Abstract
In the title molecule, C26H22P2Se2, both P atoms have distorted tetrahedral environments, resulting in effective cone angles of 177 and 174°. Inversion twinning was detected and refined to a ratio of 0.35:0.65. Weak intermolecular C—H⋯Se interactions are observed.
Related literature
For background to the steric and electronic effects of group 15 ligands, see: Roodt et al. (2003 ▶); Muller et al. (2008 ▶). For information on cone angles, see: Tolman (1977 ▶); Otto (2001 ▶).
Experimental
Crystal data
C26H22P2Se2
M r = 554.3
Orthorhombic,
a = 9.0604 (9) Å
b = 14.3239 (14) Å
c = 17.9617 (18) Å
V = 2331.1 (4) Å3
Z = 4
Mo Kα radiation
μ = 3.32 mm−1
T = 100 K
0.26 × 0.21 × 0.04 mm
Data collection
Bruker APEX DUO 4K CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2008 ▶) T min = 0.479, T max = 0.879
14567 measured reflections
5814 independent reflections
5356 reflections with I > 2σ(I)
R int = 0.028
Refinement
R[F 2 > 2σ(F 2)] = 0.025
wR(F 2) = 0.053
S = 1.01
5814 reflections
272 parameters
H-atom parameters constrained
Δρmax = 0.51 e Å−3
Δρmin = −0.48 e Å−3
Absolute structure: Flack (1983 ▶), 2517 Friedel pairs
Flack parameter: 0.354 (6)
Data collection: APEX2 (Bruker, 2011 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT and XPREP (Bruker, 2008 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 2005 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681105183X/fj2485sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681105183X/fj2485Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C3—H3⋯Se2i | 0.95 | 3.02 | 3.953 (2) | 168 |
| C21—H21⋯Se1ii | 0.95 | 3.06 | 3.812 (2) | 138 |
| C17—H17⋯Se2iii | 0.95 | 3.01 | 3.885 (3) | 155 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
Research funds of the University of Johannesburg are gratefully acknowledged.
supplementary crystallographic information
Comment
The study of the transition metal phosphorous bond spans over several decades using various techniques such as crystallography, multi nuclear NMR and IR (Roodt et al., 2003). As part of this systematic investigation we have extended this study to selenium derivatives of the phosphorus ligands (see Muller et al., 2008). Reported as part of the above continuing study, the single-crystal structure of the bis-phosphorus containing compound, (SePPh2)2C2H2 where Ph = C6H5, is reported here.
The structure of the title compound (see Figure 1, Table 1) shows distorted tetrahedral environments for both the phosphorus centers. The P═Se bond distances (2.1026 (6), 2.1054 (6) Å for Se1 and Se2 respectively) are marginally statistically different, possibly due to the weak C—H···Se intermolecular hydrogen bonding observed (see Figure 2, Table 2; comparison based on 1% normal distribution coefficient).
The phosphorus ligand bulkiness was evaluated by using an adaptation of the well known Tolman cone angle model (Tolman, 1977). Instead of using a CPK model, the actual geometry from the crystal structure was taken to determine an 'effective cone angle' (Otto et al. 2001). The Se═P distances were also adjusted to 2.28 Å (the default value used by Tolman) to remove the effect of bond distance variation. Two different cone angles of 177° and 174° were obtained for P1and P2 respectively. The difference in cone angles may also be attributed to the weak interactions mentioned previously.
Experimental
Trans-1,2-bis(diphenylphosphino)ethylene and KSeCN were purchased from Sigma-Aldrich and used without purification. Eqimolar amounts of KSeCN and the trans-1,2-bis(diphenylphosphino)ethylene compound (ca 0.04 mmol) were dissolved in the minimum amounts of methanol (10 - 20 ml). The KSeCN solution was added drop wise (5 min.) to the phosphine solution with stirring at room temperature. The final solution was left to evaporate slowly until dry to give crystals suitable for a single-crystal X-ray study.
