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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2020 Jun 23;76(Pt 7):1131–1135. doi: 10.1107/S2056989020008051

Crystal structure of the [(THF)Cs(μ-η55-Cp′)3Yb]n oligomer

Daniel N Huh a, Joseph W Ziller a, William J Evans a,*
PMCID: PMC7336790  PMID: 32695466

Reduction of (C5H4SiMe3)3YbIII in THF using excess Cs metal forms the oligomeric complex [(THF)Cs(μ-η55-Cp′)3YbII]n. The complex has hexa­gonal layers of Cs3Yb3 with THF ligands and Me3Si groups in between the layers.

Keywords: lanthanide, caesium, cyclo­penta­dienide, oligomer, crystal structure

Abstract

The green compound poly[(tetra­hydro­furan)­tris­[μ-η55-1-(tri­methyl­sil­yl)cyclo­penta­dien­yl]caesium(I)ytterbium(II)], [CsYb(C8H13Si)3(C4H8O)]n or [(THF)Cs(μ-η55-Cp′)3YbII]n was synthesized by reduction of a red THF solution of (C5H4SiMe3)3YbIII with excess Cs metal and identified by X-ray diffraction. The compound crystallizes as a two-dimensional array of hexa­gons with alternating CsI and YbII ions at the vertices and cyclo­penta­dienyl groups bridging each edge. This, based off the six-electron cyclo­penta­dienyl rings occupying three coordination positions, gives a formally nine-coordinate tris­(cyclo­penta­dien­yl) coordination environment to Yb and the Cs is ten-coordinate due to the three cyclo­penta­dienyl rings and a coordinated mol­ecule of THF. The complex comprises layers of Cs3Yb3 hexa­gons with THF ligands and Me3Si groups in between the layers. The Yb—C metrical parameters are consistent with a 4f 14 YbII electron configuration.

Chemical context  

The new +2 oxidation states for the rare-earth metals Y, La, Ce, Pr, Gd, Tb, Ho, Er, and Lu were recently discovered by reduction of Cpx 3 Ln (Cpx = C5H4SiMe3, C5H3(SiMe3)2; Ln = rare-earth metal) using alkali metal reductants Li, Na, K, and KC8 (Fig. 1) (Hitchcock et al., 2008; MacDonald et al., 2013; Fieser et al., 2015; Evans, 2016; Palumbo et al., 2018). In each of these cases, 2.2.2-cryptand was added in these reactions to encapsulate the alkali metal. It was thought that chelating agents were necessary to sequester the alkali metal to prevent inter­actions with cyclo­penta­dienide ligands and subsequent ligand dissociation leading to product decomposition. This idea was challenged by examining reduction reactions of Cp′′3 M (Cp′′ = C5H3(SiMe3)2; M = La, Ce, U) with Li and Cs in the absence of chelating agents (Huh et al., 2018). The reaction resulted in the isolation of the first chelate-free synthesis of LaII, CeII, and UII complexes. The [Li(THF)4]1+ cation of the Li salts in these chelate-free M II complexes were well-separated from the (Cp′′3 M)1− anion. However, the Cs reductions yielded polymeric complexes of general formula [Cp′′M(μ-Cp′′)2Cs(THF)2]n where the Cs cation has coord­in­ated THF and cyclo­penta­dienide ligands. Attempts to extend this chemistry to smaller rare-earth metals by reduction of Cp′3 Ln (Cp′ = C5H4SiMe3; Ln = Y, Tb, Dy) showed evidence of Ln II in solution; however, the reduction products were highly unstable and decomposed even at 238 K.graphic file with name e-76-01131-scheme1.jpg

Figure 1.

Figure 1

Synthesis of (Cpx 3 Ln II)1− complexes by alkali metal reduction of Cpx 3 Ln III precursors; Cpx = C5H4SiMe3, C5H3(SiMe3)2.

In this study, we were inter­ested in examining the reduction of Cp′3YbIII with Cs metal. Unlike YII, TbII, and DyII ions, YbII complexes are more easily obtainable, as reflected by their less negative reduction potentials (Morss, 1976). A crystal containing the oligomeric compound; [(THF)Cs(μ-η55-Cp′)3Yb]n, 1 (Cp′ = C5H4SiMe3) was isolated by reduction of the Cp′3YbIII complex (Fieser et al., 2015) in THF using Cs metal (Figs. 2 and 3).

Figure 2.

Figure 2

Synthesis of [(THF)Cs(μ-η55-Cp′)3YbII]n, 1, by caesium metal reduction of the Cp′3YbIII precursor.

Figure 3.

Figure 3

ORTEP representation of an asymmetric unit of [(THF)Cs(μ-η55-Cp′)3Yb]n, 1, with probability ellipsoids drawn at the 50% probability level. Hydrogen atoms were omitted for clarity.

