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Tetra-tert-butyl­tetraphosphacubane, P4C4tBu4, reacts with water in the presence of `GaI' to yield two products, namely 4,6,7,8-tetra-tert-butyl-1,2,3-triphospha-5-phospho­niatetra­cyclo­[3.2.1.02,4.03,8]­oct-6-ene tetra­iodo­gallate(III), (C20H37P4)[GaI4], and tri­iodo(3,5,7,8-tetra-tert-butyl-1,2,4λ5,6-tetra­phos­pha­tetra­cyclo­[4.1.1.02,5.07,8]­octan-4-one)­gallium(III), [GaI3(C20H38OP4)], both of which have been structurally characterized. The X-ray crystal structure determination of the former compound shows it to be an ion-separated salt, while the latter compound is a neutral phosphinite complex of GaI3.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270103014501/bm1533sup1.cif
Contains datablocks global, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270103014501/bm1533Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270103014501/bm1533IIsup3.hkl
Contains datablock II

CCDC references: 221051; 221052

Comment top

There is much interest in the reactivity of compounds derived from the cyclo-oligomerization of phosphaalkynes, RCP, especially the cyclotetramer of tBuCP (Hitchcock et al., 1995). This compound is of interest because a strong interaction between the P lone-pair electrons and the P–C σ*antibonding orbitals considerably reduces the nucleophilicity of the P atoms (Wettling et al., 1989).

We have recently published a study on the reactivity of secondary phosphines towards "GaI". These reactions have yielded Ga—Ga bonded dimers with the coordination of one phosphine molecule per GaII centre (Baker et al., 2003). Therefore, we thought it worthwhile to investigate the reaction of "GaI" towards the relatively non-nucleophilic tetraphosphacubane, P4C4tBu4. No reaction occurred, but in the presence of trace water a rearrangement of the P4C4 skeleton occurred, yielding two products, both of which have been structurally characterized and are reported here.

The molecular structure of [C20H36P4]+ [GaI4], (I), is shown in Fig 1. The bond lengths and angles around the gallium centre of the anion are unremarkable. The tetraphosphabishomoprismane framework of the cation is comparable to the neutal analogue that forms a complex with two W(CO)5 moeities, [(C20H36P4){W(CO)5}2] (Hitchcock et al., 1995). The only major differences between these species are in the bond lengths around atom P4, which are slightly longer in (I). The bond angles around atom P4 are also greater in (I); the ΣCPC angle is 314.1° in (I) and 289° in [(C20H36P4){W(CO)5}2]. In addition, the CC bond length is 0.076 Å longer in (I) than in the tungsten complex. There is no specific, directional interaction between the cation and anion in (I).

The molecular structure of [C20H38GaI3P4O], (II), is shown in Fig 2. The 2,4-diphosphabicyclo[1.1.0]butane fragment is a rare structural motif and only three examples have been reported previously. The P—C and C—C bond lengths of the bicyclic framework are similar to those in previous examples (Jones et al., 2001; Niecke et al., 1999; Mack et al., 2002), and the P—O and Ga—O bond lengths of the phosphinite functionalty are also in keeping with previously reported examples of phosphinite-gallium adducts (Barron et al., 1996). The mechanisms of formation of (I) and (II) are unknown, but in both cases, the rearrangement of the tetraphosphacubane framework in the presence of water is mediated by "GaI", since no reaction occurs in its absence.

Experimental top

"GaI" was prepared by the ultrasonic activation of Ga (0.07 g, 0.99 mmol) and I2 (0.24 g, 0.98 mmol) in toluene (10 ml) for 2 h. To the resulting green suspension, a solution of P4C4tBu4 (0.10 g, 0.25 mmol) in toluene (10 ml) was added. The reaction mixture was stirred for 30 min and a few drops of water were added. The suspension was then stirred overnight, after which the solvent was removed in vacuo. The residue was extraced with hexane, concentrated and stored at 243 K and yielded crystals of (I) in low yield (< 5%). Compound (II) was isolated (yield < 5%) by extraction of the residue with Et2O, which was concentrated in vacuo. Storage at 243 K yielded suitable crystals.

Refinement top

In both compounds, methyl H atoms were placed in idealized positions [C—H = 0.96 Å] and refined as riding, with Uiso(H) values of 1.5Ueq(C). In (II), atom H4 attached to atom P4 was located from a difference Fourier map and refined isotropically, with the P—H distance restrained to 1.33 (2) Å. In (II), methine atom H1 was placed in an idealized position (C—H = 1.00 A) and refined as riding [Uiso(H) = 1.2 Ueq(C)], while atom H21 attached to atom P1 was treated in the same way as atom H4 in (I).

