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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 May 31;70(Pt 6):m237. doi: 10.1107/S1600536814011945

Bis{μ-[(di­phenyl­phosphor­yl)meth­yl](phen­yl)bis­(1H-pyrazol-1-yl)boranuido}dilithium

Manuela Müller a, Hans-Wolfram Lerner a, Michael Bolte a,*
PMCID: PMC4051015  PMID: 24940216

Abstract

The title compound, [Li2(C25H23BN4OP)2], features a centrosymmetric dimeric complex. The four-memberered Li2O2 ring is exactly planar due to symmetry. The Li atom is four-coordinated by two O atoms and by two N atoms of two different pyrazole rings. The dihedral angle between two pyrazole rings bonded to the same B atom is 45.66 (9)°. The B—N—N—Li—N—N metalla ring adopts a boat conformation. The crystal packing is stabilized by van der Waals inter­actions only.

Related literature  

For background to scorpionates, see: Trofimenko (1993, 1999); Bieller et al. (2006). For related structures, see: Müller et al. (2014a ,b ).graphic file with name e-70-0m237-scheme1.jpg

Experimental  

Crystal data  

  • [Li2(C25H23BN4OP)2]

  • M r = 888.39

  • Monoclinic, Inline graphic

  • a = 10.0585 (6) Å

  • b = 16.2371 (8) Å

  • c = 14.4301 (8) Å

  • β = 98.854 (5)°

  • V = 2328.7 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.14 mm−1

  • T = 173 K

  • 0.32 × 0.28 × 0.27 mm

Data collection  

  • Stoe IPDS II two-circle diffractometer

  • Absorption correction: multi-scan (MULABS; Spek, 2009; Blessing, 1995) T min = 0.956, T max = 0.962

  • 36952 measured reflections

  • 4362 independent reflections

  • 3630 reflections with I > 2σ(I)

  • R int = 0.062

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.101

  • S = 1.02

  • 4362 reflections

  • 298 parameters

  • H-atom parameters constrained

  • Δρmax = 0.36 e Å−3

  • Δρmin = −0.29 e Å−3

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536814011945/sj5403sup1.cif

e-70-0m237-sup1.cif (34.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814011945/sj5403Isup2.hkl

e-70-0m237-Isup2.hkl (213.8KB, hkl)

CCDC reference: 883935

Additional supporting information: crystallographic information; 3D view; checkCIF report

supplementary crystallographic information

1. Comment

One way to alter the donor/acceptor properties of scorpionate ligands over a wider range is to replace the pyrazolyl rings by phosphorus-containing groups (Trofimenko, 1993; Trofimenko, 1999; Bieller et al., 2006). Similar to parent scorpionates these ligands provide a monoanionic, tridentate, face-capping coordination mode, but they differ from parent scorpionates with regard to the softness of their donor sets. Recently we have investigated the syntheses of the hybrid scorpionates Li(tmeda)[PhBpz2(CH2PPh2)] (I) and Li(tmeda)2[PhB(CH2PPh2)3] (II) (Müller et al., 2014a). The lithium scorpionates I and II, however, are air-sensitive. The heteroscorpionates I and II react with oxygen from the air to give the corresponding oxo-heteroscorpionates as shown in the scheme (Fig. 1). After storing solutions of I and II under ambient conditions (in the presence of oxygen from the air) crystals of the oxo-heteroscorpionates III and IV could be isolated (Müller et al., 2014b).

The title compound features a centrosymmetric dimeric complex (Fig. 2). The four-memberered Li2O2 ring is exactly planar due to the symmetry. Each Li centre is four-coordinated by two oxygen atoms and two nitrogen atoms of two different pyrazol rings. The dihedral angle between two pyrazol rings bonded to the same boron atom is 45.66 (9)°. The B—N—N—Li—N—N ring adopts a boat conformation. The crystal packing is stabilized only by van der Waals interactions (Fig. 3).

2. Experimental

Single crystals of the oxo-scorpionate III were grown from a thf solution of I in the presence of air oxygen at r.t.

3. Refinement

H atoms were refined using a riding model, with Caromatic —H = 0.95 Å or Cmethylene —H = 0.99 Å and with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

Oxidation of diphenylphosphanylmethyl-substituted heteroscorpionates Li[PhBpzn(CH2PPh2)3-n] (n = 2, 0) with O2.