Refinement
All hydrogen atoms were positioned in geometrically idealized positions with C—H = 0.95 Å and allowed to ride on their parent atoms with Uiso(H) = 1.2Ueq. The Flack parameter (based on 2517 Friedel pairs) indicates racemic twinning of the compound. This refined to a 35.4:64.6 racemic twin. The highest residual electron density of 0.51 e.Å-3 is 0.98 Å from Se1 representing no physical meaning.
Figures
Fig. 1.
: View of the title compound indicating labelling and displacement ellipsoids (drawn at a 50% probability level).
Fig. 2.
: Partial packing diagram of the title compound illustrating the weak C–H···Se interactions stabilizing the crystal packing.
Crystal data
| C26H22P2Se2 | F(000) = 1104 |
| Mr = 554.3 | Dx = 1.579 Mg m−3 |
| Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2ac 2ab | Cell parameters from 5956 reflections |
| a = 9.0604 (9) Å | θ = 2.3–28.2° |
| b = 14.3239 (14) Å | µ = 3.32 mm−1 |
| c = 17.9617 (18) Å | T = 100 K |
| V = 2331.1 (4) Å3 | Plate, colourless |
| Z = 4 | 0.26 × 0.21 × 0.04 mm |
Data collection
| Bruker APEX DUO 4K CCD diffractometer | 5814 independent reflections |
| graphite | 5356 reflections with I > 2σ(I) |
| Detector resolution: 8.4 pixels mm-1 | Rint = 0.028 |
| φ and ω scans | θmax = 28.5°, θmin = 1.8° |
| Absorption correction: multi-scan (SADABS; Bruker, 2008) | h = −10→12 |
| Tmin = 0.479, Tmax = 0.879 | k = −12→19 |
| 14567 measured reflections | l = −24→22 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.025 | H-atom parameters constrained |
| wR(F2) = 0.053 | w = 1/[σ2(Fo2) + (0.0268P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.01 | (Δ/σ)max = 0.001 |
| 5814 reflections | Δρmax = 0.51 e Å−3 |
| 272 parameters | Δρmin = −0.48 e Å−3 |
| 0 restraints | Absolute structure: Flack (1983), 2517 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.354 (6) |
Special details
| Experimental. The intensity data was collected on a Bruker Apex DUO 4 K CCD diffractometer using an exposure time of 20 s/frame. A total of 588 frames were collected with a frame width of 0.5° covering up to θ = 28.49° with 99.2% completeness accomplished.Analytical data: 1H NMR (CDCl3, 400 MHz) δ 7.50–7.70 (m, 10H), 7.51–7.42 (m, 10H), 7.89 (t, 3J = 22.8 Hz, 2H); 13C {H} NMR (CDCl3, 100 MHz) δ 142.4 (ethylene), 132.1, 131.8, 129.0 (Ar); 31P {H} NMR (CDCl3, 160 MHz):δ = 28.58 (dd, 1JSe—P = 694.9, 814.8 Hz, 2P). |