Computing details top

For both compounds, data collection: COLLECT (Hooft, 2000); cell refinement: DENZO–SMN (Otwinowski & Minor, 1997); data reduction: DENZO–SMN; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure of the cation of (I). Displacement ellipsoids are drawn at the 50% probability level and methyl H atoms have been omitted for clarity.
[Figure 2] Fig. 2. The molecular structure of (II). Displacement ellipsoids are drawn at the 50% probability level and methyl H atoms have been omitted for clarity.
(I) 4,6,7,8-tetra-tert-butyl-1,2,3-triphospha-5- phosphoniapentacyclo[3.2.1.02,4.03,8]oct-6-ene tetraiodogallate top
Crystal data top
(C20H37P4)[GaI4]Z = 2
Mr = 978.70F(000) = 920
Triclinic, P1Dx = 2.001 Mg m3
a = 9.6290 (19) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.459 (3) ÅCell parameters from 18935 reflections
c = 13.867 (3) Åθ = 2.9–27.5°
α = 82.91 (3)°µ = 4.85 mm1
β = 81.28 (3)°T = 150 K
γ = 83.65 (3)°Cut plate, yellow
V = 1624.6 (6) Å30.15 × 0.15 × 0.07 mm
Data collection top
Nonius KappaCCD
diffractometer
7382 independent reflections
Radiation source: fine-focus sealed tube5661 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.131
ϕ and ω scans to fill Ewald sphereθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
h = 1212
Tmin = 0.471, Tmax = 0.712k = 1616
25682 measured reflectionsl = 1717
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)] = 0.057Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.151H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.067P)2 + 4.243P]
where P = (Fo2 + 2Fc2)/3
7382 reflections(Δ/σ)max = 0.001
277 parametersΔρmax = 2.15 e Å3
1 restraintΔρmin = 2.69 e Å3
Crystal data top
(C20H37P4)[GaI4]γ = 83.65 (3)°
Mr = 978.70V = 1624.6 (6) Å3
Triclinic, P1Z = 2
a = 9.6290 (19) ÅMo Kα radiation
b = 12.459 (3) ŵ = 4.85 mm1
c = 13.867 (3) ÅT = 150 K
α = 82.91 (3)°0.15 × 0.15 × 0.07 mm
β = 81.28 (3)°
Data collection top
Nonius KappaCCD
diffractometer
7382 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
5661 reflections with I > 2σ(I)
Tmin = 0.471, Tmax = 0.712Rint = 0.131
25682 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0571 restraint
wR(F2) = 0.151H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 2.15 e Å3
7382 reflectionsΔρmin = 2.69 e Å3
277 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. Atom H4 attached to P4 was located from difference maps and its U(iso) set to 0.025, i.e. approximately 1.2 times that of P4. Its position refined satisfactorily using the DFIX command set at 1.33 Angstroms.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.06047 (5)0.85582 (4)0.26162 (4)0.03642 (14)
I20.32581 (6)0.57923 (5)0.20991 (6)0.0664 (2)
I30.46260 (5)0.88334 (5)0.10629 (3)0.04253 (16)
I40.42185 (5)0.78986 (4)0.40124 (3)0.03937 (15)
Ga10.31709 (7)0.77685 (6)0.24522 (5)0.02456 (17)
P10.07153 (18)0.84752 (15)0.57320 (12)0.0280 (4)
P20.04906 (18)0.68298 (16)0.53638 (12)0.0310 (4)
P30.22702 (16)0.75207 (13)0.66427 (11)0.0226 (3)
P40.02632 (16)0.67533 (13)0.73010 (11)0.0205 (3)
C10.0771 (6)0.7636 (5)0.6252 (4)0.0220 (12)
C20.1318 (6)0.6310 (5)0.6555 (4)0.0229 (12)
C30.1451 (7)0.7832 (5)0.7910 (4)0.0221 (12)
C40.0230 (7)0.7377 (5)0.8288 (4)0.0227 (12)
C50.2302 (7)0.8086 (6)0.6138 (5)0.0277 (14)
C60.2347 (8)0.8682 (7)0.5109 (6)0.0450 (19)
H6A0.33070.89240.50250.067*
H6B0.19560.81980.46280.067*
H6C0.18050.92970.50270.067*
C70.3242 (7)0.7149 (6)0.6265 (6)0.0345 (16)
H7A0.32350.67680.69110.052*
H7B0.28900.66580.57840.052*
H7C0.41900.74330.61820.052*
C80.2828 (8)0.8856 (7)0.6898 (6)0.044 (2)
H8A0.37570.91770.68020.067*
H8B0.22020.94170.68360.067*
H8C0.28610.84650.75420.067*
C90.2115 (7)0.5172 (5)0.6703 (5)0.0313 (15)
C100.1171 (9)0.4318 (7)0.6586 (8)0.056 (3)
H10A0.16590.36090.66990.084*
H10B0.09270.44220.59330.084*
H10C0.03280.43800.70520.084*
C110.3435 (9)0.5123 (7)0.5934 (6)0.047 (2)
H11A0.40250.56680.60180.071*
H11B0.31630.52540.52890.071*
H11C0.39450.44190.60140.071*
C120.2548 (8)0.4974 (6)0.7718 (5)0.0404 (17)
