Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
In the title compound, (CH2)2(PPh2)2Se2 or C26H24P2Se2, there are two half-mol­ecules in the asymmetric unit, both molecules having inversion symmetry. The P—Se bond lengths suggest weak double-bond character. Weak C—H...Se hydrogen bonds help to assemble the mol­ecules into a three-dimensional network.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807046594/hb2546sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807046594/hb2546Isup2.hkl
Contains datablock I

CCDC reference: 663842

Key indicators

  • Single-crystal X-ray study
  • T = 120 K
  • Mean [sigma](C-C) = 0.009 Å
  • R factor = 0.052
  • wR factor = 0.160
  • Data-to-parameter ratio = 15.1

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.98 PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 3000 Deg. PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 9 PLAT480_ALERT_4_C Long H...A H-Bond Reported H15 .. SE1 .. 3.03 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H25 .. SE2 .. 3.01 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H24 .. SE2 .. 2.99 Ang.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 7 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The crystals of the title compound, (I), (CH2)2(PPh2)2Se2, were isolated as a side product during the synthesis (Risto et al., 2007) of [Pd(SeC4H4S)2(dppe)] (dppe = diphenylphosphine) from [PdCl2(dppe)] and LiSeC4H4S (prepared from thiophene, n-butyllithium, and an excess of elemental selenium). The asymmetric unit of (I) consists of two independent half-molecules, both molecular environments being completed by crystallographic inversion symmetry (Fig. 1). The two independent P—Se bond lengths are 2.104 (2) and 2.109 (2) Å indicating a slight double bond character [the sum of the covalent radii of phosphorus and selenium is 2.22 Å (Emsley 1998)]. The other bonds show normal single bond lengths. The molecules are assembled into a three-dimensional network by weak C—H···Se interactions (Table 2, Fig. 2).

Related literature top

For further details, see: Risto et al. (2007). For a related structure and background, see: Brown et al. (1980). For reference structural data, see: Emsley (1998).

Experimental top

The crystals of the title compound were isolated in synthesis of [Pd(SeC4H4S)2(dppe)] from [PdCl2(dppe)] (0.387 g, 0.673 mmol, in 15 ml dichloromethane) and lithium 2-thienylselenolate (1.474 mmol in 4.1 ml tetrahydrofuran, prepared from thiophene, n-butyllithium, and an excess of elemental selenium; used in situ). Colourless plates of (I) were obtained from the reaction mixture.

Refinement top

The H atoms were positioned geometrically (C—H = 0.95–0.98 Å) and refined as riding with Uiso(H) = 1.2 Ueq(C).

Structure description top

The crystals of the title compound, (I), (CH2)2(PPh2)2Se2, were isolated as a side product during the synthesis (Risto et al., 2007) of [Pd(SeC4H4S)2(dppe)] (dppe = diphenylphosphine) from [PdCl2(dppe)] and LiSeC4H4S (prepared from thiophene, n-butyllithium, and an excess of elemental selenium). The asymmetric unit of (I) consists of two independent half-molecules, both molecular environments being completed by crystallographic inversion symmetry (Fig. 1). The two independent P—Se bond lengths are 2.104 (2) and 2.109 (2) Å indicating a slight double bond character [the sum of the covalent radii of phosphorus and selenium is 2.22 Å (Emsley 1998)]. The other bonds show normal single bond lengths. The molecules are assembled into a three-dimensional network by weak C—H···Se interactions (Table 2, Fig. 2).

For further details, see: Risto et al. (2007). For a related structure and background, see: Brown et al. (1980). For reference structural data, see: Emsley (1998).

