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The crystal structure of the title compound, [(S)-(-)-BINAP] or C44H32P2, is enantiomorphous to the previously reported (R)-(+)-BINAP [Deeming et al. (1997). Organometallics, 16, 6004-6009], with effectively no differences in the molecular geometry apart from being of opposite absolute configuration.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803006019/cf6247sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803006019/cf6247Isup2.hkl
Contains datablock I

CCDC reference: 209977

Key indicators

  • Single-crystal X-ray study
  • T = 180 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.042
  • wR factor = 0.088
  • Data-to-parameter ratio = 12.8

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

REFLT_03 From the CIF: _diffrn_reflns_theta_max 25.06 From the CIF: _reflns_number_total 5303 Count of symmetry unique reflns 3045 Completeness (_total/calc) 174.15% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 2258 Fraction of Friedel pairs measured 0.742 Are heavy atom types Z>Si present yes Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.

Comment top

The ability to selectively form one enantiomer in preference to the other (asymmetric catalysis) is undoubtedly one of the major advances in modern drug design and synthesis. In 2000, the total worldwide sales of single-enantiomer compounds was 123 billion US dollars (Stinson, 2001). In recognition of the outstanding contributions to this field, Noyori received the Nobel Prize for Chemistry in 2001, with much of his work being centred around the different chiral forms of 2,2'-bis(diphenylphosphino)-1,1'-binaphthyl (BINAP) (Noyori, 2002). BINAP is a conformationally flexible atropisometric diphosphine, which is able to coordinate to several transition metal centres, such as rhodium (Ikariya et al., 1985), ruthenium (Touriumi et al., 1982) and palladium (Ozawa et al., 1992). Once BINAP is coordinated, the high steric hindrance around the metal centre affords complexes which are extremely potent for asymmetric hydrogenation (Noyori, 2002). An example of this is the synthesis of (-)-menthol, in which a [Rh-(S)-BINAP] derivative is utilized to induce chirality in the final product. A search in the Cambridge Structural Database (Allen, 2002) reveals that only the (R)-(+)-BINAP crystal structure has been reported so far (Deeming et al., 1997). We report here the structure of the S enantiomer of this renowned organic ligand.

[(S)-(-)-BINAP], (I), crystallizes in the monoclinic space group P21, with one molecule in the asymmetric unit, as depicted in Fig. 1. Individual molecules of (S)-(-)-BINAP are spatially arranged in close packing along the a direction (Figs. 2 and 3). The structures of the R and S enantiomers are essentially the same, except for being of opposite absolute configuration (Deeming et al., 1997).

Experimental top

(S)-(-)-2,2'-Bis(diphenylphosphino)-1,1'-binaphthyl was purchased from Aldrich (99.99% purity). Crystals suitable for X-Ray diffraction analysis were obtained by recrystallization from methanol.

Refinement top

All H atoms were placed in calculated positions and allowed to ride during subsequent refinement, with Uiso(H) = 1.2Ueq(C). A total of 2287 Friedel pairs were used in the refinement.