H12A0.17220.50130.82010.061*
H12B0.31460.55160.77950.061*
H12C0.30510.42670.78020.061*
C130.2416 (7)0.8565 (5)0.8293 (5)0.0272 (14)
C140.2933 (7)0.9408 (6)0.7443 (5)0.0357 (16)
H14A0.35360.98610.76670.054*
H14B0.21370.98480.72210.054*
H14C0.34500.90390.69130.054*
C150.3681 (7)0.7807 (6)0.8598 (6)0.0372 (17)
H15A0.40820.73880.80690.056*
H15B0.33720.73270.91670.056*
H15C0.43790.82310.87460.056*
C160.1758 (7)0.9226 (6)0.9143 (5)0.0325 (15)
H16A0.14290.87400.97040.049*
H16B0.09790.97100.89470.049*
H16C0.24540.96390.93100.049*
C170.0675 (7)0.7289 (6)0.9314 (5)0.0307 (15)
C180.1839 (10)0.6535 (7)0.9350 (6)0.046 (2)
H18A0.14250.58420.91610.069*
H18B0.24860.68490.89070.069*
H18C0.23350.64421.00060.069*
C190.1423 (8)0.8414 (7)0.9559 (6)0.0413 (18)
H19A0.20300.86890.90780.062*
H19B0.07280.89110.95540.062*
H19C0.19740.83361.01980.062*
C200.0272 (10)0.6783 (7)1.0085 (5)0.045 (2)
H20A0.02790.67311.07240.068*
H20B0.10230.72331.00790.068*
H20C0.06640.60710.99340.068*
H40.114 (6)0.598 (4)0.756 (4)0.025*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0210 (2)0.0424 (3)0.0447 (3)0.00242 (19)0.00730 (19)0.0019 (2)
I20.0357 (3)0.0322 (3)0.1383 (7)0.0013 (2)0.0245 (4)0.0235 (3)
I30.0358 (3)0.0684 (4)0.0254 (2)0.0226 (2)0.00118 (19)0.0007 (2)
I40.0297 (3)0.0602 (3)0.0272 (2)0.0022 (2)0.00935 (19)0.0003 (2)
Ga10.0176 (3)0.0277 (4)0.0287 (4)0.0029 (3)0.0049 (3)0.0014 (3)
P10.0191 (8)0.0363 (9)0.0293 (8)0.0060 (7)0.0070 (7)0.0006 (7)
P20.0228 (9)0.0468 (11)0.0264 (8)0.0010 (8)0.0067 (7)0.0158 (8)
P30.0144 (7)0.0311 (9)0.0238 (8)0.0012 (6)0.0031 (6)0.0088 (6)
P40.0143 (7)0.0245 (8)0.0240 (7)0.0010 (6)0.0034 (6)0.0076 (6)
C10.012 (3)0.026 (3)0.029 (3)0.000 (2)0.004 (2)0.008 (2)
C20.017 (3)0.029 (3)0.024 (3)0.001 (2)0.004 (2)0.009 (2)
C30.023 (3)0.021 (3)0.024 (3)0.002 (2)0.008 (2)0.008 (2)
C40.023 (3)0.023 (3)0.023 (3)0.001 (2)0.004 (2)0.007 (2)
C50.018 (3)0.035 (4)0.031 (3)0.001 (3)0.009 (3)0.002 (3)
C60.027 (4)0.057 (5)0.052 (5)0.003 (4)0.014 (3)0.003 (4)
C70.017 (3)0.037 (4)0.051 (4)0.004 (3)0.009 (3)0.008 (3)
C80.029 (4)0.046 (5)0.063 (5)0.009 (3)0.015 (4)0.024 (4)
C90.020 (3)0.031 (4)0.045 (4)0.006 (3)0.006 (3)0.017 (3)
C100.035 (4)0.034 (4)0.107 (8)0.003 (4)0.012 (5)0.032 (5)
C110.045 (5)0.047 (5)0.047 (4)0.018 (4)0.001 (4)0.020 (4)
C120.038 (4)0.036 (4)0.044 (4)0.012 (3)0.011 (3)0.002 (3)
C130.022 (3)0.034 (4)0.031 (3)0.002 (3)0.008 (3)0.018 (3)
C140.026 (4)0.039 (4)0.046 (4)0.002 (3)0.009 (3)0.021 (3)
C150.026 (4)0.049 (4)0.041 (4)0.004 (3)0.013 (3)0.020 (3)
C160.023 (3)0.038 (4)0.041 (4)0.002 (3)0.009 (3)0.020 (3)
C170.032 (4)0.037 (4)0.021 (3)0.001 (3)0.001 (3)0.007 (3)
C180.056 (5)0.046 (5)0.037 (4)0.022 (4)0.009 (4)0.011 (3)
C190.031 (4)0.048 (5)0.043 (4)0.002 (3)0.010 (3)0.020 (4)
C200.061 (6)0.049 (5)0.022 (3)0.001 (4)0.002 (3)0.004 (3)
Geometric parameters (Å, º) top
I1—Ga12.5442 (11)C9—C111.531 (10)
I2—Ga12.5590 (10)C10—H10A0.9600
I3—Ga12.5290 (12)C10—H10B0.9600
I4—Ga12.5513 (10)C10—H10C0.9600
P1—C11.869 (6)C11—H11A0.9600
P1—P22.214 (3)C11—H11B0.9600
P1—P32.249 (2)C11—H11C0.9600
P2—C11.893 (6)C12—H12A0.9600
P2—C21.950 (6)C12—H12B0.9600
P3—C21.875 (6)C12—H12C0.9600
P3—C31.882 (6)C13—C151.535 (10)
P4—C21.781 (6)C13—C161.539 (8)
P4—C41.801 (6)C13—C141.540 (10)
P4—C11.807 (7)C14—H14A0.9600
P4—H41.33 (2)C14—H14B0.9600
C1—C51.542 (8)C14—H14C0.9600
C2—C91.542 (9)C15—H15A0.9600
C3—C41.366 (9)C15—H15B0.9600
C3—C131.561 (8)C15—H15C0.9600
C4—C171.550 (9)C16—H16A0.9600
C5—C81.507 (10)C16—H16B0.9600
C5—C61.529 (10)C16—H16C0.9600
C5—C71.533 (9)C17—C181.531 (10)
C6—H6A0.9600C17—C201.542 (11)
C6—H6B0.9600C17—C191.555 (10)
C6—H6C0.9600C18—H18A0.9600
C7—H7A0.9600C18—H18B0.9600
C7—H7B0.9600C18—H18C0.9600
C7—H7C0.9600C19—H19A0.9600
C8—H8A0.9600C19—H19B0.9600
C8—H8B0.9600C19—H19C0.9600
C8—H8C0.9600C20—H20A0.9600
C9—C101.511 (10)C20—H20B0.9600
C9—C121.512 (10)C20—H20C0.9600
I3—Ga1—I1110.29 (4)C11—C9—C2108.2 (6)
I3—Ga1—I4106.99 (3)C9—C10—H10A109.5
I1—Ga1—I4110.60 (4)C9—C10—H10B109.5
I3—Ga1—I2109.85 (4)H10A—C10—H10B109.5
