
C1—C21.399 (8)C10—H10C0.96
C1—C71.498 (8)C11—Se31.982 (6)
C2—C31.403 (8)C11—H11A0.97
C2—C81.509 (8)C11—H11B0.97
C3—C41.385 (8)C12—H12A0.96
C3—C91.529 (8)C12—H12B0.96
C4—C51.398 (8)C12—H12C0.96
C4—C101.514 (8)C13—N11.134 (9)
C5—C61.410 (8)C13—Se11.816 (8)
C5—C111.495 (8)C14—N21.159 (9)
C6—C121.517 (8)C14—Se21.829 (8)
C7—Se11.983 (6)C15—N31.114 (9)
C7—H7A0.97C15—Se31.857 (9)
C7—H7B0.97C16—O11.240 (9)
C8—H8A0.96C16—C18i1.460 (11)
C8—H8B0.96C16—C171.466 (10)
C8—H8C0.96C17—C181.323 (10)
C9—Se21.978 (6)C17—H170.93
C9—H9A0.97C18—C16i1.460 (11)
C9—H9B0.97C18—H180.93
C10—H10A0.96
C6—C1—C2120.8 (5)H9A—C9—H9B107.7
C6—C1—C7119.9 (5)C4—C10—H10A109.5
C2—C1—C7119.3 (5)C4—C10—H10B109.5
C1—C2—C3118.7 (5)H10A—C10—H10B109.5
C1—C2—C8120.4 (5)C4—C10—H10C109.5
C3—C2—C8120.9 (5)H10A—C10—H10C109.5
C4—C3—C2121.1 (5)H10B—C10—H10C109.5
C4—C3—C9119.2 (5)C5—C11—Se3114.9 (4)
C2—C3—C9119.7 (5)C5—C11—H11A108.5
C3—C4—C5119.8 (5)Se3—C11—H11A108.5
C3—C4—C10120.6 (5)C5—C11—H11B108.5
C5—C4—C10119.5 (5)Se3—C11—H11B108.5
C4—C5—C6119.6 (5)H11A—C11—H11B107.5
C4—C5—C11121.2 (5)C6—C12—H12A109.5
C6—C5—C11119.2 (5)C6—C12—H12B109.5
C1—C6—C5119.9 (5)H12A—C12—H12B109.5
C1—C6—C12120.5 (5)C6—C12—H12C109.5
C5—C6—C12119.6 (5)H12A—C12—H12C109.5
C1—C7—Se1114.8 (4)H12B—C12—H12C109.5
C1—C7—H7A108.6N1—C13—Se1176.6 (9)
Se1—C7—H7A108.6N2—C14—Se2179.2 (7)
C1—C7—H7B108.6N3—C15—Se3176.5 (7)
Se1—C7—H7B108.6O1—C16—C18i119.7 (7)
H7A—C7—H7B107.5O1—C16—C17121.1 (8)
C2—C8—H8A109.5C18i—C16—C17119.2 (7)
C2—C8—H8B109.5C18—C17—C16121.9 (8)
H8A—C8—H8B109.5C18—C17—H17119
C2—C8—H8C109.5C16—C17—H17119
H8A—C8—H8C109.5C17—C18—C16i118.9 (7)
H8B—C8—H8C109.5C17—C18—H18120.6
C3—C9—Se2113.6 (4)C16i—C18—H18120.6
C3—C9—H9A108.9C13—Se1—C796.6 (3)
Se2—C9—H9A108.9C14—Se2—C997.2 (3)
C3—C9—H9B108.9C15—Se3—C1197.3 (3)
Se2—C9—H9B108.9
C6—C1—C2—C31.5 (8)C7—C1—C6—C5178.9 (5)
C7—C1—C2—C3179.4 (5)C2—C1—C6—C12179.9 (5)
C6—C1—C2—C8179.8 (5)C7—C1—C6—C122.0 (8)
C7—C1—C2—C82.3 (8)C4—C5—C6—C11.2 (8)
C1—C2—C3—C40.1 (8)C11—C5—C6—C1178.7 (5)
C8—C2—C3—C4178.2 (5)C4—C5—C6—C12177.9 (5)
C1—C2—C3—C9179.1 (5)C11—C5—C6—C122.2 (8)
C8—C2—C3—C90.9 (8)C6—C1—C7—Se175.7 (6)
C2—C3—C4—C52.3 (8)C2—C1—C7—Se1106.4 (5)
C9—C3—C4—C5178.7 (5)C4—C3—C9—Se277.2 (6)
C2—C3—C4—C10179.0 (5)C2—C3—C9—Se2103.8 (5)
C9—C3—C4—C102.0 (8)C4—C5—C11—Se3102.8 (6)
C3—C4—C5—C62.8 (8)C6—C5—C11—Se377.3 (6)
C10—C4—C5—C6179.6 (5)O1—C16—C17—C18179.7 (7)
C3—C4—C5—C11177.1 (5)C18i—C16—C17—C180.1 (11)
C10—C4—C5—C110.3 (8)C16—C17—C18—C16i0.1 (11)
C2—C1—C6—C51.0 (8)
Symmetry code: (i) x, y1, z+1.