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXTL (Bruker, 2001); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the labelling scheme for all non-H atoms. Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres.
[Figure 2] Fig. 2. Crystal packing of two (filled and hollow bonds) molecules of (I).
[Figure 3] Fig. 3. Perspective view of the crystal structure of (I) along the c direction.
(S)-(-)-2,2'-Bis(diphenylphosphino)-1,1'-binaphthyl top
Crystal data top
C44H32P2F(000) = 652
Mr = 622.64Dx = 1.244 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 6595 reflections
a = 9.1206 (2) Åθ = 1.0–25.0°
b = 18.7541 (7) ŵ = 0.16 mm1
c = 9.9829 (3) ÅT = 180 K
β = 103.206 (2)°Block, white
V = 1662.40 (9) Å30.23 × 0.21 × 0.16 mm
Z = 2
Data collection top
Nonius KappaCCD
diffractometer
4457 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.043
Thin–slice ω and ϕ scansθmax = 25.1°, θmin = 3.6°
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
h = 1010
Tmin = 0.934, Tmax = 0.981k = 2220
11117 measured reflectionsl = 1111
5303 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.088 w = 1/[σ2(Fo2) + (0.0313P)2 + 0.2494P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
5303 reflectionsΔρmax = 0.22 e Å3
415 parametersΔρmin = 0.28 e Å3
1 restraintAbsolute structure: Flack (1983)
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.04 (8)
Crystal data top
C44H32P2V = 1662.40 (9) Å3
Mr = 622.64Z = 2
Monoclinic, P21Mo Kα radiation
a = 9.1206 (2) ŵ = 0.16 mm1
b = 18.7541 (7) ÅT = 180 K
c = 9.9829 (3) Å0.23 × 0.21 × 0.16 mm
β = 103.206 (2)°
Data collection top
Nonius KappaCCD
diffractometer
5303 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
4457 reflections with I > 2σ(I)
Tmin = 0.934, Tmax = 0.981Rint = 0.043
11117 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.042H-atom parameters constrained
wR(F2) = 0.088Δρmax = 0.22 e Å3
S = 1.04Δρmin = 0.28 e Å3
5303 reflectionsAbsolute structure: Flack (1983)
415 parametersAbsolute structure parameter: 0.04 (8)
1 restraint
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
P10.09925 (8)0.82894 (4)0.86920 (7)0.02977 (19)
P20.04783 (8)0.66685 (4)0.57059 (7)0.02816 (18)
C10.2926 (3)0.80354 (16)0.9502 (3)0.0302 (7)
C20.3464 (3)0.73532 (18)0.9371 (3)0.0394 (8)
H20.27850.69880.89650.047*
C30.4990 (4)0.7200 (2)0.9829 (3)0.0493 (9)
H30.53420.67280.97480.059*
C40.5995 (4)0.7728 (2)1.0399 (3)0.0500 (10)
H40.70350.76211.07160.060*
C50.5478 (3)0.8408 (2)1.0505 (3)0.0467 (9)
H50.61650.87761.08830.056*
C60.3958 (3)0.85620 (18)1.0064 (3)0.0375 (7)
H60.36150.90351.01460.045*
C70.0489 (3)0.88919 (17)0.9967 (3)0.0339 (7)
C80.1054 (4)0.88449 (18)1.1389 (3)0.0437 (8)
H80.17380.84751.17580.052*
C90.0621 (5)0.9335 (2)1.2266 (4)0.0578 (10)
H90.10210.93061.32300.069*
C100.0393 (5)0.9866 (2)1.1729 (5)0.0663 (11)
H100.06861.02031.23280.080*
C110.0982 (4)0.9911 (2)1.0334 (4)0.0596 (10)