I1—Ga1—I2107.91 (4)C9—C10—H10C109.5
I4—Ga1—I2111.21 (4)H10A—C10—H10C109.5
C1—P1—P254.46 (19)H10B—C10—H10C109.5
C1—P1—P394.8 (2)C9—C11—H11A109.5
P2—P1—P381.26 (9)C9—C11—H11B109.5
C1—P2—C281.5 (3)H11A—C11—H11B109.5
C1—P2—P153.5 (2)C9—C11—H11C109.5
C2—P2—P185.4 (2)H11A—C11—H11C109.5
C2—P3—C398.9 (3)H11B—C11—H11C109.5
C2—P3—P186.2 (2)C9—C12—H12A109.5
C3—P3—P1100.8 (2)C9—C12—H12B109.5
C2—P4—C4107.6 (3)H12A—C12—H12B109.5
C2—P4—C188.8 (3)C9—C12—H12C109.5
C4—P4—C1117.7 (3)H12A—C12—H12C109.5
C2—P4—H4113 (3)H12B—C12—H12C109.5
C4—P4—H4116 (3)C15—C13—C16109.6 (5)
C1—P4—H4110 (3)C15—C13—C14109.5 (6)
C5—C1—P4124.4 (4)C16—C13—C14105.5 (6)
C5—C1—P1119.8 (5)C15—C13—C3106.0 (5)
P4—C1—P1108.4 (3)C16—C13—C3117.6 (5)
C5—C1—P2126.6 (4)C14—C13—C3108.5 (5)
P4—C1—P292.2 (3)C13—C14—H14A109.5
P1—C1—P272.1 (2)C13—C14—H14B109.5
C9—C2—P4124.3 (5)H14A—C14—H14B109.5
C9—C2—P3118.2 (4)C13—C14—H14C109.5
P4—C2—P395.5 (3)H14A—C14—H14C109.5
C9—C2—P2122.1 (4)H14B—C14—H14C109.5
P4—C2—P291.2 (3)C13—C15—H15A109.5
P3—C2—P298.9 (3)C13—C15—H15B109.5
C4—C3—C13135.0 (5)H15A—C15—H15B109.5
C4—C3—P3116.6 (4)C13—C15—H15C109.5
C13—C3—P3108.3 (4)H15A—C15—H15C109.5
C3—C4—C17134.0 (5)H15B—C15—H15C109.5
C3—C4—P4105.7 (4)C13—C16—H16A109.5
C17—C4—P4120.3 (5)C13—C16—H16B109.5
C8—C5—C6110.0 (6)H16A—C16—H16B109.5
C8—C5—C7110.1 (6)C13—C16—H16C109.5
C6—C5—C7108.2 (6)H16A—C16—H16C109.5
C8—C5—C1109.1 (5)H16B—C16—H16C109.5
C6—C5—C1109.6 (5)C18—C17—C20107.1 (6)
C7—C5—C1109.8 (5)C18—C17—C4110.8 (5)
C5—C6—H6A109.5C20—C17—C4109.0 (6)
C5—C6—H6B109.5C18—C17—C19106.7 (6)
H6A—C6—H6B109.5C20—C17—C19112.0 (6)
C5—C6—H6C109.5C4—C17—C19111.3 (6)
H6A—C6—H6C109.5C17—C18—H18A109.5
H6B—C6—H6C109.5C17—C18—H18B109.5
C5—C7—H7A109.5H18A—C18—H18B109.5
C5—C7—H7B109.5C17—C18—H18C109.5
H7A—C7—H7B109.5H18A—C18—H18C109.5
C5—C7—H7C109.5H18B—C18—H18C109.5
H7A—C7—H7C109.5C17—C19—H19A109.5
H7B—C7—H7C109.5C17—C19—H19B109.5
C5—C8—H8A109.5H19A—C19—H19B109.5
C5—C8—H8B109.5C17—C19—H19C109.5
H8A—C8—H8B109.5H19A—C19—H19C109.5
C5—C8—H8C109.5H19B—C19—H19C109.5
H8A—C8—H8C109.5C17—C20—H20A109.5
H8B—C8—H8C109.5C17—C20—H20B109.5
C10—C9—C12109.2 (7)H20A—C20—H20B109.5
C10—C9—C11110.4 (6)C17—C20—H20C109.5
C12—C9—C11109.3 (6)H20A—C20—H20C109.5
C10—C9—C2109.7 (6)H20B—C20—H20C109.5
C12—C9—C2110.0 (5)
P3—P1—P2—C1102.4 (2)P1—P3—C3—C470.6 (5)
C1—P1—P2—C282.9 (3)C2—P3—C3—C13161.5 (4)
P3—P1—P2—C219.49 (19)P1—P3—C3—C13110.8 (4)
C1—P1—P3—C232.6 (3)C13—C3—C4—C177.4 (13)
P2—P1—P3—C220.28 (19)P3—C3—C4—C17170.7 (6)
C1—P1—P3—C365.7 (3)C13—C3—C4—P4174.6 (6)
P2—P1—P3—C3118.6 (2)P3—C3—C4—P47.3 (6)
C2—P4—C1—C5158.2 (5)C2—P4—C4—C331.7 (5)
C4—P4—C1—C592.5 (5)C1—P4—C4—C366.5 (5)
C2—P4—C1—P152.1 (3)C2—P4—C4—C17146.7 (5)
C4—P4—C1—P157.2 (4)C1—P4—C4—C17115.1 (5)
C2—P4—C1—P219.7 (3)P4—C1—C5—C866.6 (7)
C4—P4—C1—P2129.1 (3)P1—C1—C5—C879.9 (7)
P2—P1—C1—C5122.4 (5)P2—C1—C5—C8169.0 (5)
P3—P1—C1—C5161.9 (4)P4—C1—C5—C6173.0 (5)
P2—P1—C1—P486.3 (3)P1—C1—C5—C640.5 (7)
P3—P1—C1—P410.6 (3)P2—C1—C5—C648.5 (8)
P3—P1—C1—P275.67 (16)P4—C1—C5—C754.2 (7)
C2—P2—C1—C5155.2 (6)P1—C1—C5—C7159.3 (5)
P1—P2—C1—C5114.2 (6)P2—C1—C5—C770.2 (7)
C2—P2—C1—P418.1 (3)P4—C2—C9—C1061.1 (8)
P1—P2—C1—P4108.7 (3)P3—C2—C9—C10179.1 (6)
C2—P2—C1—P190.5 (2)P2—C2—C9—C1056.1 (8)
C4—P4—C2—C991.0 (6)P4—C2—C9—C1259.0 (7)
C1—P4—C2—C9150.3 (5)P3—C2—C9—C1260.8 (7)
C4—P4—C2—P338.8 (3)P2—C2—C9—C12176.3 (5)
C1—P4—C2—P379.9 (3)P4—C2—C9—C11178.4 (5)
C4—P4—C2—P2137.8 (3)P3—C2—C9—C1158.6 (7)
C1—P4—C2—P219.1 (3)P2—C2—C9—C1164.3 (7)
C3—P3—C2—C9102.5 (5)C4—C3—C13—C15101.7 (8)
P1—P3—C2—C9157.2 (5)P3—C3—C13—C1576.5 (6)
C3—P3—C2—P431.5 (3)C4—C3—C13—C1621.3 (11)
P1—P3—C2—P468.9 (2)P3—C3—C13—C16160.5 (5)
C3—P3—C2—P2123.5 (3)C4—C3—C13—C14140.9 (7)
P1—P3—C2—P223.2 (2)P3—C3—C13—C1440.9 (6)
C1—P2—C2—C9151.2 (6)C3—C4—C17—C18171.7 (7)
P1—P2—C2—C9155.1 (5)P4—C4—C17—C186.1 (8)
C1—P2—C2—P418.4 (3)C3—C4—C17—C2054.1 (10)
P1—P2—C2—P472.1 (2)P4—C4—C17—C20123.7 (6)
C1—P2—C2—P377.3 (3)C3—C4—C17—C1969.8 (10)
P1—P2—C2—P323.6 (2)P4—C4—C17—C19112.3 (6)
C2—P3—C3—C417.1 (5)