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg & Berndt, 1999); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) with displacement ellipsoids for the non-hydrogen atoms drawn at the 50% probability limit. The unlabelled atoms in the C1 and C2 molecule are generated by the symmetry operations (-x, -y, 2 - z) and (-x, 1 - y, 1 - z), respectively.
[Figure 2] Fig. 2. The packing of molecules in (I) with C—H···Se interactions indicated by dashed lines.
1,2-bis(Diphenylphosphinoselenoyl)ethane top
Crystal data top
C26H24P2Se2Z = 2
Mr = 556.31F(000) = 556
Triclinic, P1Dx = 1.544 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 10.322 (2) ÅCell parameters from 3328 reflections
b = 10.843 (2) Åθ = 2.3–25.0°
c = 12.285 (3) ŵ = 3.24 mm1
α = 90.93 (3)°T = 120 K
β = 108.13 (3)°Plate, colourless
γ = 112.14 (3)°0.10 × 0.10 × 0.05 mm
V = 1196.3 (4) Å3
Data collection top
Nonius KappaCCD area-detector
diffractometer
4095 independent reflections
Radiation source: fine-focus sealed tube3328 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.099
φ scans, and ω scans with κ offsetsθmax = 25.0°, θmin = 2.3°
Absorption correction: multi-scan
(XPREP in SHELXTL; Bruker, 2001)
h = 1212
Tmin = 0.738, Tmax = 0.855k = 1212
14810 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.160H-atom parameters constrained
S = 1.11 w = 1/[σ2(Fo2) + (0.0852P)2 + 2.3976P]
where P = (Fo2 + 2Fc2)/3
4095 reflections(Δ/σ)max = 0.001
271 parametersΔρmax = 0.58 e Å3
0 restraintsΔρmin = 0.75 e Å3
Crystal data top
C26H24P2Se2γ = 112.14 (3)°
Mr = 556.31V = 1196.3 (4) Å3
Triclinic, P1Z = 2
a = 10.322 (2) ÅMo Kα radiation
b = 10.843 (2) ŵ = 3.24 mm1
c = 12.285 (3) ÅT = 120 K
α = 90.93 (3)°0.10 × 0.10 × 0.05 mm
β = 108.13 (3)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
4095 independent reflections
Absorption correction: multi-scan
(XPREP in SHELXTL; Bruker, 2001)
3328 reflections with I > 2σ(I)
Tmin = 0.738, Tmax = 0.855Rint = 0.099
14810 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0520 restraints
wR(F2) = 0.160H-atom parameters constrained
S = 1.11Δρmax = 0.58 e Å3
4095 reflectionsΔρmin = 0.75 e Å3
271 parameters
Special details top