(pDNB) top
Crystal data top
C15H15N3Se3·0.5(C6H4N2O4)Z = 2
Mr = 558.23F(000) = 542
Triclinic, P1Dx = 1.821 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 10.187 (3) ÅCell parameters from 4815 reflections
b = 10.415 (2) Åθ = 2.7–24.5°
c = 11.232 (3) ŵ = 5.44 mm1
α = 75.891 (8)°T = 296 K
β = 82.213 (9)°Needle, colorless
γ = 61.753 (8)°0.31 × 0.03 × 0.01 mm
V = 1017.8 (5) Å3
Data collection top
APEXII, Bruker-AXS
diffractometer
4665 independent reflections
Radiation source: fine-focus sealed tube2903 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.050
CCD rotation images, thick slices scansθmax = 27.5°, θmin = 3.2°
Absorption correction: multi-scan
[Sheldrick, G.M. (2014). SADABS Bruker AXS Inc., Madison, Wisconsin, USA]
h = 1213
Tmin = 0.822, Tmax = 0.947k = 913
16919 measured reflectionsl = 1414
Refinement top
Refinement on F20 constraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.106 w = 1/[σ2(Fo2) + (0.0466P)2 + 0.8073P]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max < 0.001
4665 reflectionsΔρmax = 1.10 e Å3
247 parametersΔρmin = 0.47 e Å3
0 restraints
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
C10.7626 (4)0.3551 (4)0.6373 (3)0.0294 (9)
C20.8745 (4)0.2905 (4)0.5518 (3)0.0318 (9)
C30.8465 (4)0.2250 (4)0.4688 (3)0.0298 (9)
C40.7094 (5)0.2235 (4)0.4722 (3)0.0315 (9)
C50.5986 (4)0.2900 (4)0.5582 (4)0.0315 (9)
C60.6261 (4)0.3537 (4)0.6419 (3)0.0313 (9)
C70.7900 (5)0.4315 (5)0.7228 (4)0.0386 (10)
H7A0.70070.52420.72720.046*
H7B0.86940.45650.68760.046*
C81.0239 (5)0.2899 (5)0.5492 (4)0.0473 (11)
H8A1.01110.37480.5780.071*
H8B1.06380.29440.46660.071*
H8C1.09140.20040.60130.071*
C90.9653 (5)0.1547 (5)0.3778 (4)0.0401 (10)
H9A0.97240.05850.37780.048*
H9B1.060.13750.40440.048*
C100.6805 (5)0.1521 (5)0.3825 (4)0.0472 (12)
H10A0.62270.22810.3160.071*
H10B0.62680.09850.4240.071*
H10C0.77380.08460.35090.071*
C110.4483 (5)0.2965 (5)0.5572 (4)0.0396 (10)
H11A0.43710.2810.47820.048*
H11B0.37260.3960.56420.048*
C120.5088 (5)0.4197 (5)0.7361 (4)0.0440 (11)
H12A0.44390.52210.70230.066*
H12B0.55550.41380.80730.066*
H12C0.45180.36540.7590.066*
C130.9562 (8)0.1316 (6)0.8556 (5)0.0750 (18)
C140.8938 (5)0.4509 (6)0.2443 (4)0.0458 (11)
C150.5742 (6)0.0177 (6)0.6603 (4)0.0446 (11)
C160.4477 (7)0.1332 (6)0.0274 (4)0.0576 (14)
C170.5966 (7)0.0544 (6)0.0116 (5)0.0680 (16)
H170.6610.09190.01930.082*
C180.3507 (7)0.0832 (6)0.0164 (5)0.0648 (15)
H180.24890.14130.02760.078*