(II) triiodo(3,5,7,8-tetra-tert-butyl-1,2,4λ5,6- tetraphosphatetracyclo[4.1.1.02,5.07,8]octan-4-one)gallium top
Crystal data top
[GaI3(C20H38OP4)]F(000) = 1664
Mr = 868.80Dx = 1.903 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 12.082 (2) ÅCell parameters from 66215 reflections
b = 17.522 (4) Åθ = 2.9–27.5°
c = 14.615 (3) ŵ = 4.18 mm1
β = 101.47 (3)°T = 150 K
V = 3032.2 (10) Å3Square prism, yellow
Z = 40.30 × 0.30 × 0.10 mm
Data collection top
Nonius KappaCCD
diffractometer
6923 independent reflections
Radiation source: fine-focus sealed tube6141 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.132
ϕ and ω scans to fill Ewald sphereθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
h = 1515
Tmin = 0.302, Tmax = 0.658k = 2222
50118 measured reflectionsl = 1818
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)] = 0.033H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.081 w = 1/[σ2(Fo2) + (0.01P)2 + 7.857P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.002
6923 reflectionsΔρmax = 1.12 e Å3
279 parametersΔρmin = 1.48 e Å3
13 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00049 (10)
Crystal data top
[GaI3(C20H38OP4)]V = 3032.2 (10) Å3
Mr = 868.80Z = 4
Monoclinic, P21/cMo Kα radiation
a = 12.082 (2) ŵ = 4.18 mm1
b = 17.522 (4) ÅT = 150 K
c = 14.615 (3) Å0.30 × 0.30 × 0.10 mm
β = 101.47 (3)°
Data collection top
Nonius KappaCCD
diffractometer
6923 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
6141 reflections with I > 2σ(I)
Tmin = 0.302, Tmax = 0.658Rint = 0.132
50118 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03313 restraints
wR(F2) = 0.081H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 1.12 e Å3
6923 reflectionsΔρmin = 1.48 e Å3
279 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. H(21) was located from difference maps, its distance from P(1) was fixed at 1.33 angstroms using the DFIX command. Its U(iso) was allowed to refine freely.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.39969 (2)0.181500 (18)0.98121 (2)0.03477 (9)
I20.18517 (2)0.160647 (17)1.174780 (16)0.03093 (9)
I30.07776 (3)0.286179 (16)0.923772 (19)0.03541 (9)
Ga10.19902 (3)0.18115 (2)1.00780 (3)0.01995 (10)
P10.14428 (7)0.05323 (5)0.85233 (6)0.01767 (18)
P20.09661 (8)0.06783 (5)0.75099 (6)0.01818 (19)
P30.18704 (8)0.03818 (6)0.63786 (6)0.01996 (19)
P40.35355 (7)0.03525 (6)0.81141 (6)0.01871 (19)
O10.1368 (2)0.09132 (15)0.94456 (17)0.0231 (5)
C10.0151 (3)0.0187 (2)0.7819 (2)0.0180 (7)
H10.03160.00010.82660.022*
C20.2140 (3)0.0388 (2)0.8517 (2)0.0169 (7)
C30.3209 (3)0.0075 (2)0.6955 (2)0.0203 (7)
C40.3224 (3)0.0800 (2)0.6950 (2)0.0198 (7)
C50.0650 (3)0.0674 (2)0.7090 (2)0.0219 (7)
C60.1407 (4)0.1146 (3)0.7597 (3)0.0384 (11)
H6A0.09380.14810.80530.058*
H6B0.18430.08030.79200.058*
H6C0.19240.14550.71420.058*
C70.0021 (4)0.1205 (3)0.6549 (3)0.0367 (10)
H7A0.04300.15670.69800.055*
H7B0.05660.14860.60820.055*
H7C0.04780.09050.62340.055*
C80.1379 (4)0.0118 (3)0.6406 (3)0.0358 (10)
H8A0.19450.04070.59670.054*
H8B0.17590.02410.67550.054*
H8C0.08960.01650.60590.054*
C90.2241 (3)0.0897 (2)0.9418 (2)0.0223 (8)
C100.1118 (3)0.0947 (3)0.9740 (3)0.0292 (9)
H10A0.05490.11780.92450.044*
H10B0.08730.04330.98770.044*
H10C0.12090.12621.03040.044*
C110.2592 (4)0.1702 (2)0.9198 (3)0.0321 (9)
H11A0.26460.20240.97540.048*
H11B0.33270.16840.90120.048*
H11C0.20270.19160.86880.048*
C120.3137 (3)0.0553 (3)1.0219 (3)0.0279 (8)
H12A0.31810.08631.07840.042*
H12B0.29220.00301.03440.042*
H12C0.38750.05491.00370.042*
C130.3834 (3)0.0721 (2)0.6566 (3)0.0252 (8)
C140.5095 (5)0.0663 (4)0.6922 (5)0.0667 (17)
H14A0.52570.06660.76060.100*
H14B0.54710.10980.66920.100*
H14C0.53750.01870.66980.100*
C150.3401 (5)0.1479 (3)0.6869 (3)0.0425 (11)
H15A0.35430.15040.75520.064*
H15B0.25880.15210.66210.064*
H15C0.37940.19010.66290.064*
C160.3582 (5)0.0716 (3)0.5494 (3)0.0486 (13)
H16A0.39260.11650.52640.073*
H16B0.27630.07270.52630.073*
H16C0.38960.02520.52710.073*
C170.3846 (3)0.1458 (2)0.6584 (3)0.0273 (8)
C180.5085 (4)0.1476 (4)0.7065 (4)0.0572 (15)
