Literature DB >> 24855466

Tri-μ-chlorido-bis-[(η(5)-penta-methyl-cyclo-penta-dien-yl)rhodium(III)] hexa-fluorido-phosphate from synchrotron radiation.

Lida Ezzedinloo1, Sumi Shrestha1, Mohan Bhadbhade2, Stephen Colbran1.   

Abstract

In the title complex salt, [{(η(5)-C5Me5)Rh}2(μ-Cl)3]PF6, the dinuclear, single-charged cation is formed by the cojoining of two classic (η(5)-C5Me5)RhCl3 'piano-stool' units by bridging of the three choride ligand 'legs'. The crystal structure shows several close H⋯F contacts between the hexa-fluorido-phosphate counter-ions and the C5Me5 ligands.

Entities:  

Year:  2013        PMID: 24855466      PMCID: PMC4029212          DOI: 10.1107/S1600536813032480

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

Complexes of the (η5-C5Me5)RhIII group, modified by innumerable co-ligands, exhibit a diverse and very useful chemistry, particularly as homogeneous catalysts, see, for example: McSkimming et al. (2013 ▶); Brewster et al. (2013 ▶); Yu, Wan & Li (2013 ▶); Yu, Yu, Xiao, et al. (2013 ▶), Becerra et al. (2013 ▶); Gupta et al. (2013 ▶). The title complex salt, [{(η5-C5Me5)Rh}2(μ-Cl)3][PF6], is a commonly encountered impurity produced in reactions of the much-used RhIII precursor [(η5-C5Me5)RhCl2]2 (Kang et al., 1969 ▶; Booth et al., 1969 ▶). [{(η5-C5Me5)Rh}2(μ-Cl)3][PF6] was first reported by Koelle (1990 ▶), and often (co-)crystallizes with or instead of the desired product of a reaction employing [(η5-C5Me5)RhCl2]2 and anion meta­thesis with a simple [PF6]− salt. Several crystal structures of the [{(η5-C5Me5)Rh}2(μ-Cl)3]+ cation with other counter-ions have been reported, including salts with [PtCl5(CH3CONH2)]− and [PtCl6]2− (Umakoshi et al., 1991 ▶), [{(C6F5)2Pd(μ-Cl)}2]2− (Ara et al., 2001 ▶), and BF4 − (Liu et al., 2004 ▶) anions.

Experimental

Crystal data

[Rh2(C10H15)2Cl3]PF6 M = 727.58 Triclinic, a = 8.0970 (16) Å b = 12.604 (3) Å c = 14.441 (3) Å α = 64.28 (3)° β = 82.42 (3)° γ = 86.70 (3)° V = 1316.1 (6) Å3 Z = 2 Synchrotron radiation λ = 0.71073 Å μ = 1.67 mm−1 T = 100 K 0.02 × 0.02 × 0.01 mm

Data collection

3-BM1 Australian Synchrotron diffractometer 15787 measured reflections 4158 independent reflections 4064 reflections with I > 2σ(I) R int = 0.021