N111.0246 (10)0.0148 (6)0.8390 (5)0.141 (3)
N20.8630 (5)0.5639 (5)0.2635 (4)0.0625 (12)
N30.6727 (5)0.1317 (6)0.6509 (4)0.0696 (13)
N40.3869 (8)0.2844 (6)0.0585 (4)0.0791 (16)
O10.2556 (7)0.3623 (5)0.0522 (5)0.1136 (19)
O20.4768 (7)0.3155 (5)0.0890 (5)0.1110 (18)
Se10.84403 (7)0.31350 (6)0.89203 (4)0.05981 (18)
Se20.93243 (6)0.27375 (5)0.20684 (4)0.05169 (17)
Se30.40943 (5)0.15159 (5)0.68743 (4)0.04589 (15)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.035 (2)0.029 (2)0.023 (2)0.0131 (18)0.0053 (17)0.0053 (16)
C20.033 (2)0.033 (2)0.029 (2)0.0160 (19)0.0061 (18)0.0028 (17)
C30.032 (2)0.027 (2)0.025 (2)0.0088 (18)0.0022 (17)0.0042 (16)
C40.041 (2)0.028 (2)0.027 (2)0.0168 (19)0.0101 (18)0.0008 (17)
C50.035 (2)0.029 (2)0.030 (2)0.0149 (18)0.0025 (18)0.0030 (17)
C60.034 (2)0.029 (2)0.027 (2)0.0112 (18)0.0018 (17)0.0027 (17)
C70.049 (3)0.041 (2)0.029 (2)0.022 (2)0.0018 (19)0.0076 (19)
C80.035 (3)0.062 (3)0.050 (3)0.023 (2)0.001 (2)0.020 (2)
C90.042 (3)0.039 (2)0.032 (2)0.012 (2)0.0008 (19)0.0120 (19)
C100.057 (3)0.051 (3)0.046 (3)0.030 (2)0.001 (2)0.021 (2)
C110.044 (3)0.042 (2)0.033 (2)0.021 (2)0.0069 (19)0.0019 (19)
C120.040 (3)0.048 (3)0.047 (3)0.018 (2)0.007 (2)0.021 (2)
C130.124 (5)0.051 (3)0.032 (3)0.025 (4)0.012 (3)0.007 (2)
C140.042 (3)0.055 (3)0.044 (3)0.026 (2)0.001 (2)0.009 (2)
C150.042 (3)0.053 (3)0.043 (3)0.028 (3)0.002 (2)0.007 (2)
C160.089 (4)0.051 (3)0.036 (3)0.036 (3)0.011 (3)0.014 (2)
C170.090 (5)0.075 (4)0.052 (3)0.050 (4)0.009 (3)0.017 (3)
C180.073 (4)0.059 (3)0.050 (3)0.019 (3)0.012 (3)0.022 (3)
N110.258 (9)0.049 (3)0.056 (4)0.017 (4)0.014 (4)0.017 (3)
N20.059 (3)0.058 (3)0.079 (3)0.031 (2)0.002 (2)0.019 (2)
N30.059 (3)0.072 (3)0.070 (3)0.028 (3)0.012 (2)0.014 (3)
N40.122 (5)0.057 (3)0.050 (3)0.035 (4)0.015 (3)0.019 (3)
O10.133 (5)0.060 (3)0.114 (4)0.010 (3)0.003 (4)0.035 (3)
O20.166 (5)0.094 (4)0.107 (4)0.077 (4)0.020 (4)0.055 (3)
Se10.0785 (4)0.0578 (3)0.0344 (3)0.0178 (3)0.0103 (2)0.0182 (2)
Se20.0685 (4)0.0520 (3)0.0304 (3)0.0231 (3)0.0065 (2)0.0151 (2)
Se30.0452 (3)0.0480 (3)0.0469 (3)0.0255 (2)0.0043 (2)0.0079 (2)
Geometric parameters (Å, º) top
C1—C61.391 (5)C10—H10C0.96
C1—C21.402 (5)C11—Se31.977 (4)
C1—C71.513 (5)C11—H11A0.97
C2—C31.408 (5)C11—H11B0.97
C2—C81.516 (6)C12—H12A0.96
C3—C41.400 (6)C12—H12B0.96
C3—C91.495 (5)C12—H12C0.96
C4—C51.406 (5)C13—N111.128 (7)
C4—C101.518 (5)C13—Se11.807 (6)
C5—C61.399 (5)C14—N21.133 (6)
C5—C111.501 (6)C14—Se21.840 (5)
C6—C121.502 (5)C15—N31.154 (6)