H110.16981.02700.99740.071*
C120.0526 (4)0.94328 (18)0.9465 (3)0.0462 (9)
H120.09140.94740.85000.055*
C130.0104 (3)0.74883 (15)0.8877 (2)0.0245 (6)
C140.0144 (3)0.70897 (16)1.0124 (3)0.0295 (7)
H140.09080.72371.08900.035*
C150.0696 (3)0.64987 (16)1.0237 (3)0.0309 (7)
H150.04940.62341.10710.037*
C160.1864 (3)0.62773 (15)0.9125 (3)0.0281 (6)
C170.2770 (3)0.56749 (16)0.9217 (3)0.0349 (7)
H170.25480.53891.00240.042*
C180.3952 (4)0.54979 (17)0.8171 (3)0.0408 (8)
H180.45500.50920.82520.049*
C190.4287 (3)0.59126 (17)0.6976 (3)0.0388 (8)
H190.51340.57950.62600.047*
C200.3412 (3)0.64844 (16)0.6825 (3)0.0324 (7)
H200.36430.67540.59980.039*
C210.2164 (3)0.66799 (16)0.7890 (2)0.0239 (6)
C220.1223 (3)0.72804 (14)0.7773 (2)0.0229 (6)
C230.1477 (3)0.76698 (14)0.6422 (2)0.0233 (6)
C240.2449 (3)0.82725 (16)0.6205 (2)0.0249 (6)
C250.3236 (3)0.85056 (16)0.7199 (3)0.0351 (7)
H250.31550.82400.80230.042*
C260.4107 (4)0.91046 (18)0.6992 (3)0.0446 (8)
H260.46080.92550.76790.054*
C270.4271 (4)0.94995 (19)0.5781 (3)0.0474 (9)
H270.48830.99150.56480.057*
C280.3554 (3)0.92892 (17)0.4792 (3)0.0388 (8)
H280.36720.95610.39710.047*
C290.2636 (3)0.86739 (15)0.4965 (3)0.0277 (6)
C300.1878 (3)0.84407 (16)0.3957 (3)0.0306 (7)
H300.19940.87000.31220.037*
C310.0985 (3)0.78511 (17)0.4164 (3)0.0294 (7)
H310.04990.77030.34650.035*
C320.0766 (3)0.74545 (15)0.5399 (2)0.0253 (6)
C330.0651 (3)0.60013 (16)0.4583 (3)0.0297 (7)
C340.2049 (3)0.61220 (17)0.3717 (3)0.0347 (7)
H340.24770.65860.36530.042*
C350.2830 (3)0.55655 (19)0.2939 (3)0.0425 (8)
H350.37930.56520.23570.051*
C360.2214 (4)0.4891 (2)0.3008 (3)0.0441 (8)
H360.27440.45170.24630.053*
C370.0839 (4)0.47624 (19)0.3862 (3)0.0444 (8)
H370.04180.42970.39190.053*
C380.0060 (4)0.53105 (18)0.4645 (3)0.0373 (8)
H380.08940.52160.52350.045*
C390.1880 (3)0.69237 (17)0.4727 (3)0.0325 (7)
C400.2258 (3)0.64990 (19)0.3711 (3)0.0402 (8)
H400.17460.60610.34590.048*
C410.3385 (4)0.6715 (2)0.3066 (3)0.0521 (9)
H410.36420.64210.23790.062*
C420.4127 (4)0.7349 (2)0.3413 (3)0.0572 (11)
H420.48820.74970.29570.069*
C430.3772 (4)0.7771 (2)0.4427 (4)0.0544 (10)
H430.42850.82090.46740.065*
C440.2663 (3)0.75509 (19)0.5083 (3)0.0437 (8)
H440.24380.78390.57930.052*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
P10.0307 (4)0.0292 (5)0.0286 (4)0.0031 (4)0.0053 (3)0.0013 (3)
P20.0286 (4)0.0299 (4)0.0259 (4)0.0033 (4)0.0063 (3)0.0010 (3)
C10.0281 (16)0.039 (2)0.0238 (14)0.0027 (14)0.0073 (11)0.0003 (12)
C20.0352 (18)0.041 (2)0.0445 (17)0.0017 (15)0.0134 (13)0.0071 (15)
C30.045 (2)0.055 (3)0.052 (2)0.0124 (19)0.0189 (16)0.0026 (17)
C40.0280 (18)0.084 (3)0.0390 (18)0.0053 (19)0.0101 (13)0.0035 (18)
C50.0329 (19)0.069 (3)0.0366 (17)0.0127 (18)0.0046 (13)0.0006 (16)
C60.0365 (18)0.039 (2)0.0350 (16)0.0053 (14)0.0044 (13)0.0009 (13)
C70.0350 (18)0.0294 (19)0.0392 (18)0.0099 (15)0.0124 (13)0.0020 (14)
C80.057 (2)0.035 (2)0.045 (2)0.0091 (17)0.0239 (16)0.0021 (15)