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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)
| x | y | z | Uiso*/Ueq | ||
| C1 | 1.0685 (2) | 0.72411 (15) | 0.64399 (13) | 0.0134 (4) | |
| C2 | 1.0826 (3) | 0.62874 (15) | 0.62917 (14) | 0.0185 (5) | |
| H2 | 0.9975 | 0.5921 | 0.619 | 0.022* | |
| C3 | 1.2215 (3) | 0.58774 (15) | 0.62938 (15) | 0.0226 (5) | |
| H3 | 1.231 | 0.5228 | 0.6198 | 0.027* | |
| C4 | 1.3460 (3) | 0.64076 (16) | 0.64339 (15) | 0.0197 (5) | |
| H4 | 1.4407 | 0.6123 | 0.6434 | 0.024* | |
| C5 | 1.3321 (3) | 0.73551 (16) | 0.65749 (14) | 0.0186 (5) | |
| H5 | 1.4175 | 0.7721 | 0.6668 | 0.022* | |
| C6 | 1.1940 (3) | 0.77686 (15) | 0.65806 (13) | 0.0173 (5) | |
| H6 | 1.185 | 0.8417 | 0.6681 | 0.021* | |
| C7 | 0.9158 (2) | 0.89938 (15) | 0.62504 (14) | 0.0158 (5) | |
| C8 | 0.9380 (3) | 0.92399 (16) | 0.55117 (14) | 0.0198 (5) | |
| H8 | 0.939 | 0.8771 | 0.5138 | 0.024* | |
| C9 | 0.9588 (3) | 1.01653 (18) | 0.53168 (17) | 0.0265 (6) | |
| H9 | 0.9743 | 1.033 | 0.481 | 0.032* | |
| C10 | 0.9571 (3) | 1.08522 (17) | 0.58612 (17) | 0.0278 (6) | |
| H10 | 0.9707 | 1.1488 | 0.5726 | 0.033* | |
| C11 | 0.9357 (3) | 1.06180 (17) | 0.65944 (18) | 0.0282 (6) | |
| H11 | 0.935 | 1.1091 | 0.6965 | 0.034* | |
| C12 | 0.9150 (3) | 0.96844 (16) | 0.67974 (16) | 0.0221 (5) | |
| H12 | 0.9004 | 0.9522 | 0.7305 | 0.027* | |
| C13 | 0.4690 (2) | 0.81404 (15) | 0.84948 (14) | 0.0156 (5) | |
| C14 | 0.4717 (3) | 0.90052 (16) | 0.81243 (15) | 0.0212 (5) | |
| H14 | 0.5622 | 0.9242 | 0.7935 | 0.025* | |
| C15 | 0.3430 (3) | 0.95120 (17) | 0.80341 (16) | 0.0252 (6) | |
| H15 | 0.3451 | 1.0095 | 0.7782 | 0.03* | |
| C16 | 0.2105 (3) | 0.91681 (17) | 0.83126 (15) | 0.0250 (6) | |
| H16 | 0.1221 | 0.9516 | 0.825 | 0.03* | |
| C17 | 0.2075 (3) | 0.83228 (17) | 0.86790 (15) | 0.0244 (5) | |
| H17 | 0.1169 | 0.8088 | 0.8869 | 0.029* | |
| C18 | 0.3369 (3) | 0.78136 (17) | 0.87717 (14) | 0.0211 (5) | |
| H18 | 0.3343 | 0.7234 | 0.9029 | 0.025* | |
| C19 | 0.5966 (2) | 0.63390 (15) | 0.88948 (14) | 0.0145 (5) | |
| C20 | 0.6670 (3) | 0.59705 (15) | 0.95104 (14) | 0.0192 (5) | |
| H20 | 0.737 | 0.6336 | 0.9775 | 0.023* | |
| C21 | 0.6355 (3) | 0.50619 (16) | 0.97447 (16) | 0.0245 (6) | |
| H21 | 0.6852 | 0.4806 | 1.0164 | 0.029* | |