H18A0.54620.10150.69030.086*
H18B0.54470.19270.68590.086*
H18C0.51420.14980.77430.086*
C190.3284 (6)0.2198 (3)0.6802 (4)0.0519 (14)
H19A0.33930.22630.74800.078*
H19B0.36250.26300.65330.078*
H19C0.24750.21770.65320.078*
C200.3734 (4)0.1403 (3)0.5526 (3)0.0375 (10)
H20A0.29350.13590.52290.056*
H20B0.40540.18630.52960.056*
H20C0.41440.09530.53730.056*
H210.192 (3)0.097 (2)0.796 (3)0.033 (12)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.02387 (14)0.04394 (19)0.03882 (16)0.00591 (11)0.01181 (11)0.00404 (13)
I20.03157 (15)0.04094 (18)0.01973 (13)0.01160 (11)0.00377 (10)0.00137 (11)
I30.04414 (17)0.02641 (16)0.03408 (15)0.00774 (12)0.00391 (12)0.00569 (11)
Ga10.0217 (2)0.0192 (2)0.01904 (19)0.00196 (15)0.00436 (15)0.00208 (16)
P10.0173 (4)0.0179 (4)0.0177 (4)0.0000 (3)0.0032 (3)0.0011 (4)
P20.0186 (4)0.0173 (5)0.0177 (4)0.0013 (3)0.0013 (3)0.0003 (3)
P30.0182 (4)0.0246 (5)0.0163 (4)0.0020 (4)0.0017 (3)0.0002 (4)
P40.0164 (4)0.0209 (5)0.0182 (4)0.0010 (3)0.0020 (3)0.0003 (4)
O10.0235 (13)0.0224 (14)0.0239 (12)0.0029 (11)0.0059 (10)0.0065 (11)
C10.0207 (16)0.0181 (18)0.0145 (15)0.0010 (13)0.0018 (13)0.0005 (13)
C20.0177 (16)0.0168 (17)0.0161 (15)0.0009 (13)0.0030 (12)0.0008 (13)
C30.0219 (17)0.0184 (18)0.0206 (16)0.0015 (14)0.0039 (13)0.0003 (14)
C40.0194 (17)0.0191 (18)0.0206 (16)0.0002 (14)0.0037 (13)0.0001 (14)
C50.0203 (17)0.0240 (19)0.0197 (17)0.0051 (14)0.0004 (14)0.0006 (15)
C60.031 (2)0.051 (3)0.031 (2)0.018 (2)0.0021 (17)0.002 (2)
C70.033 (2)0.034 (2)0.044 (2)0.0078 (19)0.0086 (19)0.020 (2)
C80.039 (2)0.035 (2)0.027 (2)0.0019 (19)0.0095 (18)0.0033 (18)
C90.0264 (18)0.024 (2)0.0158 (16)0.0010 (15)0.0023 (14)0.0038 (15)
C100.029 (2)0.037 (2)0.0223 (18)0.0027 (17)0.0058 (15)0.0070 (17)
C110.042 (2)0.024 (2)0.028 (2)0.0034 (18)0.0019 (17)0.0048 (17)
C120.029 (2)0.033 (2)0.0199 (17)0.0025 (17)0.0005 (15)0.0011 (17)
C130.0242 (18)0.024 (2)0.0291 (19)0.0017 (15)0.0091 (15)0.0020 (16)
C140.038 (3)0.068 (3)0.091 (4)0.011 (2)0.006 (2)0.034 (3)
C150.065 (3)0.026 (2)0.044 (3)0.010 (2)0.028 (2)0.003 (2)
C160.085 (4)0.035 (3)0.035 (2)0.011 (3)0.035 (3)0.002 (2)
C170.0269 (19)0.029 (2)0.0252 (18)0.0092 (16)0.0047 (15)0.0043 (17)
C180.040 (2)0.065 (3)0.061 (3)0.021 (2)0.003 (2)0.030 (3)
C190.089 (4)0.024 (2)0.051 (3)0.013 (2)0.034 (3)0.002 (2)
C200.057 (3)0.031 (2)0.030 (2)0.011 (2)0.019 (2)0.0039 (19)
Geometric parameters (Å, º) top
I1—Ga12.5305 (7)C9—C111.526 (6)
I2—Ga12.5050 (7)C9—C121.550 (5)
I3—Ga12.5152 (7)C10—H10A0.9800
Ga1—O11.903 (3)C10—H10B0.9800
P1—O11.523 (3)C10—H10C0.9800
P1—C11.795 (4)C11—H11A0.9800
P1—C21.819 (4)C11—H11B0.9800
P1—H211.33 (2)C11—H11C0.9800
P2—C21.899 (3)C12—H12A0.9800
P2—C11.911 (4)C12—H12B0.9800
P2—P32.2171 (14)C12—H12C0.9800
P3—C41.835 (4)C13—C141.512 (7)
P3—C31.851 (4)C13—C161.535 (6)
P4—C31.823 (4)C13—C151.526 (6)
P4—C41.842 (4)C14—H14A0.9800
P4—C21.895 (4)C14—H14B0.9800
C1—C51.545 (5)C14—H14C0.9800
C1—H11.0000C15—H15A0.9800
C2—C91.575 (5)C15—H15B0.9800
C3—C131.531 (5)C15—H15C0.9800
C3—C41.534 (5)C16—H16A0.9800
C4—C171.530 (5)C16—H16B0.9800
C5—C71.520 (6)C16—H16C0.9800
C5—C61.529 (6)C17—C191.526 (7)
C5—C81.541 (6)C17—C201.529 (5)
C6—H6A0.9800C17—C181.522 (6)
C6—H6B0.9800C18—H18A0.9800
C6—H6C0.9800C18—H18B0.9800
C7—H7A0.9800C18—H18C0.9800
C7—H7B0.9800C19—H19A0.9800
C7—H7C0.9800C19—H19B0.9800
C8—H8A0.9800C19—H19C0.9800
C8—H8B0.9800C20—H20A0.9800
C8—H8C0.9800C20—H20B0.9800
C9—C101.525 (5)C20—H20C0.9800
O1—Ga1—I2104.97 (8)C10—C9—C12108.7 (3)
O1—Ga1—I3103.46 (8)C11—C9—C12109.7 (3)
I2—Ga1—I3115.81 (2)C10—C9—C2111.4 (3)
O1—Ga1—I1103.02 (8)C11—C9—C2109.0 (3)
I2—Ga1—I1113.68 (3)C12—C9—C2109.8 (3)
I3—Ga1—I1113.96 (2)C9—C10—H10A109.5
O1—P1—C1117.21 (16)C9—C10—H10B109.5
O1—P1—C2120.11 (15)H10A—C10—H10B109.5
C1—P1—C292.83 (16)C9—C10—H10C109.5
O1—P1—H21114 (2)H10A—C10—H10C109.5
C1—P1—H21105.7 (19)H10B—C10—H10C109.5
C2—P1—H21104 (2)C9—C11—H11A109.5
C2—P2—C186.80 (15)C9—C11—H11B109.5
C2—P2—P396.46 (11)H11A—C11—H11B109.5
C1—P2—P3110.13 (12)C9—C11—H11C109.5
C4—P3—C349.18 (16)H11A—C11—H11C109.5