Refinement

R[F 2 > 2σ(F 2)] = 0.025 wR(F 2) = 0.060 S = 1.09 4158 reflections 299 parameters H-atom parameters constrained Δρmax = 1.03 e Å−3 Δρmin = −0.57 e Å−3 Data collection: BLU-ICE (McPhillips et al., 2002 ▶); cell refinement: XDS (Kabsch, 1993 ▶); data reduction: XDS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶) and OLEX2 (Dolomanov et al., 2009 ▶); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008 ▶); molecular graphics: CrystalMaker (CrystalMaker, 2013 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536813032480/tk5276sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813032480/tk5276Isup2.hkl Additional supporting information: crystallographic information; 3D view; checkCIF report
[Rh2(C10H15)2Cl3]PF6Z = 2
Mr = 727.58F(000) = 720
Triclinic, P1Dx = 1.836 Mg m3
a = 8.0970 (16) ÅSynchrotron radiation, λ = 0.71073 Å
b = 12.604 (3) ÅCell parameters from 9980 reflections
c = 14.441 (3) Åθ = 2.5–22.5°
α = 64.28 (3)°µ = 1.67 mm1
β = 82.42 (3)°T = 100 K
γ = 86.70 (3)°Plate, yellow
V = 1316.1 (6) Å30.02 × 0.02 × 0.01 mm
3-BM1 Australian Synchrotron diffractometer4064 reflections with I > 2σ(I)
Radiation source: Synchrotron BMRint = 0.021
Si<111> monochromatorθmax = 25.0°, θmin = 1.8°
Phi Scan scansh = −9→9
15787 measured reflectionsk = −14→14
4158 independent reflectionsl = −17→17
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025H-atom parameters constrained
wR(F2) = 0.060w = 1/[σ2(Fo2) + (0.018P)2 + 3.0381P] where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
4158 reflectionsΔρmax = 1.03 e Å3
299 parametersΔρmin = −0.57 e Å3
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 is 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.
xyzUiso*/Ueq
Rh1A0.10004 (3)0.61463 (2)0.24284 (2)0.01511 (8)
C1A0.1288 (4)0.7995 (2)0.1858 (2)0.0193 (6)
C2A0.0856 (4)0.7501 (2)0.2954 (2)0.0204 (6)
C3A−0.0722 (4)0.6920 (2)0.3203 (3)0.0216 (6)
C4A−0.1288 (4)0.7091 (2)0.2238 (2)0.0205 (6)
C5A−0.0069 (4)0.7767 (2)0.1414 (2)0.0195 (6)
C6A0.2816 (4)0.8692 (3)0.1264 (3)0.0270 (7)
H6AA0.37260.84140.16750.041*
H6AB0.26160.95090.11020.041*
H6AC0.30890.86020.06350.041*
C7A0.1867 (4)0.7580 (3)0.3717 (3)0.0290 (7)
H7AA0.16210.69180.43760.044*
H7AB0.15990.82960.37860.044*
H7AC0.30300.75760.34780.044*
C8A−0.1641 (4)0.6277 (3)0.4248 (3)0.0288 (7)
H8AA−0.21670.55960.42830.043*
H8AB−0.24730.67840.43800.043*
H8AC−0.08770.60350.47580.043*
C9A−0.2884 (4)0.6647 (3)0.2138 (3)0.0283 (7)
H9AA−0.27740.65440.15120.043*
H9AB−0.37540.72050.21160.043*
H9AC−0.31550.59060.27210.043*
C10A−0.0175 (4)0.8173 (3)0.0292 (3)0.0258 (7)
H10A0.09270.8243−0.00690.039*
H10B−0.07200.89250.00250.039*
H10C−0.08000.76130.01930.039*
Cl10.34572 (8)0.51534 (6)0.32353 (6)0.02165 (16)
Cl20.21608 (12)0.55011 (7)0.11061 (6)0.0337 (2)
Cl3−0.00889 (8)0.40972 (6)0.32708 (6)0.02133 (16)
Rh1B0.27583 (3)0.37186 (2)0.26318 (2)0.01627 (8)
C1B0.5043 (4)0.2970 (2)0.2305 (2)0.0200 (6)
C2B0.4541 (4)0.2404 (2)0.3399 (2)0.0208 (6)