C90.080 (3)0.052 (3)0.052 (2)0.019 (2)0.0369 (19)0.0087 (19)
C100.086 (3)0.045 (3)0.087 (3)0.011 (2)0.060 (2)0.019 (2)
C110.059 (3)0.036 (2)0.092 (3)0.0029 (19)0.035 (2)0.009 (2)
C120.042 (2)0.037 (2)0.060 (2)0.0022 (18)0.0134 (16)0.0012 (17)
C130.0229 (15)0.0253 (16)0.0263 (14)0.0008 (12)0.0074 (11)0.0002 (12)
C140.0271 (15)0.0345 (19)0.0246 (14)0.0008 (14)0.0011 (11)0.0020 (13)
C150.0346 (17)0.033 (2)0.0248 (14)0.0019 (14)0.0062 (11)0.0088 (12)
C160.0288 (16)0.0258 (17)0.0312 (15)0.0044 (13)0.0102 (12)0.0029 (12)
C170.0429 (19)0.0252 (18)0.0368 (16)0.0001 (15)0.0098 (13)0.0089 (13)
C180.044 (2)0.031 (2)0.0467 (19)0.0152 (15)0.0091 (15)0.0021 (15)
C190.0411 (19)0.034 (2)0.0377 (17)0.0099 (15)0.0020 (13)0.0013 (14)
C200.0397 (17)0.031 (2)0.0261 (15)0.0027 (14)0.0059 (12)0.0003 (12)
C210.0254 (14)0.0227 (16)0.0243 (13)0.0039 (13)0.0074 (10)0.0014 (12)
C220.0255 (14)0.0202 (16)0.0238 (13)0.0048 (12)0.0069 (10)0.0013 (11)
C230.0244 (14)0.0219 (17)0.0224 (13)0.0054 (12)0.0029 (10)0.0009 (11)
C240.0224 (14)0.0243 (16)0.0266 (13)0.0031 (13)0.0029 (10)0.0035 (12)
C250.0334 (16)0.039 (2)0.0351 (16)0.0078 (15)0.0117 (13)0.0068 (13)
C260.044 (2)0.046 (2)0.0472 (19)0.0141 (17)0.0167 (15)0.0033 (16)
C270.044 (2)0.039 (2)0.061 (2)0.0193 (17)0.0153 (16)0.0158 (17)
C280.0323 (17)0.039 (2)0.0441 (18)0.0020 (15)0.0060 (13)0.0151 (15)
C290.0232 (15)0.0261 (18)0.0321 (15)0.0027 (13)0.0026 (11)0.0036 (12)
C300.0296 (16)0.035 (2)0.0262 (15)0.0040 (14)0.0034 (11)0.0098 (12)
C310.0307 (17)0.0361 (19)0.0220 (14)0.0039 (14)0.0073 (11)0.0014 (12)
C320.0263 (15)0.0250 (17)0.0237 (14)0.0021 (13)0.0042 (11)0.0009 (12)
C330.0332 (17)0.0297 (19)0.0291 (15)0.0024 (14)0.0131 (12)0.0028 (12)
C340.0325 (17)0.035 (2)0.0359 (16)0.0038 (14)0.0065 (12)0.0022 (14)
C350.0290 (18)0.051 (2)0.0459 (19)0.0031 (17)0.0047 (13)0.0082 (16)
C360.040 (2)0.044 (2)0.0511 (19)0.0089 (17)0.0155 (15)0.0174 (16)
C370.050 (2)0.032 (2)0.0519 (19)0.0018 (16)0.0129 (16)0.0056 (16)
C380.0351 (18)0.038 (2)0.0380 (18)0.0057 (15)0.0060 (13)0.0007 (14)
C390.0232 (15)0.043 (2)0.0289 (15)0.0045 (14)0.0018 (11)0.0066 (13)
C400.0362 (17)0.050 (2)0.0347 (16)0.0063 (16)0.0097 (13)0.0016 (14)
C410.044 (2)0.077 (3)0.0396 (18)0.014 (2)0.0176 (14)0.0061 (19)
C420.0342 (19)0.091 (3)0.050 (2)0.004 (2)0.0150 (15)0.026 (2)
C430.0318 (19)0.063 (3)0.066 (2)0.0096 (18)0.0066 (16)0.014 (2)
C440.0310 (18)0.056 (2)0.0430 (18)0.0065 (17)0.0064 (13)0.0030 (16)
Geometric parameters (Å, º) top
P1—C11.828 (3)C20—H200.950
P1—C131.838 (3)C21—C221.437 (4)
P1—C71.837 (3)C22—C231.504 (3)
P2—C331.832 (3)C23—C321.389 (3)
P2—C391.841 (3)C23—C241.422 (4)
P2—C321.843 (3)C24—C251.420 (4)
C1—C21.387 (4)C24—C291.426 (4)
C1—C61.391 (4)C25—C261.364 (4)
C2—C31.392 (4)C25—H250.950
C2—H20.950C26—C271.396 (4)
C3—C41.381 (5)C26—H260.950
C3—H30.950C27—C281.362 (4)
C4—C51.374 (5)C27—H270.950
C4—H40.950C28—C291.413 (4)