C4—P3—P295.39 (12)H11B—C11—H11C109.5
C3—P3—P2106.12 (12)C9—C12—H12A109.5
C3—P4—C449.47 (16)C9—C12—H12B109.5
C3—P4—C2105.11 (16)H12A—C12—H12B109.5
C4—P4—C2104.02 (16)C9—C12—H12C109.5
P1—O1—Ga1134.87 (17)H12A—C12—H12C109.5
C5—C1—P1124.3 (3)H12B—C12—H12C109.5
C5—C1—P2123.8 (2)C14—C13—C16109.4 (4)
P1—C1—P288.42 (16)C14—C13—C15109.8 (4)
C5—C1—H1106.0C16—C13—C15107.0 (4)
P1—C1—H1106.0C14—C13—C3111.1 (4)
P2—C1—H1106.0C16—C13—C3111.2 (3)
C9—C2—P1117.2 (2)C15—C13—C3108.2 (3)
C9—C2—P2114.7 (2)C13—C14—H14A109.5
P1—C2—P288.09 (15)C13—C14—H14B109.5
C9—C2—P4110.6 (2)H14A—C14—H14B109.5
P1—C2—P4114.46 (18)C13—C14—H14C109.5
P2—C2—P4109.96 (17)H14A—C14—H14C109.5
C13—C3—C4136.9 (3)H14B—C14—H14C109.5
C13—C3—P4128.1 (3)C13—C15—H15A109.5
C4—C3—P465.94 (19)C13—C15—H15B109.5
C13—C3—P3127.0 (3)H15A—C15—H15B109.5
C4—C3—P364.87 (19)C13—C15—H15C109.5
P4—C3—P3104.66 (19)H15A—C15—H15C109.5
C17—C4—C3139.7 (3)H15B—C15—H15C109.5
C17—C4—P3126.6 (3)C13—C16—H16A109.5
C3—C4—P365.95 (19)C13—C16—H16B109.5
C17—C4—P4128.3 (3)H16A—C16—H16B109.5
C3—C4—P464.59 (19)C13—C16—H16C109.5
P3—C4—P4104.50 (18)H16A—C16—H16C109.5
C7—C5—C6109.2 (4)H16B—C16—H16C109.5
C7—C5—C8109.3 (3)C19—C17—C20108.1 (4)
C6—C5—C8109.7 (4)C19—C17—C4107.4 (3)
C7—C5—C1112.8 (3)C20—C17—C4110.9 (3)
C6—C5—C1108.5 (3)C19—C17—C18108.8 (4)
C8—C5—C1107.3 (3)C20—C17—C18110.4 (4)
C5—C6—H6A109.5C4—C17—C18111.1 (3)
C5—C6—H6B109.5C17—C18—H18A109.5
H6A—C6—H6B109.5C17—C18—H18B109.5
C5—C6—H6C109.5H18A—C18—H18B109.5
H6A—C6—H6C109.5C17—C18—H18C109.5
H6B—C6—H6C109.5H18A—C18—H18C109.5
C5—C7—H7A109.5H18B—C18—H18C109.5
C5—C7—H7B109.5C17—C19—H19A109.5
H7A—C7—H7B109.5C17—C19—H19B109.5
C5—C7—H7C109.5H19A—C19—H19B109.5
H7A—C7—H7C109.5C17—C19—H19C109.5
H7B—C7—H7C109.5H19A—C19—H19C109.5
C5—C8—H8A109.5H19B—C19—H19C109.5
C5—C8—H8B109.5C17—C20—H20A109.5
H8A—C8—H8B109.5C17—C20—H20B109.5
C5—C8—H8C109.5H20A—C20—H20B109.5
H8A—C8—H8C109.5C17—C20—H20C109.5
H8B—C8—H8C109.5H20A—C20—H20C109.5
C10—C9—C11108.2 (3)H20B—C20—H20C109.5
C2—P2—P3—C443.55 (16)C13—C3—C4—P3118.1 (4)
C1—P2—P3—C4132.50 (16)P4—C3—C4—P3121.03 (16)
C2—P2—P3—C35.44 (17)C13—C3—C4—P4120.8 (4)
C1—P2—P3—C383.51 (17)P3—C3—C4—P4121.03 (16)
C1—P1—O1—Ga1135.4 (2)C3—P3—C4—C17135.1 (4)
C2—P1—O1—Ga1113.4 (2)P2—P3—C4—C17118.2 (3)
I2—Ga1—O1—P1160.3 (2)P2—P3—C4—C3106.68 (18)
I3—Ga1—O1—P177.9 (2)C3—P3—C4—P453.08 (19)
I1—Ga1—O1—P141.0 (2)P2—P3—C4—P453.60 (16)
O1—P1—C1—C587.8 (3)C3—P4—C4—C17134.5 (4)
C2—P1—C1—C5146.0 (3)C2—P4—C4—C17127.5 (3)
O1—P1—C1—P2141.31 (15)C2—P4—C4—C398.1 (2)
C2—P1—C1—P215.14 (15)C3—P4—C4—P353.9 (2)
C2—P2—C1—C5145.8 (3)C2—P4—C4—P344.1 (2)
P3—P2—C1—C550.1 (3)P1—C1—C5—C738.7 (4)
C2—P2—C1—P114.50 (15)P2—C1—C5—C775.9 (4)
P3—P2—C1—P181.22 (13)P1—C1—C5—C682.5 (4)
O1—P1—C2—C922.2 (3)P2—C1—C5—C6162.9 (3)
C1—P1—C2—C9101.7 (3)P1—C1—C5—C8159.1 (3)
O1—P1—C2—P2139.15 (14)P2—C1—C5—C844.5 (4)
C1—P1—C2—P215.24 (16)P1—C2—C9—C1047.7 (4)
O1—P1—C2—P4109.7 (2)P2—C2—C9—C1053.6 (4)
C1—P1—C2—P4126.35 (19)P4—C2—C9—C10178.7 (3)
C1—P2—C2—C9104.9 (3)P1—C2—C9—C11167.0 (3)
P3—P2—C2—C9145.2 (2)P2—C2—C9—C1165.8 (4)
C1—P2—C2—P114.30 (15)P4—C2—C9—C1159.3 (3)
P3—P2—C2—P195.61 (11)P1—C2—C9—C1272.7 (3)
C1—P2—C2—P4129.69 (19)P2—C2—C9—C12174.0 (3)
P3—P2—C2—P419.78 (17)P4—C2—C9—C1260.9 (3)
C3—P4—C2—C9168.3 (2)C4—C3—C13—C1457.7 (6)
C4—P4—C2—C9117.1 (2)P4—C3—C13—C1436.9 (5)
C3—P4—C2—P156.7 (2)P3—C3—C13—C14149.2 (4)
C4—P4—C2—P1107.9 (2)C4—C3—C13—C1664.5 (6)
C3—P4—C2—P240.6 (2)P4—C3—C13—C16159.0 (3)
C4—P4—C2—P210.7 (2)P3—C3—C13—C1627.1 (5)
C4—P4—C3—C13131.7 (4)C4—C3—C13—C15178.3 (4)
C2—P4—C3—C13132.6 (3)P4—C3—C13—C1583.8 (4)
C2—P4—C3—C495.7 (2)P3—C3—C13—C1590.2 (4)
C4—P4—C3—P353.31 (19)C3—C4—C17—C19175.0 (4)
C2—P4—C3—P342.4 (2)P3—C4—C17—C1979.7 (4)
C4—P3—C3—C13131.0 (4)P4—C4—C17—C1990.1 (4)
P2—P3—C3—C13145.9 (3)C3—C4—C17—C2057.1 (6)
P2—P3—C3—C483.08 (18)P3—C4—C17—C2038.2 (5)
C4—P3—C3—P453.98 (19)P4—C4—C17—C20152.0 (3)
P2—P3—C3—P429.10 (19)C3—C4—C17—C1866.1 (6)
C13—C3—C4—C170.8 (8)P3—C4—C17—C18161.4 (4)
P4—C3—C4—C17120.0 (5)P4—C4—C17—C1828.8 (5)
P3—C3—C4—C17119.0 (5)