Fig. 2.

Fig. 2.

Perspective view of the title compound with displacement ellipsoids drawn at the 50% probability level. Hydrogen atoms omitted for clarity.

Fig. 3.

Fig. 3.

Packing diagram of the title compound with view onto the bc plane. Hydrogen atoms omitted for clarity.

Crystal data

[Li2(C25H23BN4OP)2] F(000) = 928
Mr = 888.39 Dx = 1.267 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 30927 reflections
a = 10.0585 (6) Å θ = 3.5–25.8°
b = 16.2371 (8) Å µ = 0.14 mm1
c = 14.4301 (8) Å T = 173 K
β = 98.854 (5)° Block, colourless
V = 2328.7 (2) Å3 0.32 × 0.28 × 0.27 mm
Z = 2

Data collection

Stoe IPDS II two-circle diffractometer 4362 independent reflections
Radiation source: fine-focus sealed tube 3630 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.062
ω scans θmax = 25.6°, θmin = 3.5°
Absorption correction: multi-scan (MULABS; Spek, 2009; Blessing, 1995) h = −12→12
Tmin = 0.956, Tmax = 0.962 k = −19→19
36952 measured reflections l = −17→16

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.101 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0511P)2 + 0.9981P] where P = (Fo2 + 2Fc2)/3
4362 reflections (Δ/σ)max = 0.001
298 parameters Δρmax = 0.36 e Å3
0 restraints Δρmin = −0.29 e Å3

Special details

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)