C3B0.2944 (4)0.1876 (2)0.3568 (3)0.0230 (6)
C4B0.2479 (4)0.2083 (2)0.2568 (3)0.0226 (6)
C5B0.3795 (4)0.2738 (2)0.1797 (2)0.0212 (6)
C6B0.6637 (4)0.3625 (3)0.1790 (3)0.0250 (7)
H6BA0.64650.42360.11220.038*
H6BB0.74760.30910.17100.038*
H6BC0.69950.39680.22080.038*
C7B0.5525 (4)0.2373 (3)0.4214 (3)0.0254 (7)
H7BA0.61120.31030.39670.038*
H7BB0.63090.17350.43730.038*
H7BC0.47850.22600.48260.038*
C8B0.1955 (4)0.1180 (3)0.4585 (3)0.0305 (7)
H8BA0.22700.14000.50950.046*
H8BB0.21660.03560.47910.046*
H8BC0.07900.13360.45230.046*
C9B0.0951 (4)0.1628 (3)0.2385 (3)0.0310 (7)
H9BA0.00700.15530.29250.046*
H9BB0.11830.08730.23860.046*
H9BC0.06180.21670.17280.046*
C10B0.3836 (4)0.3111 (3)0.0667 (3)0.0273 (7)
H10D0.27560.33940.04600.041*
H10E0.41370.24510.05130.041*
H10F0.46420.37270.02970.041*
P10.65562 (9)−0.00832 (6)0.23670 (6)0.02081 (17)
F10.6989 (3)0.12409 (17)0.1566 (2)0.0543 (7)
F20.6292 (4)0.0304 (2)0.32864 (19)0.0580 (8)
F30.6095 (3)−0.14070 (16)0.31547 (17)0.0444 (6)
F40.6793 (3)−0.04801 (18)0.14494 (16)0.0435 (5)
F50.4642 (2)0.01935 (18)0.2209 (2)0.0425 (5)
F60.8456 (3)−0.0364 (2)0.2528 (3)0.0699 (9)
U11U22U33U12U13U23
Rh1A0.01543 (12)0.01295 (12)0.01698 (14)0.00227 (8)−0.00149 (9)−0.00688 (9)
C1A0.0213 (14)0.0129 (13)0.0248 (17)0.0034 (11)−0.0064 (13)−0.0084 (11)
C2A0.0217 (14)0.0168 (13)0.0266 (17)0.0056 (11)−0.0052 (13)−0.0129 (12)
C3A0.0227 (14)0.0176 (14)0.0253 (18)0.0061 (11)−0.0002 (13)−0.0113 (12)
C4A0.0182 (14)0.0162 (13)0.0274 (18)0.0059 (11)−0.0025 (13)−0.0105 (12)
C5A0.0202 (14)0.0122 (12)0.0249 (17)0.0029 (10)−0.0050 (13)−0.0067 (11)
C6A0.0234 (15)0.0205 (15)0.0341 (19)−0.0017 (12)−0.0068 (14)−0.0078 (13)
C7A0.0357 (17)0.0268 (16)0.0307 (19)0.0050 (13)−0.0125 (15)−0.0163 (14)
C8A0.0305 (16)0.0269 (16)0.0252 (19)0.0057 (13)0.0045 (15)−0.0106 (14)
C9A0.0197 (15)0.0236 (15)0.043 (2)0.0006 (12)−0.0042 (14)−0.0151 (14)
C10A0.0277 (16)0.0245 (15)0.0255 (18)0.0022 (12)−0.0082 (14)−0.0098 (13)
Cl10.0140 (3)0.0187 (3)0.0367 (4)0.0013 (2)−0.0064 (3)−0.0153 (3)
Cl20.0535 (5)0.0247 (4)0.0181 (4)0.0177 (3)−0.0013 (4)−0.0077 (3)
Cl30.0147 (3)0.0172 (3)0.0337 (4)0.0003 (2)−0.0044 (3)−0.0121 (3)
Rh1B0.01803 (12)0.01362 (12)0.01822 (14)0.00375 (8)−0.00374 (9)−0.00785 (9)
C1B0.0216 (14)0.0185 (13)0.0239 (17)0.0078 (11)−0.0064 (13)−0.0127 (12)
C2B0.0217 (14)0.0150 (13)0.0265 (18)0.0089 (11)−0.0085 (13)−0.0093 (12)
C3B0.0273 (15)0.0141 (13)0.0277 (18)0.0060 (11)−0.0076 (14)−0.0086 (12)
C4B0.0249 (15)0.0163 (13)0.0303 (18)0.0043 (11)−0.0066 (14)−0.0131 (12)
C5B0.0227 (14)0.0179 (14)0.0278 (18)0.0072 (11)−0.0071 (13)−0.0141 (12)
C6B0.0224 (15)0.0253 (15)0.0315 (19)0.0044 (12)−0.0046 (14)−0.0162 (14)
C7B0.0280 (16)0.0258 (15)0.0238 (18)0.0053 (12)−0.0089 (14)−0.0110 (13)
C8B0.0335 (17)0.0220 (15)0.0293 (19)−0.0002 (13)−0.0017 (15)−0.0054 (13)
C9B0.0277 (16)0.0284 (16)0.043 (2)0.0001 (13)−0.0100 (16)−0.0198 (15)
C10B0.0297 (16)0.0304 (16)0.0290 (19)0.0074 (13)−0.0097 (15)−0.0187 (14)