C5—C61.385 (4)C28—H280.950
C5—H50.950C29—C301.413 (4)
C6—H60.950C30—C311.361 (4)
C7—C121.387 (4)C30—H300.950
C7—C81.399 (4)C31—C321.414 (4)
C8—C91.387 (5)C31—H310.950
C8—H80.950C33—C341.385 (4)
C9—C101.381 (6)C33—C381.399 (4)
C9—H90.950C34—C351.395 (4)
C10—C111.376 (5)C34—H340.950
C10—H100.950C35—C361.380 (5)
C11—C121.377 (5)C35—H350.950
C11—H110.950C36—C371.367 (4)
C12—H120.950C36—H360.950
C13—C221.376 (3)C37—C381.385 (4)
C13—C141.425 (4)C37—H370.950
C14—C151.367 (4)C38—H380.950
C14—H140.950C39—C441.380 (4)
C15—C161.414 (4)C39—C401.393 (4)
C15—H150.950C40—C411.392 (4)
C16—C171.415 (4)C40—H400.950
C16—C211.418 (4)C41—C421.372 (5)
C17—C181.360 (4)C41—H410.950
C17—H170.950C42—C431.380 (5)
C18—C191.398 (4)C42—H420.950
C18—H180.950C43—C441.388 (4)
C19—C201.365 (4)C43—H430.950
C19—H190.950C44—H440.950
C20—C211.417 (4)
C1—P1—C13103.59 (13)C13—C22—C21120.3 (2)
C1—P1—C7102.88 (13)C13—C22—C23121.0 (2)
C13—P1—C7101.83 (12)C21—C22—C23118.7 (2)
C33—P2—C39102.39 (13)C32—C23—C24119.9 (2)
C33—P2—C32101.88 (12)C32—C23—C22121.0 (2)
C39—P2—C32100.36 (13)C24—C23—C22119.0 (2)
C2—C1—C6118.2 (3)C25—C24—C23122.4 (2)
C2—C1—P1121.7 (2)C25—C24—C29117.7 (3)
C6—C1—P1119.3 (2)C23—C24—C29119.9 (2)
C1—C2—C3120.5 (3)C26—C25—C24121.1 (3)
C1—C2—H2119.7C26—C25—H25119.4
C3—C2—H2119.7C24—C25—H25119.4
C4—C3—C2120.5 (3)C25—C26—C27120.8 (3)
C4—C3—H3119.8C25—C26—H26119.6
C2—C3—H3119.8C27—C26—H26119.6
C5—C4—C3119.4 (3)C28—C27—C26120.0 (3)
C5—C4—H4120.3C28—C27—H27120.0
C3—C4—H4120.3C26—C27—H27120.0
C4—C5—C6120.4 (3)C27—C28—C29121.2 (3)
C4—C5—H5119.8C27—C28—H28119.4
C6—C5—H5119.8C29—C28—H28119.4
C5—C6—C1121.1 (3)C28—C29—C30122.6 (2)
C5—C6—H6119.5C28—C29—C24119.1 (2)
C1—C6—H6119.5C30—C29—C24118.3 (2)
C12—C7—C8118.3 (3)C31—C30—C29121.1 (2)
C12—C7—P1116.8 (2)C31—C30—H30119.5
C8—C7—P1124.9 (3)C29—C30—H30119.5
C9—C8—C7120.5 (3)C30—C31—C32121.4 (2)
C9—C8—H8119.8C30—C31—H31119.3
C7—C8—H8119.8C32—C31—H31119.3
C10—C9—C8119.6 (3)C23—C32—C31119.4 (2)
C10—C9—H9120.2C23—C32—P2118.93 (19)
C8—C9—H9120.2C31—C32—P2121.6 (2)
C11—C10—C9120.7 (3)C34—C33—C38118.0 (3)
C11—C10—H10119.7C34—C33—P2125.4 (2)
C9—C10—H10119.7C38—C33—P2116.6 (2)
C10—C11—C12119.5 (4)C33—C34—C35120.3 (3)
C10—C11—H11120.2C33—C34—H34119.8
C12—C11—H11120.2C35—C34—H34119.8
C11—C12—C7121.4 (3)C36—C35—C34120.5 (3)
C11—C12—H12119.3C36—C35—H35119.7
C7—C12—H12119.3C34—C35—H35119.7
C22—C13—C14119.5 (3)C37—C36—C35119.9 (3)
C22—C13—P1118.16 (19)C37—C36—H36120.1
C14—C13—P1122.35 (19)C35—C36—H36120.1
C15—C14—C13121.1 (2)C36—C37—C38120.0 (3)
C15—C14—H14119.4C36—C37—H37120.0
C13—C14—H14119.4C38—C37—H37120.0
C14—C15—C16120.6 (2)C37—C38—C33121.3 (3)
C14—C15—H15119.7C37—C38—H38119.4
C16—C15—H15119.7C33—C38—H38119.4
C17—C16—C15122.0 (2)C44—C39—C40118.4 (3)
C17—C16—C21118.8 (2)C44—C39—P2117.8 (2)
C15—C16—C21119.2 (3)C40—C39—P2123.7 (2)
C18—C17—C16121.1 (3)C39—C40—C41120.1 (3)
C18—C17—H17119.4C39—C40—H40119.9
C16—C17—H17119.4C41—C40—H40119.9