x y z Uiso*/Ueq
P1 0.77171 (4) 0.58856 (2) 0.40685 (3) 0.02091 (12)
O1 0.87612 (11) 0.53113 (7) 0.45806 (8) 0.0246 (3)
Li1 1.0357 (3) 0.57250 (17) 0.5403 (2) 0.0276 (6)
B1 0.85890 (18) 0.73774 (11) 0.52436 (13) 0.0222 (4)
C1 0.73591 (16) 0.67798 (10) 0.47084 (12) 0.0235 (4)
H1A 0.6761 0.7135 0.4268 0.028*
H1B 0.6827 0.6595 0.5193 0.028*
N11 0.98554 (14) 0.73847 (8) 0.47140 (10) 0.0237 (3)
N12 1.08107 (14) 0.67759 (9) 0.47811 (11) 0.0271 (3)
C13 1.16767 (18) 0.69986 (12) 0.42279 (14) 0.0335 (4)
H13 1.2452 0.6689 0.4146 0.040*
C14 1.1313 (2) 0.77457 (13) 0.37775 (16) 0.0398 (5)
H14 1.1764 0.8035 0.3346 0.048*
C15 1.0150 (2) 0.79640 (11) 0.41052 (14) 0.0347 (4)
H15 0.9635 0.8446 0.3931 0.042*
N21 0.90523 (14) 0.70587 (8) 0.62812 (10) 0.0236 (3)
N22 0.97663 (15) 0.63450 (9) 0.64916 (11) 0.0297 (3)
C23 0.99077 (19) 0.62600 (12) 0.74154 (13) 0.0332 (4)
H23 1.0377 0.5819 0.7754 0.040*
C24 0.92834 (18) 0.68974 (11) 0.78261 (13) 0.0305 (4)
H24 0.9237 0.6977 0.8473 0.037*
C25 0.87472 (18) 0.73874 (11) 0.70831 (13) 0.0276 (4)
H25 0.8244 0.7877 0.7127 0.033*
C31 0.81327 (17) 0.83390 (10) 0.53039 (12) 0.0257 (4)
C32 0.6922 (2) 0.86585 (12) 0.48509 (14) 0.0359 (4)
H32 0.6274 0.8293 0.4526 0.043*
C33 0.6627 (3) 0.95001 (13) 0.48588 (17) 0.0510 (6)
H33 0.5797 0.9697 0.4530 0.061*
C34 0.7532 (3) 1.00449 (13) 0.53392 (17) 0.0510 (6)
H34 0.7330 1.0616 0.5348 0.061*
C35 0.8735 (2) 0.97487 (12) 0.58076 (17) 0.0473 (6)
H35 0.9364 1.0116 0.6149 0.057*
C36 0.9030 (2) 0.89140 (11) 0.57815 (15) 0.0387 (5)
H36 0.9873 0.8725 0.6099 0.046*
C41 0.61642 (17) 0.53155 (10) 0.37391 (12) 0.0244 (4)
C42 0.4899 (2) 0.56546 (14) 0.3715 (2) 0.0575 (7)
H42 0.4816 0.6219 0.3868 0.069*
C43 0.3744 (2) 0.51809 (16) 0.3469 (2) 0.0693 (9)
H43 0.2884 0.5425 0.3456 0.083*
C44 0.3841 (2) 0.43647 (13) 0.32474 (15) 0.0404 (5)
H44 0.3052 0.4041 0.3089 0.048*
C45 0.5090 (2) 0.40206 (12) 0.32563 (18) 0.0498 (6)
H45 0.5163 0.3457 0.3093 0.060*
C46 0.6247 (2) 0.44880 (12) 0.35018 (17) 0.0444 (5)
H46 0.7104 0.4240 0.3508 0.053*
C51 0.82258 (17) 0.62314 (10) 0.29840 (12) 0.0246 (4)
C52 0.7426 (2) 0.67760 (12) 0.23831 (14) 0.0352 (4)
H52 0.6607 0.6977 0.2549 0.042*
C53 0.7826 (2) 0.70227 (14) 0.15467 (15) 0.0446 (5)
H53 0.7280 0.7391 0.1141 0.054*
C54 0.9024 (2) 0.67316 (13) 0.13017 (15) 0.0436 (5)
H54 0.9294 0.6901 0.0728 0.052*
C55 0.9827 (2) 0.61951 (13) 0.18918 (15) 0.0397 (5)
H55 1.0647 0.5999 0.1724 0.048*
C56 0.94305 (18) 0.59439 (11) 0.27293 (13) 0.0301 (4)