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

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Se10.37097 (7)0.12472 (6)1.09921 (5)0.0283 (2)
Se20.76343 (7)0.38570 (6)0.51739 (5)0.0245 (2)
P10.19425 (17)0.09757 (15)0.94441 (13)0.0179 (3)
P20.60174 (16)0.36746 (14)0.59353 (13)0.0172 (3)
C10.0226 (7)0.0653 (6)0.9721 (5)0.0212 (13)
H1A0.03600.14261.02480.025*
H1B0.05770.05530.89850.025*
C20.5289 (7)0.4973 (6)0.5655 (5)0.0202 (12)
H2A0.44680.47850.59670.024*
H2B0.60850.58590.60600.024*
C110.1511 (6)0.0439 (6)0.8372 (5)0.0168 (12)
C120.0077 (7)0.1131 (6)0.7594 (5)0.0243 (13)
H120.06970.08700.76160.029*
C130.0230 (7)0.2195 (6)0.6788 (5)0.0251 (14)
H130.12150.26720.62630.030*
C140.0889 (7)0.2562 (6)0.6748 (5)0.0264 (14)
H140.06740.33030.62010.032*
C150.2308 (7)0.1869 (6)0.7489 (5)0.0264 (14)
H150.30790.21200.74420.032*
C160.2642 (7)0.0800 (6)0.8311 (6)0.0259 (14)
H160.36330.03230.88250.031*
C210.2249 (6)0.2447 (5)0.8708 (5)0.0173 (12)
C220.3695 (7)0.3401 (6)0.8960 (5)0.0219 (13)
H220.45090.32810.95020.026*
C230.3934 (7)0.4541 (6)0.8404 (5)0.0255 (14)
H230.49180.51990.85690.031*
C240.2746 (8)0.4717 (6)0.7614 (5)0.0277 (15)
H240.29200.54920.72390.033*
C250.1316 (8)0.3772 (6)0.7374 (6)0.0301 (15)
H250.05010.38970.68400.036*
C260.1073 (7)0.2630 (6)0.7919 (5)0.0264 (14)
H260.00890.19700.77470.032*
C310.4360 (7)0.2109 (6)0.5413 (5)0.0190 (12)
C320.3272 (7)0.1831 (6)0.5921 (5)0.0235 (13)
H320.33760.24840.65030.028*
C330.2047 (7)0.0625 (6)0.5595 (5)0.0274 (14)
H330.13240.04330.59640.033*
C340.1881 (7)0.0310 (6)0.4719 (6)0.0286 (15)
H340.10370.11450.44850.034*
C350.2937 (7)0.0027 (6)0.4188 (6)0.0303 (15)
H350.28110.06680.35860.036*
C360.4176 (7)0.1178 (6)0.4524 (5)0.0237 (13)
H360.48960.13700.41520.028*
C410.6711 (6)0.3761 (6)0.7497 (5)0.0182 (12)
C420.7566 (7)0.5016 (6)0.8218 (5)0.0255 (14)
H420.77430.58280.78940.031*
C430.8148 (8)0.5053 (7)0.9404 (6)0.0314 (15)
H430.87120.58960.98960.038*
C440.7916 (8)0.3880 (7)0.9876 (6)0.0299 (15)
H440.83160.39161.06910.036*
C450.7107 (8)0.2655 (7)0.9171 (5)0.0308 (15)
H450.69630.18490.95010.037*
C460.6504 (7)0.2584 (6)0.7992 (5)0.0256 (14)
H460.59460.17320.75130.031*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se10.0319 (4)0.0263 (4)0.0202 (4)0.0109 (3)0.0013 (3)0.0036 (3)
Se20.0223 (4)0.0299 (4)0.0237 (4)0.0112 (3)0.0101 (3)0.0055 (3)
P10.0202 (8)0.0160 (7)0.0177 (8)0.0061 (6)0.0080 (6)0.0042 (6)
P20.0197 (8)0.0165 (8)0.0156 (8)0.0078 (6)0.0057 (6)0.0043 (6)
C10.029 (3)0.019 (3)0.028 (3)0.014 (3)0.021 (3)0.012 (3)
C20.021 (3)0.015 (3)0.018 (3)0.005 (2)0.002 (2)0.002 (2)
C110.017 (3)0.021 (3)0.015 (3)0.007 (2)0.008 (2)0.007 (2)
C120.022 (3)0.028 (3)0.027 (3)0.010 (3)0.013 (3)0.012 (3)
C130.024 (3)0.022 (3)0.020 (3)0.001 (3)0.005 (3)0.001 (3)
C140.034 (4)0.021 (3)0.021 (3)0.006 (3)0.013 (3)0.001 (3)
C150.030 (4)0.028 (3)0.027 (3)0.015 (3)0.014 (3)0.003 (3)
C160.021 (3)0.025 (3)0.032 (4)0.009 (3)0.009 (3)0.005 (3)
C210.021 (3)0.013 (3)0.018 (3)0.004 (2)0.010 (2)0.002 (2)
C220.025 (3)0.022 (3)0.021 (3)0.010 (3)0.010 (3)0.001 (2)
C230.033 (4)0.018 (3)0.030 (4)0.007 (3)0.019 (3)0.003 (3)
C240.046 (4)0.016 (3)0.024 (3)0.012 (3)0.016 (3)0.006 (3)
C250.034 (4)0.028 (4)0.026 (4)0.013 (3)0.007 (3)0.011 (3)
C260.022 (3)0.019 (3)0.028 (4)0.000 (3)0.007 (3)0.002 (3)
C310.025 (3)0.014 (3)0.018 (3)0.009 (3)0.006 (2)0.004 (2)
C320.023 (3)0.022 (3)0.022 (3)0.007 (3)0.007 (3)0.001 (3)
C330.026 (3)0.025 (3)0.025 (3)0.004 (3)0.009 (3)0.003 (3)
C340.025 (3)0.024 (3)0.026 (4)0.005 (3)0.001 (3)0.009 (3)
C350.031 (4)0.019 (3)0.033 (4)0.007 (3)0.004 (3)0.010 (3)
C360.021 (3)0.024 (3)0.025 (3)0.011 (3)0.004 (3)0.004 (3)
C410.018 (3)0.019 (3)0.020 (3)0.008 (2)0.009 (2)0.007 (2)
C420.031 (4)0.019 (3)0.025 (3)0.011 (3)0.008 (3)0.005 (3)
C430.037 (4)0.030 (4)0.025 (4)0.014 (3)0.007 (3)0.006 (3)
C440.036 (4)0.038 (4)0.017 (3)0.017 (3)0.007 (3)0.009 (3)
C450.038 (4)0.035 (4)0.022 (4)0.020 (3)0.008 (3)0.012 (3)
C460.032 (4)0.021 (3)0.020 (3)0.011 (3)0.004 (3)0.005 (3)
Geometric parameters (Å, º) top
P1—Se12.1093 (19)C23—C241.387 (9)
P2—Se22.1042 (16)C23—H230.9500
P1—C11.814 (6)C24—C251.377 (9)
P1—C211.819 (6)C24—H240.9500
P1—C111.828 (6)C25—C261.394 (9)
P2—C411.814 (6)C25—H250.9500