C17—C18—C19120.0 (3)C42—C41—C40120.6 (3)
C17—C18—H18120.0C42—C41—H41119.7
C19—C18—H18120.0C40—C41—H41119.7
C20—C19—C18120.7 (3)C41—C42—C43119.8 (3)
C20—C19—H19119.6C41—C42—H42120.1
C18—C19—H19119.6C43—C42—H42120.1
C19—C20—C21120.7 (3)C42—C43—C44119.6 (4)
C19—C20—H20119.6C42—C43—H43120.2
C21—C20—H20119.6C44—C43—H43120.2
C20—C21—C16118.5 (3)C39—C44—C43121.5 (3)
C20—C21—C22122.3 (2)C39—C44—H44119.3
C16—C21—C22119.2 (2)C43—C44—H44119.3
C7—P1—C1—C2143.3 (2)C13—C22—C23—C2487.6 (3)
C13—P1—C1—C237.6 (2)C21—C22—C23—C2492.9 (3)
C7—P1—C1—C647.7 (2)C32—C23—C24—C25178.3 (3)
C13—P1—C1—C6153.5 (2)C22—C23—C24—C252.4 (4)
C6—C1—C2—C31.8 (4)C32—C23—C24—C292.9 (4)
P1—C1—C2—C3170.9 (2)C22—C23—C24—C29176.3 (2)
C1—C2—C3—C41.1 (5)C23—C24—C25—C26177.0 (3)
C2—C3—C4—C50.4 (5)C29—C24—C25—C261.8 (4)
C3—C4—C5—C61.0 (4)C24—C25—C26—C271.1 (5)
C4—C5—C6—C10.2 (4)C25—C26—C27—C280.2 (5)
C2—C1—C6—C51.2 (4)C26—C27—C28—C290.1 (5)
P1—C1—C6—C5170.5 (2)C27—C28—C29—C30179.9 (3)
C1—P1—C7—C12149.1 (2)C27—C28—C29—C240.7 (4)
C13—P1—C7—C12103.8 (2)C25—C24—C29—C281.5 (4)
C1—P1—C7—C830.7 (3)C23—C24—C29—C28177.3 (3)
C13—P1—C7—C876.4 (3)C25—C24—C29—C30179.0 (3)
C12—C7—C8—C90.9 (5)C23—C24—C29—C302.2 (4)
P1—C7—C8—C9178.9 (3)C28—C29—C30—C31179.1 (3)
C7—C8—C9—C101.1 (5)C24—C29—C30—C310.4 (4)
C8—C9—C10—C110.2 (6)C29—C30—C31—C320.8 (4)
C9—C10—C11—C121.6 (6)C24—C23—C32—C311.7 (4)
C10—C11—C12—C71.7 (5)C22—C23—C32—C31177.5 (2)
C8—C7—C12—C110.4 (5)C24—C23—C32—P2179.64 (19)
P1—C7—C12—C11179.7 (3)C22—C23—C32—P21.2 (3)
C1—P1—C13—C22137.7 (2)C30—C31—C32—C230.1 (4)
C7—P1—C13—C22115.8 (2)C30—C31—C32—P2178.5 (2)
C1—P1—C13—C1443.7 (2)C33—P2—C32—C23107.5 (2)
C7—P1—C13—C1462.9 (2)C39—P2—C32—C23147.4 (2)
C22—C13—C14—C150.8 (4)C33—P2—C32—C3174.0 (2)
P1—C13—C14—C15179.5 (2)C39—P2—C32—C3131.2 (2)
C13—C14—C15—C161.6 (4)C39—P2—C33—C34101.1 (3)
C14—C15—C16—C17179.0 (3)C32—P2—C33—C342.4 (3)
C14—C15—C16—C210.5 (4)C39—P2—C33—C3880.8 (2)
C15—C16—C17—C18175.5 (3)C32—P2—C33—C38175.6 (2)
C21—C16—C17—C182.9 (4)C38—C33—C34—C350.1 (4)
C16—C17—C18—C190.2 (5)P2—C33—C34—C35177.9 (2)
C17—C18—C19—C202.0 (5)C33—C34—C35—C360.8 (5)
C18—C19—C20—C211.4 (5)C34—C35—C36—C371.1 (5)
C19—C20—C21—C161.3 (4)C35—C36—C37—C380.7 (5)
C19—C20—C21—C22179.6 (3)C36—C37—C38—C330.0 (5)
C15—C16—C21—C20175.1 (3)C34—C33—C38—C370.3 (4)
C17—C16—C21—C203.4 (4)P2—C33—C38—C37178.5 (2)
C15—C16—C21—C223.3 (4)C33—P2—C39—C44162.8 (2)
C17—C16—C21—C22178.3 (2)C32—P2—C39—C4458.1 (2)
C14—C13—C22—C212.0 (4)C33—P2—C39—C4021.3 (3)
P1—C13—C22—C21176.74 (19)C32—P2—C39—C40126.1 (2)
C14—C13—C22—C23177.5 (2)C44—C39—C40—C411.0 (4)
P1—C13—C22—C233.8 (3)P2—C39—C40—C41176.8 (2)
C20—C21—C22—C13174.3 (3)C39—C40—C41—C420.5 (5)
C16—C21—C22—C134.0 (4)C40—C41—C42—C431.1 (5)
C20—C21—C22—C236.3 (4)C41—C42—C43—C440.2 (5)
C16—C21—C22—C23175.5 (2)C40—C39—C44—C431.9 (4)
C13—C22—C23—C3291.6 (3)P2—C39—C44—C43177.9 (2)
C21—C22—C23—C3287.9 (3)C42—C43—C44—C391.3 (5)