H56 0.9981 0.5575 0.3131 0.036*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P1 0.0181 (2) 0.0160 (2) 0.0273 (2) 0.00044 (15) −0.00081 (16) 0.00026 (16)
O1 0.0228 (6) 0.0185 (5) 0.0307 (7) 0.0025 (4) −0.0022 (5) 0.0004 (5)
Li1 0.0284 (15) 0.0197 (13) 0.0321 (16) 0.0048 (11) −0.0031 (12) −0.0027 (11)
B1 0.0218 (9) 0.0194 (9) 0.0250 (10) 0.0012 (7) 0.0020 (8) −0.0002 (7)
C1 0.0203 (8) 0.0191 (8) 0.0308 (9) 0.0017 (6) 0.0030 (7) −0.0011 (7)
N11 0.0224 (7) 0.0198 (7) 0.0282 (8) 0.0001 (5) 0.0021 (6) 0.0001 (6)
N12 0.0235 (7) 0.0248 (7) 0.0321 (8) 0.0030 (6) 0.0015 (6) −0.0069 (6)
C13 0.0251 (9) 0.0348 (10) 0.0414 (11) −0.0014 (8) 0.0078 (8) −0.0115 (8)
C14 0.0363 (11) 0.0416 (11) 0.0449 (12) −0.0064 (9) 0.0169 (9) 0.0035 (9)
C15 0.0362 (10) 0.0277 (9) 0.0423 (11) −0.0002 (8) 0.0125 (9) 0.0075 (8)
N21 0.0239 (7) 0.0200 (7) 0.0265 (8) 0.0011 (5) 0.0023 (6) −0.0001 (6)
N22 0.0365 (8) 0.0223 (7) 0.0290 (8) 0.0081 (6) 0.0008 (7) 0.0028 (6)
C23 0.0372 (10) 0.0314 (10) 0.0293 (10) 0.0035 (8) −0.0009 (8) 0.0044 (8)
C24 0.0294 (9) 0.0380 (10) 0.0236 (9) −0.0015 (8) 0.0025 (7) −0.0010 (8)
C25 0.0261 (9) 0.0295 (9) 0.0275 (9) 0.0002 (7) 0.0047 (7) −0.0048 (7)
C31 0.0304 (9) 0.0216 (8) 0.0253 (9) 0.0017 (7) 0.0052 (7) 0.0012 (7)
C32 0.0388 (10) 0.0288 (9) 0.0376 (11) 0.0076 (8) −0.0019 (8) −0.0060 (8)
C33 0.0579 (14) 0.0380 (12) 0.0524 (14) 0.0236 (10) −0.0065 (11) −0.0029 (10)
C34 0.0745 (16) 0.0227 (10) 0.0544 (14) 0.0133 (10) 0.0056 (12) −0.0018 (9)
C35 0.0625 (14) 0.0230 (10) 0.0546 (14) −0.0049 (9) 0.0033 (11) −0.0054 (9)
C36 0.0394 (11) 0.0254 (9) 0.0488 (13) 0.0002 (8) −0.0011 (9) −0.0010 (8)
C41 0.0228 (8) 0.0203 (8) 0.0287 (9) −0.0021 (6) −0.0007 (7) −0.0005 (7)
C42 0.0247 (10) 0.0355 (11) 0.110 (2) −0.0012 (9) 0.0024 (12) −0.0304 (13)
C43 0.0243 (11) 0.0593 (15) 0.124 (3) −0.0076 (10) 0.0106 (13) −0.0438 (16)
C44 0.0329 (10) 0.0429 (11) 0.0444 (12) −0.0181 (9) 0.0028 (9) −0.0072 (9)
C45 0.0459 (12) 0.0246 (10) 0.0728 (16) −0.0062 (9) −0.0100 (11) −0.0081 (10)
C46 0.0296 (10) 0.0272 (10) 0.0711 (16) 0.0011 (8) −0.0087 (10) −0.0109 (10)
C51 0.0250 (8) 0.0201 (8) 0.0272 (9) −0.0024 (7) −0.0006 (7) −0.0015 (7)
C52 0.0329 (10) 0.0341 (10) 0.0367 (11) 0.0035 (8) −0.0008 (8) 0.0066 (8)
C53 0.0488 (12) 0.0449 (12) 0.0364 (12) −0.0021 (10) −0.0052 (10) 0.0125 (9)
C54 0.0553 (13) 0.0462 (12) 0.0298 (11) −0.0132 (10) 0.0084 (9) 0.0016 (9)
C55 0.0413 (11) 0.0419 (11) 0.0377 (11) −0.0051 (9) 0.0122 (9) −0.0071 (9)
C56 0.0314 (9) 0.0270 (9) 0.0314 (10) −0.0001 (7) 0.0033 (8) −0.0027 (7)