P10.0211 (4)0.0157 (4)0.0277 (5)0.0025 (3)−0.0044 (3)−0.0112 (3)
F10.0556 (14)0.0169 (10)0.0746 (19)−0.0048 (9)0.0307 (13)−0.0151 (10)
F20.100 (2)0.0476 (13)0.0488 (15)0.0435 (14)−0.0434 (15)−0.0372 (12)
F30.0634 (14)0.0196 (9)0.0375 (13)0.0082 (9)0.0102 (11)−0.0058 (9)
F40.0713 (15)0.0319 (11)0.0294 (12)0.0141 (10)−0.0040 (11)−0.0174 (9)
F50.0265 (10)0.0384 (11)0.0757 (17)0.0103 (8)−0.0171 (11)−0.0348 (11)
F60.0297 (11)0.0550 (14)0.163 (3)0.0194 (10)−0.0407 (15)−0.0760 (18)
Rh1A—C1A2.123 (3)Rh1B—C1B2.119 (3)
Rh1A—C4A2.126 (3)Rh1B—C4B2.129 (3)
Rh1A—C3A2.127 (3)Rh1B—C3B2.129 (3)
Rh1A—C2A2.140 (3)Rh1B—C5B2.142 (3)
Rh1A—C5A2.145 (3)Rh1B—C2B2.147 (3)
Rh1A—Cl12.4372 (11)C1B—C2B1.434 (5)
Rh1A—Cl22.4448 (10)C1B—C5B1.435 (4)
Rh1A—Cl32.4860 (11)C1B—C6B1.496 (4)
C1A—C2A1.428 (5)C2B—C3B1.433 (4)
C1A—C5A1.443 (4)C2B—C7B1.491 (4)
C1A—C6A1.493 (4)C3B—C4B1.449 (4)
C2A—C3A1.434 (4)C3B—C8B1.490 (5)
C2A—C7A1.496 (4)C4B—C5B1.430 (5)
C3A—C4A1.447 (4)C4B—C9B1.492 (4)
C3A—C8A1.483 (5)C5B—C10B1.486 (5)
C4A—C5A1.423 (4)C6B—H6BA0.9600
C4A—C9A1.485 (4)C6B—H6BB0.9600
C5A—C10A1.485 (4)C6B—H6BC0.9600
C6A—H6AA0.9600C7B—H7BA0.9600
C6A—H6AB0.9600C7B—H7BB0.9600
C6A—H6AC0.9600C7B—H7BC0.9600
C7A—H7AA0.9600C8B—H8BA0.9600
C7A—H7AB0.9600C8B—H8BB0.9600
C7A—H7AC0.9600C8B—H8BC0.9600
C8A—H8AA0.9600C9B—H9BA0.9600
C8A—H8AB0.9600C9B—H9BB0.9600
C8A—H8AC0.9600C9B—H9BC0.9600
C9A—H9AA0.9600C10B—H10D0.9600
C9A—H9AB0.9600C10B—H10E0.9600
C9A—H9AC0.9600C10B—H10F0.9600
C10A—H10A0.9600P1—F61.583 (2)
C10A—H10B0.9600P1—F21.589 (2)
C10A—H10C0.9600P1—F31.590 (2)
Cl1—Rh1B2.4426 (9)P1—F11.591 (2)
Cl2—Rh1B2.4485 (13)P1—F51.593 (2)
Cl3—Rh1B2.4675 (10)P1—F41.594 (2)
C1A—Rh1A—C4A66.16 (11)C1B—Rh1B—C2B39.27 (12)
C1A—Rh1A—C3A66.24 (12)C4B—Rh1B—C2B65.99 (11)
C4A—Rh1A—C3A39.78 (12)C3B—Rh1B—C2B39.15 (12)
C1A—Rh1A—C2A39.13 (12)C5B—Rh1B—C2B65.51 (11)
C4A—Rh1A—C2A65.91 (11)C1B—Rh1B—Cl1106.37 (8)
C3A—Rh1A—C2A39.26 (12)C4B—Rh1B—Cl1160.83 (9)
C1A—Rh1A—C5A39.53 (11)C3B—Rh1B—Cl1121.24 (9)
C4A—Rh1A—C5A38.91 (12)C5B—Rh1B—Cl1142.82 (8)
C3A—Rh1A—C5A65.94 (12)C2B—Rh1B—Cl196.84 (8)
C2A—Rh1A—C5A65.55 (11)C1B—Rh1B—Cl2109.99 (9)
C1A—Rh1A—Cl1109.38 (8)C4B—Rh1B—Cl2116.63 (9)
C4A—Rh1A—Cl1158.78 (9)C3B—Rh1B—Cl2156.37 (9)
C3A—Rh1A—Cl1119.00 (9)C5B—Rh1B—Cl295.96 (9)
C2A—Rh1A—Cl197.15 (8)C2B—Rh1B—Cl2147.91 (9)
C5A—Rh1A—Cl1146.87 (8)Cl1—Rh1B—Cl282.39 (3)
C1A—Rh1A—Cl2110.16 (9)C1B—Rh1B—Cl3166.37 (8)
C4A—Rh1A—Cl2118.62 (9)C4B—Rh1B—Cl3102.35 (9)
C3A—Rh1A—Cl2158.36 (9)C3B—Rh1B—Cl3100.28 (10)
C2A—Rh1A—Cl2147.40 (9)C5B—Rh1B—Cl3134.81 (8)
C5A—Rh1A—Cl297.28 (9)C2B—Rh1B—Cl3130.39 (9)
Cl1—Rh1A—Cl282.58 (3)Cl1—Rh1B—Cl381.93 (3)
C1A—Rh1A—Cl3164.71 (8)Cl2—Rh1B—Cl381.46 (5)
C4A—Rh1A—Cl399.66 (9)C2B—C1B—C5B108.0 (3)
C3A—Rh1A—Cl399.37 (9)C2B—C1B—C6B125.8 (3)
C2A—Rh1A—Cl3131.24 (9)C5B—C1B—C6B126.1 (3)
C5A—Rh1A—Cl3131.26 (8)C2B—C1B—Rh1B71.41 (16)
Cl1—Rh1A—Cl381.65 (4)C5B—C1B—Rh1B71.21 (16)
Cl2—Rh1A—Cl381.16 (4)C6B—C1B—Rh1B125.8 (2)
C2A—C1A—C5A107.8 (3)C3B—C2B—C1B108.2 (3)
C2A—C1A—C6A126.4 (3)C3B—C2B—C7B126.3 (3)