Experimental details

Crystal data
Chemical formulaC44H32P2
Mr622.64
Crystal system, space groupMonoclinic, P21
Temperature (K)180
a, b, c (Å)9.1206 (2), 18.7541 (7), 9.9829 (3)
β (°) 103.206 (2)
V3)1662.40 (9)
Z2
Radiation typeMo Kα
µ (mm1)0.16
Crystal size (mm)0.23 × 0.21 × 0.16
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(SORTAV; Blessing, 1995)
Tmin, Tmax0.934, 0.981
No. of measured, independent and
observed [I > 2σ(I)] reflections
11117, 5303, 4457
Rint0.043
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.042, 0.088, 1.04
No. of reflections5303
No. of parameters415
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.22, 0.28
Absolute structureFlack (1983)
Absolute structure parameter0.04 (8)

Computer programs: COLLECT (Nonius, 1998), HKL SCALEPACK (Otwinowski & Minor, 1997), HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK, SIR92 (Altomare et al., 1994), SHELXTL (Bruker, 2001), SHELXTL.

Selected geometric parameters (Å, º) top
P1—C11.828 (3)P2—C391.841 (3)
P1—C131.838 (3)P2—C321.843 (3)
P1—C71.837 (3)C22—C231.504 (3)
P2—C331.832 (3)
C1—P1—C13103.59 (13)C33—P2—C39102.39 (13)
C1—P1—C7102.88 (13)C33—P2—C32101.88 (12)
C13—P1—C7101.83 (12)C39—P2—C32100.36 (13)
 

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