Experimental details

(I)(II)
Crystal data
Chemical formula(C20H37P4)[GaI4][GaI3(C20H38OP4)]
Mr978.70868.80
Crystal system, space groupTriclinic, P1Monoclinic, P21/c
Temperature (K)150150
a, b, c (Å)9.6290 (19), 12.459 (3), 13.867 (3)12.082 (2), 17.522 (4), 14.615 (3)
α, β, γ (°)82.91 (3), 81.28 (3), 83.65 (3)90, 101.47 (3), 90
V3)1624.6 (6)3032.2 (10)
Z24
Radiation typeMo KαMo Kα
µ (mm1)4.854.18
Crystal size (mm)0.15 × 0.15 × 0.070.30 × 0.30 × 0.10
Data collection
DiffractometerNonius KappaCCD
diffractometer
Nonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(SORTAV; Blessing, 1995)
Multi-scan
(SORTAV; Blessing, 1995)
Tmin, Tmax0.471, 0.7120.302, 0.658
No. of measured, independent and
observed [I > 2σ(I)] reflections
25682, 7382, 5661 50118, 6923, 6141
Rint0.1310.132
(sin θ/λ)max1)0.6490.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.057, 0.151, 1.04 0.033, 0.081, 1.04
No. of reflections73826923
No. of parameters277279
No. of restraints113
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)2.15, 2.691.12, 1.48

Computer programs: COLLECT (Hooft, 2000), DENZO–SMN (Otwinowski & Minor, 1997), DENZO–SMN, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), SHELXL97.

Selected geometric parameters (Å, º) for (I) top
I1—Ga12.5442 (11)P2—C21.950 (6)
I2—Ga12.5590 (10)P3—C21.875 (6)
I3—Ga12.5290 (12)P3—C31.882 (6)
I4—Ga12.5513 (10)P4—C21.781 (6)
P1—C11.869 (6)P4—C41.801 (6)
P1—P22.214 (3)P4—C11.807 (7)
P1—P32.249 (2)P4—H41.33 (2)
P2—C11.893 (6)C3—C41.366 (9)
I3—Ga1—I1110.29 (4)C1—P4—H4110 (3)
I3—Ga1—I4106.99 (3)C5—C1—P4124.4 (4)
I1—Ga1—I4110.60 (4)C5—C1—P1119.8 (5)
I3—Ga1—I2109.85 (4)P4—C1—P1108.4 (3)
I1—Ga1—I2107.91 (4)C5—C1—P2126.6 (4)
I4—Ga1—I2111.21 (4)P4—C1—P292.2 (3)
C1—P1—P254.46 (19)P1—C1—P272.1 (2)
C1—P1—P394.8 (2)C9—C2—P4124.3 (5)
P2—P1—P381.26 (9)C9—C2—P3118.2 (4)
C1—P2—C281.5 (3)P4—C2—P395.5 (3)
C1—P2—P153.5 (2)C9—C2—P2122.1 (4)
C2—P2—P185.4 (2)P4—C2—P291.2 (3)
C2—P3—C398.9 (3)P3—C2—P298.9 (3)
C2—P3—P186.2 (2)C4—C3—C13135.0 (5)
C3—P3—P1100.8 (2)C4—C3—P3116.6 (4)
C2—P4—C4107.6 (3)C13—C3—P3108.3 (4)
C2—P4—C188.8 (3)C3—C4—C17134.0 (5)
C4—P4—C1117.7 (3)C3—C4—P4105.7 (4)
C2—P4—H4113 (3)C17—C4—P4120.3 (5)
C4—P4—H4116 (3)
Selected geometric parameters (Å, º) for (II) top
I1—Ga12.5305 (7)P2—P32.2171 (14)
I2—Ga12.5050 (7)P3—C41.835 (4)
I3—Ga12.5152 (7)P3—C31.851 (4)
Ga1—O11.903 (3)P4—C31.823 (4)
P1—O11.523 (3)P4—C41.842 (4)
P1—C11.795 (4)P4—C21.895 (4)
P1—C21.819 (4)C2—C91.575 (5)
P1—H211.33 (2)C3—C131.531 (5)
P2—C21.899 (3)C3—C41.534 (5)
P2—C11.911 (4)
O1—Ga1—I2104.97 (8)P1—C1—P288.42 (16)
O1—Ga1—I3103.46 (8)C5—C1—H1106.0
I2—Ga1—I3115.81 (2)P1—C1—H1106.0
O1—Ga1—I1103.02 (8)P2—C1—H1106.0
I2—Ga1—I1113.68 (3)C9—C2—P1117.2 (2)
I3—Ga1—I1113.96 (2)C9—C2—P2114.7 (2)
O1—P1—C1117.21 (16)P1—C2—P288.09 (15)
O1—P1—C2120.11 (15)C9—C2—P4110.6 (2)
C1—P1—C292.83 (16)P1—C2—P4114.46 (18)
O1—P1—H21114 (2)P2—C2—P4109.96 (17)
C1—P1—H21105.7 (19)C13—C3—C4136.9 (3)
C2—P1—H21104 (2)C13—C3—P4128.1 (3)
C2—P2—C186.80 (15)C4—C3—P465.94 (19)
C2—P2—P396.46 (11)C13—C3—P3127.0 (3)
C1—P2—P3110.13 (12)C4—C3—P364.87 (19)
C4—P3—C349.18 (16)P4—C3—P3104.66 (19)
C4—P3—P295.39 (12)C17—C4—C3139.7 (3)
C3—P3—P2106.12 (12)C17—C4—P3126.6 (3)
C3—P4—C449.47 (16)C3—C4—P365.95 (19)
C3—P4—C2105.11 (16)C17—C4—P4128.3 (3)
C4—P4—C2104.02 (16)C3—C4—P464.59 (19)
P1—O1—Ga1134.87 (17)P3—C4—P4104.50 (18)
C5—C1—P1124.3 (3)C7—C5—C6109.2 (4)
C5—C1—P2123.8 (2)
 

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