| C22 | 0.5324 (3) | 0.45375 (16) | 0.93677 (16) | 0.0230 (6) | |
| H22 | 0.5092 | 0.3925 | 0.9534 | 0.028* | |
| C23 | 0.4621 (3) | 0.49016 (17) | 0.87437 (17) | 0.0243 (6) | |
| H23 | 0.3923 | 0.4535 | 0.8479 | 0.029* | |
| C24 | 0.4944 (3) | 0.58029 (17) | 0.85093 (16) | 0.0214 (5) | |
| H24 | 0.4464 | 0.6053 | 0.8084 | 0.026* | |
| C25 | 0.7048 (2) | 0.74177 (14) | 0.76513 (12) | 0.0142 (4) | |
| H25 | 0.6431 | 0.711 | 0.7301 | 0.017* | |
| C26 | 0.8328 (2) | 0.77552 (14) | 0.74213 (13) | 0.0147 (4) | |
| H26 | 0.8992 | 0.8002 | 0.778 | 0.018* | |
| P1 | 0.88646 (6) | 0.77673 (4) | 0.64539 (3) | 0.01278 (11) | |
| P2 | 0.64250 (6) | 0.75184 (4) | 0.86038 (3) | 0.01338 (12) | |
| Se1 | 0.73133 (2) | 0.712573 (15) | 0.574954 (15) | 0.01794 (6) | |
| Se2 | 0.79614 (2) | 0.821665 (14) | 0.928447 (14) | 0.01582 (5) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0146 (10) | 0.0147 (10) | 0.0108 (10) | 0.0023 (8) | 0.0025 (9) | 0.0012 (8) |
| C2 | 0.0186 (11) | 0.0144 (11) | 0.0226 (14) | −0.0001 (9) | 0.0022 (11) | −0.0013 (9) |
| C3 | 0.0248 (12) | 0.0135 (11) | 0.0295 (14) | 0.0039 (9) | 0.0034 (12) | −0.0008 (9) |
| C4 | 0.0178 (11) | 0.0191 (11) | 0.0224 (13) | 0.0056 (9) | −0.0008 (11) | 0.0032 (10) |
| C5 | 0.0155 (11) | 0.0190 (11) | 0.0213 (13) | −0.0012 (9) | −0.0027 (10) | −0.0005 (9) |
| C6 | 0.0200 (11) | 0.0127 (10) | 0.0193 (12) | 0.0014 (9) | 0.0001 (10) | −0.0049 (9) |
| C7 | 0.0123 (10) | 0.0174 (11) | 0.0178 (13) | 0.0019 (8) | −0.0017 (10) | 0.0017 (9) |
| C8 | 0.0250 (12) | 0.0168 (11) | 0.0176 (13) | 0.0007 (10) | −0.0004 (11) | 0.0001 (9) |
| C9 | 0.0265 (14) | 0.0257 (14) | 0.0274 (16) | −0.0004 (11) | 0.0010 (13) | 0.0078 (11) |
| C10 | 0.0263 (12) | 0.0147 (12) | 0.0423 (19) | −0.0005 (9) | −0.0028 (14) | 0.0064 (11) |
| C11 | 0.0316 (14) | 0.0149 (12) | 0.0379 (18) | 0.0000 (11) | −0.0067 (14) | −0.0048 (11) |
| C12 | 0.0249 (12) | 0.0184 (11) | 0.0230 (14) | 0.0000 (10) | −0.0028 (12) | −0.0010 (10) |
| C13 | 0.0182 (10) | 0.0151 (11) | 0.0136 (11) | 0.0030 (9) | 0.0024 (10) | −0.0028 (9) |
| C14 | 0.0209 (12) | 0.0174 (12) | 0.0252 (14) | −0.0010 (9) | −0.0023 (11) | 0.0023 (10) |
| C15 | 0.0269 (13) | 0.0172 (11) | 0.0317 (16) | 0.0059 (10) | −0.0039 (12) | 0.0034 (10) |
| C16 | 0.0239 (12) | 0.0254 (12) | 0.0259 (14) | 0.0100 (11) | −0.0037 (12) | −0.0062 (10) |