Geometric parameters (Å, º)

P1—O1 1.5099 (11) C31—C32 1.391 (3)
P1—C1 1.7868 (16) C31—C36 1.404 (3)
P1—C51 1.8092 (18) C32—C33 1.399 (3)
P1—C41 1.8150 (17) C32—H32 0.9500
P1—Li1 3.042 (3) C33—C34 1.377 (3)
O1—Li1i 1.901 (3) C33—H33 0.9500
O1—Li1 1.962 (3) C34—C35 1.379 (3)
Li1—O1i 1.901 (3) C34—H34 0.9500
Li1—N12 2.013 (3) C35—C36 1.389 (3)
Li1—N22 2.030 (3) C35—H35 0.9500
Li1—Li1i 2.675 (5) C36—H36 0.9500
B1—N11 1.583 (2) C41—C42 1.382 (3)
B1—N21 1.585 (2) C41—C46 1.392 (3)
B1—C31 1.633 (2) C42—C43 1.393 (3)
B1—C1 1.666 (2) C42—H42 0.9500
C1—H1A 0.9900 C43—C44 1.370 (3)
C1—H1B 0.9900 C43—H43 0.9500
N11—C15 1.351 (2) C44—C45 1.373 (3)
N11—N12 1.3716 (19) C44—H44 0.9500
N12—C13 1.319 (2) C45—C46 1.389 (3)
C13—C14 1.398 (3) C45—H45 0.9500
C13—H13 0.9500 C46—H46 0.9500
C14—C15 1.374 (3) C51—C56 1.399 (2)
C14—H14 0.9500 C51—C52 1.402 (2)
C15—H15 0.9500 C52—C53 1.389 (3)
N21—C25 1.352 (2) C52—H52 0.9500
N21—N22 1.3725 (19) C53—C54 1.390 (3)
N22—C23 1.326 (2) C53—H53 0.9500
C23—C24 1.390 (3) C54—C55 1.387 (3)
C23—H23 0.9500 C54—H54 0.9500
C24—C25 1.377 (3) C55—C56 1.391 (3)
C24—H24 0.9500 C55—H55 0.9500
C25—H25 0.9500 C56—H56 0.9500
O1—P1—C1 115.43 (7) C24—C23—H23 124.3
O1—P1—C51 110.30 (7) C25—C24—C23 104.29 (16)
C1—P1—C51 107.53 (8) C25—C24—H24 127.9
O1—P1—C41 108.59 (7) C23—C24—H24 127.9
C1—P1—C41 108.43 (8) N21—C25—C24 108.97 (16)
C51—P1—C41 106.16 (8) N21—C25—H25 125.5
C1—P1—Li1 88.17 (8) C24—C25—H25 125.5
C51—P1—Li1 103.82 (8) C32—C31—C36 115.67 (16)
C41—P1—Li1 138.96 (8) C32—C31—B1 124.36 (16)
P1—O1—Li1i 147.24 (12) C36—C31—B1 119.81 (15)
P1—O1—Li1 121.82 (10) C31—C32—C33 122.12 (19)
Li1i—O1—Li1 87.65 (13) C31—C32—H32 118.9
O1i—Li1—O1 92.35 (13) C33—C32—H32 118.9
O1i—Li1—N12 128.20 (17) C34—C33—C32 120.5 (2)
O1—Li1—N12 103.93 (14) C34—C33—H33 119.8
O1i—Li1—N22 128.42 (16) C32—C33—H33 119.8
O1—Li1—N22 109.17 (15) C33—C34—C35 119.00 (19)
N12—Li1—N22 92.19 (12) C33—C34—H34 120.5
O1i—Li1—Li1i 47.13 (9) C35—C34—H34 120.5
O1—Li1—Li1i 45.22 (9) C34—C35—C36 120.1 (2)
N12—Li1—Li1i 128.0 (2) C34—C35—H35 119.9
N22—Li1—Li1i 133.0 (2) C36—C35—H35 119.9
O1i—Li1—P1 116.35 (12) C35—C36—C31 122.56 (19)
O1—Li1—P1 24.94 (5) C35—C36—H36 118.7
N12—Li1—P1 83.14 (10) C31—C36—H36 118.7
N22—Li1—P1 96.69 (11) C42—C41—C46 117.88 (17)
Li1i—Li1—P1 69.52 (11) C42—C41—P1 123.73 (14)
N11—B1—N21 108.48 (13) C46—C41—P1 118.38 (14)
N11—B1—C31 105.79 (13) C41—C42—C43 121.00 (19)
N21—B1—C31 107.82 (13) C41—C42—H42 119.5
N11—B1—C1 112.07 (13) C43—C42—H42 119.5
N21—B1—C1 109.71 (13) C44—C43—C42 120.5 (2)
C31—B1—C1 112.75 (13) C44—C43—H43 119.8
B1—C1—P1 121.24 (11) C42—C43—H43 119.8