P2—C311.820 (6)C26—H260.9500
P2—C21.822 (6)C31—C321.389 (8)
C1—C1i1.557 (11)C31—C361.392 (8)
C1—H1A0.9900C32—C331.375 (9)
C1—H1B0.9900C32—H320.9500
C2—C2ii1.544 (11)C33—C341.390 (9)
C2—H2A0.9900C33—H330.9500
C2—H2B0.9900C34—C351.380 (10)
C11—C161.385 (8)C34—H340.9500
C11—C121.388 (8)C35—C361.382 (9)
C12—C131.379 (9)C35—H350.9500
C12—H120.9500C36—H360.9500
C13—C141.369 (9)C41—C461.394 (8)
C13—H130.9500C41—C421.409 (8)
C14—C151.363 (9)C42—C431.387 (9)
C14—H140.9500C42—H420.9500
C15—C161.387 (9)C43—C441.376 (9)
C15—H150.9500C43—H430.9500
C16—H160.9500C44—C451.374 (10)
C21—C261.380 (9)C44—H440.9500
C21—C221.390 (8)C45—C461.375 (9)
C22—C231.399 (9)C45—H450.9500
C22—H220.9500C46—H460.9500
C1—P1—C21105.2 (3)C24—C23—C22120.5 (6)
C1—P1—C11105.5 (3)C24—C23—H23119.7
C21—P1—C11106.3 (2)C22—C23—H23119.7
C1—P1—Se1111.2 (2)C25—C24—C23120.2 (6)
C21—P1—Se1113.4 (2)C25—C24—H24119.9
C11—P1—Se1114.52 (19)C23—C24—H24119.9
C41—P2—C31105.4 (3)C24—C25—C26119.5 (6)
C41—P2—C2106.5 (3)C24—C25—H25120.3
C31—P2—C2103.7 (3)C26—C25—H25120.3
C41—P2—Se2112.92 (19)C21—C26—C25120.7 (6)
C31—P2—Se2114.43 (19)C21—C26—H26119.7
C2—P2—Se2113.1 (2)C25—C26—H26119.7
C1i—C1—P1110.4 (5)C32—C31—C36119.6 (6)
C1i—C1—H1A109.6C32—C31—P2119.4 (4)
P1—C1—H1A109.6C36—C31—P2121.0 (5)
C1i—C1—H1B109.6C33—C32—C31121.0 (6)
P1—C1—H1B109.6C33—C32—H32119.5
H1A—C1—H1B108.1C31—C32—H32119.5
C2ii—C2—P2111.1 (5)C32—C33—C34119.2 (6)
C2ii—C2—H2A109.4C32—C33—H33120.4
P2—C2—H2A109.4C34—C33—H33120.4
C2ii—C2—H2B109.4C35—C34—C33120.2 (6)
P2—C2—H2B109.4C35—C34—H34119.9
H2A—C2—H2B108.0C33—C34—H34119.9
C16—C11—C12119.4 (5)C34—C35—C36120.7 (6)
C16—C11—P1119.5 (4)C34—C35—H35119.7
C12—C11—P1121.1 (4)C36—C35—H35119.7
C13—C12—C11120.4 (6)C35—C36—C31119.4 (6)
C13—C12—H12119.8C35—C36—H36120.3
C11—C12—H12119.8C31—C36—H36120.3
C14—C13—C12119.8 (6)C46—C41—C42119.1 (5)
C14—C13—H13120.1C46—C41—P2120.3 (4)
C12—C13—H13120.1C42—C41—P2120.4 (4)
C15—C14—C13120.3 (6)C43—C42—C41119.3 (6)
C15—C14—H14119.8C43—C42—H42120.4
C13—C14—H14119.8C41—C42—H42120.4
C14—C15—C16120.9 (6)C44—C43—C42120.6 (6)
C14—C15—H15119.6C44—C43—H43119.7
C16—C15—H15119.6C42—C43—H43119.7
C11—C16—C15119.2 (6)C45—C44—C43120.1 (6)
C11—C16—H16120.4C45—C44—H44120.0
C15—C16—H16120.4C43—C44—H44120.0
C26—C21—C22120.1 (5)C44—C45—C46120.7 (6)
C26—C21—P1121.1 (4)C44—C45—H45119.7
C22—C21—P1118.8 (5)C46—C45—H45119.7
C21—C22—C23119.0 (6)C45—C46—C41120.2 (6)
C21—C22—H22120.5C45—C46—H46119.9
C23—C22—H22120.5C41—C46—H46119.9
C21—P1—C1—C1i176.1 (6)C22—C21—C26—C250.5 (9)
C11—P1—C1—C1i64.0 (6)P1—C21—C26—C25178.9 (5)
Se1—P1—C1—C1i60.7 (6)C24—C25—C26—C210.9 (10)
C41—P2—C2—C2ii178.1 (5)C41—P2—C31—C3250.1 (5)
C31—P2—C2—C2ii70.9 (6)C2—P2—C31—C3261.6 (5)
Se2—P2—C2—C2ii53.6 (6)Se2—P2—C31—C32174.8 (4)
C1—P1—C11—C16154.2 (5)C41—P2—C31—C36128.9 (5)
C21—P1—C11—C1694.5 (5)C2—P2—C31—C36119.4 (5)
Se1—P1—C11—C1631.5 (5)Se2—P2—C31—C364.2 (5)
C1—P1—C11—C1227.9 (5)C36—C31—C32—C332.8 (9)
C21—P1—C11—C1283.5 (5)P2—C31—C32—C33176.2 (5)
Se1—P1—C11—C12150.5 (4)C31—C32—C33—C341.9 (10)
C16—C11—C12—C131.9 (9)C32—C33—C34—C350.2 (10)
P1—C11—C12—C13179.9 (5)C33—C34—C35—C360.5 (10)
C11—C12—C13—C140.7 (9)C34—C35—C36—C310.5 (10)
C12—C13—C14—C150.9 (9)C32—C31—C36—C352.1 (9)
C13—C14—C15—C161.3 (10)P2—C31—C36—C35176.9 (5)
C12—C11—C16—C151.5 (9)C31—P2—C41—C4631.2 (5)
P1—C11—C16—C15179.5 (5)C2—P2—C41—C46140.9 (5)
C14—C15—C16—C110.1 (9)Se2—P2—C41—C4694.4 (5)
C1—P1—C21—C2637.1 (5)C31—P2—C41—C42153.9 (5)
C11—P1—C21—C2674.4 (5)C2—P2—C41—C4244.2 (5)
Se1—P1—C21—C26158.9 (4)Se2—P2—C41—C4280.4 (5)
C1—P1—C21—C22142.3 (5)C46—C41—C42—C431.8 (9)
C11—P1—C21—C22106.2 (5)P2—C41—C42—C43176.7 (5)
Se1—P1—C21—C2220.5 (5)C41—C42—C43—C441.0 (10)
C26—C21—C22—C230.0 (8)C42—C43—C44—C450.3 (10)
P1—C21—C22—C23179.4 (4)C43—C44—C45—C460.9 (10)
C21—C22—C23—C240.1 (9)C44—C45—C46—C410.1 (10)
C22—C23—C24—C250.3 (9)C42—C41—C46—C451.2 (9)
C23—C24—C25—C260.7 (9)P2—C41—C46—C45176.2 (5)
Symmetry codes: (i) x, y, z+2; (ii) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15···Se1iii0.953.033.732 (6)132
C25—H25···Se2iv0.953.013.954 (6)171
C14—H14···Se2v0.952.983.690 (7)133
C24—H24···Se2ii0.952.993.751 (6)138
Symmetry codes: (ii) x+1, y+1, z+1; (iii) x+1, y, z+2; (iv) x1, y, z; (v) x+1, y, z+1.