| C17 | 0.0193 (11) | 0.0306 (13) | 0.0232 (14) | 0.0027 (11) | 0.0034 (12) | 0.0003 (10) |
| C18 | 0.0241 (12) | 0.0227 (12) | 0.0165 (12) | 0.0032 (10) | 0.0061 (11) | 0.0039 (10) |
| C19 | 0.0153 (10) | 0.0114 (11) | 0.0168 (12) | 0.0026 (8) | 0.0044 (10) | −0.0009 (9) |
| C20 | 0.0184 (11) | 0.0187 (11) | 0.0206 (13) | −0.0023 (9) | 0.0001 (10) | 0.0001 (9) |
| C21 | 0.0328 (14) | 0.0183 (12) | 0.0225 (15) | 0.0018 (11) | −0.0029 (12) | 0.0048 (10) |
| C22 | 0.0283 (12) | 0.0149 (11) | 0.0257 (15) | −0.0027 (9) | 0.0049 (12) | 0.0054 (11) |
| C23 | 0.0233 (12) | 0.0208 (12) | 0.0288 (16) | −0.0062 (10) | 0.0010 (12) | −0.0026 (11) |
| C24 | 0.0216 (12) | 0.0219 (12) | 0.0207 (13) | −0.0009 (9) | −0.0024 (11) | 0.0029 (10) |
| C25 | 0.0189 (10) | 0.0106 (9) | 0.0130 (11) | 0.0014 (9) | 0.0008 (10) | 0.0000 (8) |
| C26 | 0.0165 (10) | 0.0135 (10) | 0.0140 (11) | 0.0019 (8) | −0.0014 (9) | −0.0001 (8) |
| P1 | 0.0135 (2) | 0.0126 (3) | 0.0122 (3) | 0.0001 (2) | 0.0011 (2) | −0.0005 (2) |
| P2 | 0.0148 (3) | 0.0124 (3) | 0.0130 (3) | 0.0017 (2) | 0.0019 (2) | 0.0009 (2) |
| Se1 | 0.01645 (10) | 0.01938 (11) | 0.01798 (12) | −0.00169 (8) | −0.00126 (11) | −0.00443 (9) |
| Se2 | 0.01802 (10) | 0.01372 (10) | 0.01572 (11) | 0.00030 (8) | 0.00040 (11) | −0.00065 (9) |
Geometric parameters (Å, °)
| C1—C6 | 1.388 (3) | C14—H14 | 0.95 |
| C1—C2 | 1.398 (3) | C15—C16 | 1.391 (4) |
| C1—P1 | 1.813 (2) | C15—H15 | 0.95 |
| C2—C3 | 1.389 (3) | C16—C17 | 1.378 (4) |
| C2—H2 | 0.95 | C16—H16 | 0.95 |
| C3—C4 | 1.383 (3) | C17—C18 | 1.391 (3) |
| C3—H3 | 0.95 | C17—H17 | 0.95 |
| C4—C5 | 1.386 (3) | C18—H18 | 0.95 |
| C4—H4 | 0.95 | C19—C20 | 1.381 (3) |
| C5—C6 | 1.384 (3) | C19—C24 | 1.388 (3) |
| C5—H5 | 0.95 | C19—P2 | 1.817 (2) |
| C6—H6 | 0.95 | C20—C21 | 1.397 (3) |
| C7—C8 | 1.387 (3) | C20—H20 | 0.95 |
| C7—C12 | 1.394 (3) | C21—C22 | 1.377 (4) |
| C7—P1 | 1.814 (2) | C21—H21 | 0.95 |
| C8—C9 | 1.384 (3) | C22—C23 | 1.391 (4) |
| C8—H8 | 0.95 | C22—H22 | 0.95 |
| C9—C10 | 1.387 (4) | C23—C24 | 1.389 (3) |
| C9—H9 | 0.95 | C23—H23 | 0.95 |
| C10—C11 | 1.373 (4) | C24—H24 | 0.95 |
| C10—H10 | 0.95 | C25—C26 | 1.322 (3) |
| C11—C12 | 1.399 (3) | C25—P2 | 1.807 (2) |
| C11—H11 | 0.95 | C25—H25 | 0.95 |
| C12—H12 | 0.95 | C26—P1 | 1.804 (2) |
| C13—C18 | 1.377 (3) | C26—H26 | 0.95 |