C5A—C1A—C6A125.7 (3)C1B—C2B—C7B125.6 (3)
C2A—C1A—Rh1A71.08 (16)C3B—C2B—Rh1B69.76 (16)
C5A—C1A—Rh1A71.05 (15)C1B—C2B—Rh1B69.32 (15)
C6A—C1A—Rh1A126.3 (2)C7B—C2B—Rh1B126.7 (2)
C1A—C2A—C3A108.5 (3)C2B—C3B—C4B107.8 (3)
C1A—C2A—C7A126.0 (3)C2B—C3B—C8B126.9 (3)
C3A—C2A—C7A125.5 (3)C4B—C3B—C8B125.2 (3)
C1A—C2A—Rh1A69.79 (16)C2B—C3B—Rh1B71.09 (16)
C3A—C2A—Rh1A69.86 (16)C4B—C3B—Rh1B70.09 (16)
C7A—C2A—Rh1A126.5 (2)C8B—C3B—Rh1B126.6 (2)
C2A—C3A—C4A107.4 (3)C5B—C4B—C3B107.7 (3)
C2A—C3A—C8A127.1 (3)C5B—C4B—C9B126.3 (3)
C4A—C3A—C8A125.5 (3)C3B—C4B—C9B125.9 (3)
C2A—C3A—Rh1A70.88 (17)C5B—C4B—Rh1B70.96 (16)
C4A—C3A—Rh1A70.09 (17)C3B—C4B—Rh1B70.12 (16)
C8A—C3A—Rh1A125.2 (2)C9B—C4B—Rh1B127.2 (2)
C5A—C4A—C3A108.2 (3)C4B—C5B—C1B108.3 (3)
C5A—C4A—C9A126.5 (3)C4B—C5B—C10B125.2 (3)
C3A—C4A—C9A125.3 (3)C1B—C5B—C10B126.5 (3)
C5A—C4A—Rh1A71.25 (16)C4B—C5B—Rh1B69.91 (17)
C3A—C4A—Rh1A70.13 (16)C1B—C5B—Rh1B69.44 (16)
C9A—C4A—Rh1A125.1 (2)C10B—C5B—Rh1B126.2 (2)
C4A—C5A—C1A108.0 (3)C1B—C6B—H6BA109.5
C4A—C5A—C10A126.1 (3)C1B—C6B—H6BB109.5
C1A—C5A—C10A125.9 (3)H6BA—C6B—H6BB109.5
C4A—C5A—Rh1A69.83 (16)C1B—C6B—H6BC109.5
C1A—C5A—Rh1A69.42 (15)H6BA—C6B—H6BC109.5
C10A—C5A—Rh1A126.6 (2)H6BB—C6B—H6BC109.5
C1A—C6A—H6AA109.5C2B—C7B—H7BA109.5
C1A—C6A—H6AB109.5C2B—C7B—H7BB109.5
H6AA—C6A—H6AB109.5H7BA—C7B—H7BB109.5
C1A—C6A—H6AC109.5C2B—C7B—H7BC109.5
H6AA—C6A—H6AC109.5H7BA—C7B—H7BC109.5
H6AB—C6A—H6AC109.5H7BB—C7B—H7BC109.5
C2A—C7A—H7AA109.5C3B—C8B—H8BA109.5
C2A—C7A—H7AB109.5C3B—C8B—H8BB109.5
H7AA—C7A—H7AB109.5H8BA—C8B—H8BB109.5
C2A—C7A—H7AC109.5C3B—C8B—H8BC109.5
H7AA—C7A—H7AC109.5H8BA—C8B—H8BC109.5
H7AB—C7A—H7AC109.5H8BB—C8B—H8BC109.5
C3A—C8A—H8AA109.5C4B—C9B—H9BA109.5
C3A—C8A—H8AB109.5C4B—C9B—H9BB109.5
H8AA—C8A—H8AB109.5H9BA—C9B—H9BB109.5
C3A—C8A—H8AC109.5C4B—C9B—H9BC109.5
H8AA—C8A—H8AC109.5H9BA—C9B—H9BC109.5
H8AB—C8A—H8AC109.5H9BB—C9B—H9BC109.5
C4A—C9A—H9AA109.5C5B—C10B—H10D109.5
C4A—C9A—H9AB109.5C5B—C10B—H10E109.5
H9AA—C9A—H9AB109.5H10D—C10B—H10E109.5
C4A—C9A—H9AC109.5C5B—C10B—H10F109.5
H9AA—C9A—H9AC109.5H10D—C10B—H10F109.5
H9AB—C9A—H9AC109.5H10E—C10B—H10F109.5
C5A—C10A—H10A109.5F6—P1—F290.85 (15)
C5A—C10A—H10B109.5F6—P1—F389.65 (15)
H10A—C10A—H10B109.5F2—P1—F390.74 (14)
C5A—C10A—H10C109.5F6—P1—F191.30 (15)
H10A—C10A—H10C109.5F2—P1—F189.88 (15)
H10B—C10A—H10C109.5F3—P1—F1178.86 (16)
Rh1A—Cl1—Rh1B82.26 (3)F6—P1—F5179.7 (2)
Rh1A—Cl2—Rh1B81.99 (3)F2—P1—F589.10 (14)
Rh1B—Cl3—Rh1A80.78 (4)F3—P1—F590.11 (13)
C1B—Rh1B—C4B66.30 (12)F1—P1—F588.95 (13)
C1B—Rh1B—C3B66.24 (12)F6—P1—F489.88 (15)
C4B—Rh1B—C3B39.79 (12)F2—P1—F4179.11 (16)
C1B—Rh1B—C5B39.35 (11)F3—P1—F488.76 (12)
C4B—Rh1B—C5B39.13 (12)F1—P1—F490.60 (13)
C3B—Rh1B—C5B65.93 (12)F5—P1—F490.17 (13)
D—H···AD—HH···AD···AD—H···A
C8A—H8AB···F3i0.962.533.244 (5)131
C10A—H10A···F1ii0.962.433.328 (4)156
C6B—H6BB···F10.962.493.152 (5)126
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C8A—H8AB⋯F3i 0.962.533.244 (5)131
C10A—H10A⋯F1ii 0.962.433.328 (4)156
C6B—H6BB⋯F10.962.493.152 (5)126