C7—Se11.983 (4)C15—Se31.828 (5)
C7—H7A0.97C16—C181.347 (8)
C7—H7B0.97C16—C171.352 (8)
C8—H8A0.96C16—N41.507 (7)
C8—H8B0.96C17—C18i1.374 (7)
C8—H8C0.96C17—H170.93
C9—Se21.989 (4)C18—C17i1.373 (7)
C9—H9A0.97C18—H180.93
C9—H9B0.97N4—O11.193 (7)
C10—H10A0.96N4—O21.217 (7)
C10—H10B0.96
C6—C1—C2121.0 (3)C4—C10—H10A109.5
C6—C1—C7119.8 (4)C4—C10—H10B109.5
C2—C1—C7119.1 (4)H10A—C10—H10B109.5
C1—C2—C3119.0 (4)C4—C10—H10C109.5
C1—C2—C8120.6 (4)H10A—C10—H10C109.5
C3—C2—C8120.4 (4)H10B—C10—H10C109.5
C4—C3—C2120.5 (3)C5—C11—Se3115.8 (3)
C4—C3—C9120.0 (4)C5—C11—H11A108.3
C2—C3—C9119.6 (4)Se3—C11—H11A108.3
C3—C4—C5119.4 (3)C5—C11—H11B108.3
C3—C4—C10120.0 (4)Se3—C11—H11B108.3
C5—C4—C10120.5 (4)H11A—C11—H11B107.4
C6—C5—C4120.5 (4)C6—C12—H12A109.5
C6—C5—C11120.0 (4)C6—C12—H12B109.5
C4—C5—C11119.6 (4)H12A—C12—H12B109.5
C1—C6—C5119.5 (4)C6—C12—H12C109.5
C1—C6—C12120.5 (4)H12A—C12—H12C109.5
C5—C6—C12119.9 (4)H12B—C12—H12C109.5
C1—C7—Se1115.1 (3)N11—C13—Se1176.3 (6)
C1—C7—H7A108.5N2—C14—Se2176.1 (5)
Se1—C7—H7A108.5N3—C15—Se3173.8 (4)
C1—C7—H7B108.5C18—C16—C17123.1 (5)
Se1—C7—H7B108.5C18—C16—N4118.3 (6)
H7A—C7—H7B107.5C17—C16—N4118.6 (6)
C2—C8—H8A109.5C16—C17—C18i117.5 (5)
C2—C8—H8B109.5C16—C17—H17121.3
H8A—C8—H8B109.5C18i—C17—H17121.3
C2—C8—H8C109.5C16—C18—C17i119.4 (5)
H8A—C8—H8C109.5C16—C18—H18120.3
H8B—C8—H8C109.5C17i—C18—H18120.3
C3—C9—Se2114.7 (3)O1—N4—O2125.8 (6)
C3—C9—H9A108.6O1—N4—C16117.5 (7)
Se2—C9—H9A108.6O2—N4—C16116.7 (6)
C3—C9—H9B108.6C13—Se1—C798.5 (2)
Se2—C9—H9B108.6C14—Se2—C996.84 (19)
H9A—C9—H9B107.6C15—Se3—C1198.19 (19)
C6—C1—C2—C30.8 (5)C7—C1—C6—C123.6 (6)
C7—C1—C2—C3177.3 (3)C4—C5—C6—C12.0 (6)
C6—C1—C2—C8178.8 (4)C11—C5—C6—C1176.1 (3)
C7—C1—C2—C83.1 (6)C4—C5—C6—C12177.9 (4)
C1—C2—C3—C40.4 (5)C11—C5—C6—C123.9 (6)
C8—C2—C3—C4179.1 (4)C6—C1—C7—Se180.4 (4)
C1—C2—C3—C9179.6 (3)C2—C1—C7—Se1101.5 (4)
C8—C2—C3—C90.0 (6)C4—C3—C9—Se276.3 (4)
C2—C3—C4—C50.9 (6)C2—C3—C9—Se2104.6 (4)
C9—C3—C4—C5180.0 (3)C6—C5—C11—Se378.3 (4)
C2—C3—C4—C10179.8 (4)C4—C5—C11—Se3103.6 (4)
C9—C3—C4—C100.7 (6)C18—C16—C17—C18i0.3 (9)
C3—C4—C5—C61.7 (6)N4—C16—C17—C18i179.8 (4)
C10—C4—C5—C6179.0 (4)C17—C16—C18—C17i0.3 (9)
C3—C4—C5—C11176.5 (3)N4—C16—C18—C17i179.8 (4)
C10—C4—C5—C112.9 (6)C18—C16—N4—O112.0 (8)
C2—C1—C6—C51.6 (6)C17—C16—N4—O1167.9 (6)
C7—C1—C6—C5176.5 (3)C18—C16—N4—O2167.4 (5)
C2—C1—C6—C12178.4 (4)C17—C16—N4—O212.7 (7)
Symmetry code: (i) x+1, y, z.
 

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