B1—C1—H1A 107.0 C43—C44—C45 119.26 (18)
P1—C1—H1A 107.0 C43—C44—H44 120.4
B1—C1—H1B 107.0 C45—C44—H44 120.4
P1—C1—H1B 107.0 C44—C45—C46 120.63 (19)
H1A—C1—H1B 106.8 C44—C45—H45 119.7
C15—N11—N12 109.06 (14) C46—C45—H45 119.7
C15—N11—B1 126.33 (14) C45—C46—C41 120.73 (19)
N12—N11—B1 124.57 (13) C45—C46—H46 119.6
C13—N12—N11 106.28 (15) C41—C46—H46 119.6
C13—N12—Li1 135.92 (15) C56—C51—C52 119.06 (17)
N11—N12—Li1 115.97 (13) C56—C51—P1 119.69 (13)
N12—C13—C14 111.66 (16) C52—C51—P1 121.25 (14)
N12—C13—H13 124.2 C53—C52—C51 120.26 (19)
C14—C13—H13 124.2 C53—C52—H52 119.9
C15—C14—C13 103.87 (17) C51—C52—H52 119.9
C15—C14—H14 128.1 C52—C53—C54 120.1 (2)
C13—C14—H14 128.1 C52—C53—H53 120.0
N11—C15—C14 109.13 (17) C54—C53—H53 120.0
N11—C15—H15 125.4 C55—C54—C53 120.2 (2)
C14—C15—H15 125.4 C55—C54—H54 119.9
C25—N21—N22 108.91 (14) C53—C54—H54 119.9
C25—N21—B1 127.38 (14) C54—C55—C56 120.00 (19)
N22—N21—B1 123.54 (13) C54—C55—H55 120.0
C23—N22—N21 106.37 (14) C56—C55—H55 120.0
C23—N22—Li1 136.66 (15) C55—C56—C51 120.39 (18)
N21—N22—Li1 116.94 (13) C55—C56—H56 119.8
N22—C23—C24 111.45 (16) C51—C56—H56 119.8
N22—C23—H23 124.3
C1—P1—O1—Li1i 171.1 (2) N11—B1—N21—N22 −51.28 (19)
C51—P1—O1—Li1i −66.8 (2) C31—B1—N21—N22 −165.41 (14)
C41—P1—O1—Li1i 49.2 (2) C1—B1—N21—N22 71.45 (18)
Li1—P1—O1—Li1i −151.0 (2) C25—N21—N22—C23 −1.26 (19)
C1—P1—O1—Li1 −37.84 (15) B1—N21—N22—C23 −176.84 (15)
C51—P1—O1—Li1 84.26 (14) C25—N21—N22—Li1 −179.89 (14)
C41—P1—O1—Li1 −159.79 (13) B1—N21—N22—Li1 4.5 (2)
P1—O1—Li1—O1i −164.79 (12) O1i—Li1—N22—C23 6.8 (3)
Li1i—O1—Li1—O1i 0.0 O1—Li1—N22—C23 116.1 (2)
P1—O1—Li1—N12 −34.41 (18) N12—Li1—N22—C23 −138.3 (2)
Li1i—O1—Li1—N12 130.4 (2) Li1i—Li1—N22—C23 70.2 (3)
P1—O1—Li1—N22 62.93 (18) P1—Li1—N22—C23 138.3 (2)
Li1i—O1—Li1—N22 −132.3 (2) O1i—Li1—N22—N21 −175.15 (17)
P1—O1—Li1—Li1i −164.79 (12) O1—Li1—N22—N21 −65.82 (19)
Li1i—O1—Li1—P1 164.79 (12) N12—Li1—N22—N21 39.75 (17)
O1—P1—Li1—O1i 17.01 (14) Li1i—Li1—N22—N21 −111.7 (2)
C1—P1—Li1—O1i 163.34 (15) P1—Li1—N22—N21 −43.60 (16)
C51—P1—Li1—O1i −89.05 (15) N21—N22—C23—C24 0.9 (2)
C41—P1—Li1—O1i 46.9 (2) Li1—N22—C23—C24 179.15 (18)
C1—P1—Li1—O1 146.34 (14) N22—C23—C24—C25 −0.2 (2)
C51—P1—Li1—O1 −106.06 (13) N22—N21—C25—C24 1.13 (19)
C41—P1—Li1—O1 29.91 (19) B1—N21—C25—C24 176.50 (15)
O1—P1—Li1—N12 146.46 (19) C23—C24—C25—N21 −0.6 (2)
C1—P1—Li1—N12 −67.20 (10) N11—B1—C31—C32 114.39 (19)
C51—P1—Li1—N12 40.40 (11) N21—B1—C31—C32 −129.69 (18)
C41—P1—Li1—N12 176.37 (10) C1—B1—C31—C32 −8.4 (2)
O1—P1—Li1—N22 −122.13 (19) N11—B1—C31—C36 −60.8 (2)
C1—P1—Li1—N22 24.21 (11) N21—B1—C31—C36 55.1 (2)
C51—P1—Li1—N22 131.82 (11) C1—B1—C31—C36 176.41 (17)