Symmetry codes: (i) ; (ii) .

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Authors:  Timothy M McPhillips; Scott E McPhillips; Hsiu-Ju Chiu; Aina E Cohen; Ashley M Deacon; Paul J Ellis; Elspeth Garman; Ana Gonzalez; Nicholas K Sauter; R Paul Phizackerley; S Michael Soltis; Peter Kuhn
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Authors:  Timothy P Brewster; Alexander J M Miller; D Michael Heinekey; Karen I Goldberg
Journal:  J Am Chem Soc       Date:  2013-10-21       Impact factor: 15.419

7.  Rhodium(III)-catalyzed azacycle-directed intermolecular insertion of arene C-H bonds into α-diazocarbonyl compounds.

Authors:  Xinzhang Yu; Songjie Yu; Jian Xiao; Boshun Wan; Xingwei Li
Journal:  J Org Chem       Date:  2013-05-20       Impact factor: 4.354

8.  Half-sandwich rhodium and iridium complexes containing homochiral imidazolyl-imine ligands: synthesis, characterization and catalytic applications.

Authors:  Alexandra Becerra; Raúl Contreras; Daniel Carmona; Fernando J Lahoz; Pilar García-Orduña
Journal:  Dalton Trans       Date:  2013-07-11       Impact factor: 4.390

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