| C13—C14 | 1.406 (3) | P1—Se1 | 2.1026 (6) |
| C13—P2 | 1.818 (2) | P2—Se2 | 2.1054 (6) |
| C14—C15 | 1.383 (3) | ||
| C6—C1—C2 | 119.4 (2) | C17—C16—C15 | 120.0 (2) |
| C6—C1—P1 | 121.07 (16) | C17—C16—H16 | 120 |
| C2—C1—P1 | 119.47 (17) | C15—C16—H16 | 120 |
| C3—C2—C1 | 119.7 (2) | C16—C17—C18 | 120.1 (2) |
| C3—C2—H2 | 120.1 | C16—C17—H17 | 120 |
| C1—C2—H2 | 120.1 | C18—C17—H17 | 120 |
| C4—C3—C2 | 120.5 (2) | C13—C18—C17 | 120.7 (2) |
| C4—C3—H3 | 119.8 | C13—C18—H18 | 119.6 |
| C2—C3—H3 | 119.8 | C17—C18—H18 | 119.6 |
| C3—C4—C5 | 119.8 (2) | C20—C19—C24 | 119.7 (2) |
| C3—C4—H4 | 120.1 | C20—C19—P2 | 118.68 (18) |
| C5—C4—H4 | 120.1 | C24—C19—P2 | 121.57 (19) |
| C6—C5—C4 | 120.1 (2) | C19—C20—C21 | 120.2 (2) |
| C6—C5—H5 | 119.9 | C19—C20—H20 | 119.9 |
| C4—C5—H5 | 119.9 | C21—C20—H20 | 119.9 |
| C5—C6—C1 | 120.40 (19) | C22—C21—C20 | 119.9 (2) |
| C5—C6—H6 | 119.8 | C22—C21—H21 | 120 |
| C1—C6—H6 | 119.8 | C20—C21—H21 | 120 |
| C8—C7—C12 | 119.6 (2) | C21—C22—C23 | 120.2 (2) |
| C8—C7—P1 | 117.39 (19) | C21—C22—H22 | 119.9 |
| C12—C7—P1 | 123.0 (2) | C23—C22—H22 | 119.9 |
| C9—C8—C7 | 120.3 (2) | C24—C23—C22 | 119.8 (2) |
| C9—C8—H8 | 119.8 | C24—C23—H23 | 120.1 |
| C7—C8—H8 | 119.8 | C22—C23—H23 | 120.1 |
| C8—C9—C10 | 120.0 (3) | C19—C24—C23 | 120.2 (3) |
| C8—C9—H9 | 120 | C19—C24—H24 | 119.9 |
| C10—C9—H9 | 120 | C23—C24—H24 | 119.9 |
| C11—C10—C9 | 120.3 (2) | C26—C25—P2 | 122.73 (18) |
| C11—C10—H10 | 119.8 | C26—C25—H25 | 118.6 |
| C9—C10—H10 | 119.8 | P2—C25—H25 | 118.6 |
| C10—C11—C12 | 120.2 (3) | C25—C26—P1 | 122.73 (18) |
| C10—C11—H11 | 119.9 | C25—C26—H26 | 118.6 |
| C12—C11—H11 | 119.9 | P1—C26—H26 | 118.6 |
| C7—C12—C11 | 119.6 (3) | C26—P1—C1 | 104.75 (11) |
| C7—C12—H12 | 120.2 | C26—P1—C7 | 104.06 (11) |
| C11—C12—H12 | 120.2 | C1—P1—C7 | 105.45 (10) |
| C18—C13—C14 | 119.0 (2) | C26—P1—Se1 | 113.27 (8) |
| C18—C13—P2 | 123.07 (18) | C1—P1—Se1 | 114.70 (8) |
| C14—C13—P2 | 117.87 (18) | C7—P1—Se1 | 113.58 (8) |
| C15—C14—C13 | 120.2 (2) | C25—P2—C19 | 105.65 (10) |
| C15—C14—H14 | 119.9 | C25—P2—C13 | 101.97 (11) |
| C13—C14—H14 | 119.9 | C19—P2—C13 | 106.79 (11) |
| C14—C15—C16 | 120.0 (2) | C25—P2—Se2 | 112.39 (8) |
| C14—C15—H15 | 120 | C19—P2—Se2 | 115.22 (8) |
| C16—C15—H15 | 120 | C13—P2—Se2 | 113.68 (8) |
| C6—C1—C2—C3 | 0.6 (4) | P2—C25—C26—P1 | −173.15 (11) |