C41—P1—Li1—N22 −92.22 (14) C36—C31—C32—C33 1.0 (3)
O1—P1—Li1—Li1i 11.46 (9) B1—C31—C32—C33 −174.4 (2)
C1—P1—Li1—Li1i 157.80 (14) C31—C32—C33—C34 −1.3 (4)
C51—P1—Li1—Li1i −94.59 (13) C32—C33—C34—C35 0.4 (4)
C41—P1—Li1—Li1i 41.4 (2) C33—C34—C35—C36 0.8 (4)
N11—B1—C1—P1 30.97 (19) C34—C35—C36—C31 −1.2 (4)
N21—B1—C1—P1 −89.61 (16) C32—C31—C36—C35 0.3 (3)
C31—B1—C1—P1 150.21 (13) B1—C31—C36—C35 175.9 (2)
O1—P1—C1—B1 49.57 (16) O1—P1—C41—C42 145.5 (2)
C51—P1—C1—B1 −74.01 (15) C1—P1—C41—C42 19.4 (2)
C41—P1—C1—B1 171.61 (13) C51—P1—C41—C42 −95.9 (2)
Li1—P1—C1—B1 29.91 (14) Li1—P1—C41—C42 128.8 (2)
N21—B1—N11—C15 −140.79 (17) O1—P1—C41—C46 −34.10 (19)
C31—B1—N11—C15 −25.3 (2) C1—P1—C41—C46 −160.22 (16)
C1—B1—N11—C15 97.93 (19) C51—P1—C41—C46 84.50 (18)
N21—B1—N11—N12 41.7 (2) Li1—P1—C41—C46 −50.9 (2)
C31—B1—N11—N12 157.17 (14) C46—C41—C42—C43 0.6 (4)
C1—B1—N11—N12 −79.57 (19) P1—C41—C42—C43 −179.0 (2)
C15—N11—N12—C13 0.96 (19) C41—C42—C43—C44 0.1 (5)
B1—N11—N12—C13 178.83 (15) C42—C43—C44—C45 −0.9 (4)
C15—N11—N12—Li1 −166.12 (15) C43—C44—C45—C46 1.0 (4)
B1—N11—N12—Li1 11.8 (2) C44—C45—C46—C41 −0.3 (4)
O1i—Li1—N12—C13 5.1 (3) C42—C41—C46—C45 −0.5 (3)
O1—Li1—N12—C13 −99.3 (2) P1—C41—C46—C45 179.16 (19)
N22—Li1—N12—C13 150.30 (18) O1—P1—C51—C56 1.27 (16)
Li1i—Li1—N12—C13 −56.0 (3) C1—P1—C51—C56 127.92 (14)
P1—Li1—N12—C13 −113.22 (19) C41—P1—C51—C56 −116.19 (14)
O1i—Li1—N12—N11 167.11 (16) Li1—P1—C51—C56 35.44 (15)
O1—Li1—N12—N11 62.69 (18) O1—P1—C51—C52 −179.60 (14)
N22—Li1—N12—N11 −47.68 (16) C1—P1—C51—C52 −52.95 (16)
Li1i—Li1—N12—N11 106.0 (2) C41—P1—C51—C52 62.94 (16)
P1—Li1—N12—N11 48.80 (13) Li1—P1—C51—C52 −145.43 (15)
N11—N12—C13—C14 −0.7 (2) C56—C51—C52—C53 0.2 (3)
Li1—N12—C13—C14 162.48 (19) P1—C51—C52—C53 −178.95 (15)
N12—C13—C14—C15 0.2 (2) C51—C52—C53—C54 −0.1 (3)
N12—N11—C15—C14 −0.8 (2) C52—C53—C54—C55 −0.1 (3)
B1—N11—C15—C14 −178.67 (16) C53—C54—C55—C56 0.3 (3)
C13—C14—C15—N11 0.4 (2) C54—C55—C56—C51 −0.2 (3)
N11—B1—N21—C25 133.99 (16) C52—C51—C56—C55 0.0 (3)
C31—B1—N21—C25 19.9 (2) P1—C51—C56—C55 179.12 (14)
C1—B1—N21—C25 −103.29 (18)

Symmetry code: (i) −x+2, −y+1, −z+1.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: SJ5403).

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) I, global. DOI: 10.1107/S1600536814011945/sj5403sup1.cif

e-70-0m237-sup1.cif (34.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814011945/sj5403Isup2.hkl

e-70-0m237-Isup2.hkl (213.8KB, hkl)

CCDC reference: 883935

Additional supporting information: crystallographic information; 3D view; checkCIF report


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