Experimental details

Crystal data
Chemical formulaC26H24P2Se2
Mr556.31
Crystal system, space groupTriclinic, P1
Temperature (K)120
a, b, c (Å)10.322 (2), 10.843 (2), 12.285 (3)
α, β, γ (°)90.93 (3), 108.13 (3), 112.14 (3)
V3)1196.3 (4)
Z2
Radiation typeMo Kα
µ (mm1)3.24
Crystal size (mm)0.10 × 0.10 × 0.05
Data collection
DiffractometerNonius KappaCCD area-detector
Absorption correctionMulti-scan
(XPREP in SHELXTL; Bruker, 2001)
Tmin, Tmax0.738, 0.855
No. of measured, independent and
observed [I > 2σ(I)] reflections
14810, 4095, 3328
Rint0.099
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.160, 1.11
No. of reflections4095
No. of parameters271
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.58, 0.75

Computer programs: COLLECT (Nonius, 1998), DENZO-SMN (Otwinowski & Minor, 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg & Berndt, 1999), WinGX (Farrugia, 1999).

Selected bond lengths (Å) top
P1—Se12.1093 (19)P2—Se22.1042 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15···Se1i0.953.033.732 (6)132
C25—H25···Se2ii0.953.013.954 (6)171
C14—H14···Se2iii0.952.983.690 (7)133
C24—H24···Se2iv0.952.993.751 (6)138
Symmetry codes: (i) x+1, y, z+2; (ii) x1, y, z; (iii) x+1, y, z+1; (iv) x+1, y+1, z+1.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

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