| P1—C1—C2—C3 | −178.8 (2) | C25—C26—P1—C1 | −129.02 (19) |
| C1—C2—C3—C4 | −0.7 (4) | C25—C26—P1—C7 | 120.51 (19) |
| C2—C3—C4—C5 | 0.1 (4) | C25—C26—P1—Se1 | −3.3 (2) |
| C3—C4—C5—C6 | 0.4 (4) | C6—C1—P1—C26 | −84.4 (2) |
| C4—C5—C6—C1 | −0.5 (4) | C2—C1—P1—C26 | 95.0 (2) |
| C2—C1—C6—C5 | 0.0 (4) | C6—C1—P1—C7 | 25.1 (2) |
| P1—C1—C6—C5 | 179.38 (19) | C2—C1—P1—C7 | −155.5 (2) |
| C12—C7—C8—C9 | −0.2 (4) | C6—C1—P1—Se1 | 150.79 (18) |
| P1—C7—C8—C9 | 179.00 (19) | C2—C1—P1—Se1 | −29.8 (2) |
| C7—C8—C9—C10 | −0.2 (4) | C8—C7—P1—C26 | −170.97 (19) |
| C8—C9—C10—C11 | 0.4 (4) | C12—C7—P1—C26 | 8.2 (2) |
| C9—C10—C11—C12 | −0.2 (4) | C8—C7—P1—C1 | 79.1 (2) |
| C8—C7—C12—C11 | 0.4 (4) | C12—C7—P1—C1 | −101.8 (2) |
| P1—C7—C12—C11 | −178.79 (19) | C8—C7—P1—Se1 | −47.3 (2) |
| C10—C11—C12—C7 | −0.2 (4) | C12—C7—P1—Se1 | 131.83 (19) |
| C18—C13—C14—C15 | −0.7 (4) | C26—C25—P2—C19 | −126.76 (19) |
| P2—C13—C14—C15 | −179.2 (2) | C26—C25—P2—C13 | 121.8 (2) |
| C13—C14—C15—C16 | 0.2 (4) | C26—C25—P2—Se2 | −0.3 (2) |
| C14—C15—C16—C17 | 0.1 (4) | C20—C19—P2—C25 | 122.47 (19) |
| C15—C16—C17—C18 | 0.1 (4) | C24—C19—P2—C25 | −56.8 (2) |
| C14—C13—C18—C17 | 0.9 (4) | C20—C19—P2—C13 | −129.50 (19) |
| P2—C13—C18—C17 | 179.33 (19) | C24—C19—P2—C13 | 51.2 (2) |
| C16—C17—C18—C13 | −0.6 (4) | C20—C19—P2—Se2 | −2.2 (2) |
| C24—C19—C20—C21 | 0.0 (4) | C24—C19—P2—Se2 | 178.50 (18) |
| P2—C19—C20—C21 | −179.30 (19) | C18—C13—P2—C25 | 125.2 (2) |
| C19—C20—C21—C22 | −1.0 (4) | C14—C13—P2—C25 | −56.3 (2) |
| C20—C21—C22—C23 | 1.6 (4) | C18—C13—P2—C19 | 14.6 (3) |
| C21—C22—C23—C24 | −1.1 (4) | C14—C13—P2—C19 | −166.89 (19) |
| C20—C19—C24—C23 | 0.4 (4) | C18—C13—P2—Se2 | −113.6 (2) |
| P2—C19—C24—C23 | 179.7 (2) | C14—C13—P2—Se2 | 64.9 (2) |
| C22—C23—C24—C19 | 0.1 (4) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C3—H3···Se2i | 0.95 | 3.02 | 3.953 (2) | 168 |
| C21—H21···Se1ii | 0.95 | 3.06 | 3.812 (2) | 138 |
| C17—H17···Se2iii | 0.95 | 3.01 | 3.885 (3) | 155 |
Symmetry codes: (i) −x+2, y−1/2, −z+3/2; (ii) −x+3/2, −y+1, z+1/2; (iii) x−1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2485).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681105183X/fj2485sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681105183X/fj2485Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