Structural commentary  

All three Cp′ rings remain coordinated to the Yb metal center after reduction and are coordinated in a trigonal–planar fashion. The Yb atom is within 0.107 Å of the plane of the three ring centroids. Each ring bridges Yb to Cs, which also is surrounded by three cyclo­penta­dienyl ligands as well as a coordinated mol­ecule of THF. The three ring centroids and the oxygen of THF are arranged in a pseudo-tetra­hedral geometry around Cs with a calculated four-coordinate Cs τ′4 value of 0.76 (τ′4 = 1 for tetra­hedral; τ′4 = 0 for square planar; Rosiak et al., 2018). The Cs metal center has a pseudo-tetra­hedral geometry with Cp′(centroid)⋯Cs⋯Cp′(centroid) angles of 109.0, 114.3, and 121.4° and Cp′(centroid)⋯Cs⋯O(THF) angles of 88.8, 94.1, and 127.8°.

The bond distances and angles in 1 are summarized in Table 1. The range of 2.504 (1)–2.513 (2) Å Cp′(centroid)⋯Yb bond distances in 1 is the same as that in the complex [K(crypt)][Cp′3YbII] (crypt = 2.2.2-cryptand), which was fully characterized as a 4f 14 YbII complex, Table 2 and Fig. 4. In Cp3 Ln reduction chemistry, the difference in Ln⋯Cp(centroid) distances between the Ln III and Ln II complexes provides important information on the electronic configuration of the lanthanide ion (Evans, 2016). Differences in Ln⋯Cp(centroid) distances for reduction of 4f n Ln III ions to 4f n+1 Ln II ions range from 0.1 to 0.2 Å (Fieser et al., 2015). In this study, the difference of 0.14 Å in the Ln⋯Cp(centroid) distance is characteristic of a 4f 13 YbIII reduction to a 4f 14 YbII ion. In contrast, Ln II ions with 4fn5d 1 configurations where the additional electron populates a d-orbital instead of the an f-orbital have differences of only 0.02–0.05 Å (Evans, 2016).

Table 1. Selected bond distances and angles for [(THF)Cs(μ-η55-Cp′)3Yb]n, 1 .

Centroid1, centroid2, and centroid3 are the centroids of the Cp rings connected to Si1, Si2, and Si3, respectively.

Yb1⋯centroid1 2.510 (1)
Yb1⋯centroid2 2.513 (2)
Yb1⋯centroid3 2.504 (1)
Cs1⋯centroid1 3.197 (1)
Cs1⋯centroid2 3.268 (2)
Cs1⋯centroid3 3.159 (1)
Cs1—O1 3.095 (3)
   
centroid1—Yb1⋯centroid2 120.1
centroid1—Yb1⋯centroid3 116.6
centroid2—Yb1⋯centroid3 122.8
centroid1—Cs1⋯centroid2 121.4
centroid1—Cs1⋯centroid3 109.0
centroid2—Cs1⋯centroid3 114.3
Yb1⋯centroid1⋯Cs1 175.3
Yb1⋯centroid2⋯Cs1 172.3
Yb1⋯centroid3⋯Cs1 176.7
centroid1⋯Cs1⋯O1 88.8
centroid2⋯Cs1⋯O1 94.1
centroid3⋯Cs1⋯O1 127.8

Table 2. Bond distance (Å) ranges for Yb⋯Cp′(centroid) and bond angle (°) ranges for Cp′(centroid)⋯Yb⋯Cp′(centroid) in Cp′3Yb (Fieser et al., 2015), [K(crypt)][Cp′3Yb] (Fieser et al., 2015), and [(THF)Cs(μ-η55-Cp′)3Yb]n .

  Cp′3Yb [K(crypt)][Cp′3Yb] 1
Yb⋯Cp′(centroid) 2.363–2.368 2.503–2.513 2.504 (1)–2.513 (2)
Cs⋯Cp′(centroid)     3.159 (1)–3.268 (2)
Cp′⋯Yb⋯Cp′ 118.85–120.55 118.10–122.93 116.64–122.76
Cp′⋯Cs⋯Cp′     109.0–121.4

Figure 4.

Figure 4

CHEMDRAW (Mills, 2006) representation of [K(2.2.2-cryptand)][Cp′3YbII] (left) and [(THF)Cs(μ-η55-Cp′)3YbII]n, 1, (right).

Supra­molecular features  

In 1, all of the cyclo­penta­dienyl ligands are bridging. The threefold symmetry of three bridging Cp′ ligands on each metal generates a hexa­gonal pattern as shown in Fig. 5. The Yb⋯Cp′(centroid)⋯Cs angles are 172.5–176.7° such that each side of the hexa­gon is nearly linear. The 112.4–117.3° Yb⋯Cs⋯Yb angles are smaller than the 120.8–125.6° Cs⋯Yb⋯Cs angles, which makes the hexa­gon slightly irregular. This could be of inter­est to quantum scientists trying to make thin-film layers of magnetic materials since the hexa­gonal pattern could lead to spin frustration with a paramagnetic lanthanide.

Figure 5.

Figure 5

Top view of the extended structure of [(THF)Cs(μ-η55-Cp′)3Yb]n, 1, with the SiMe3 substituent of the C5H4SiMe3 group and the THF attached to Cs removed for clarity.

The side view of these layers in Fig. 6 shows how the space in between them is filled with THF and Me3Si substituent groups. The 116.6–122.8° Cp′(centroid)⋯Yb⋯Cp′(centroid) and 109.0–121.4° Cp′(centroid)⋯Cs⋯Cp′(centroid) angles generate the undulation of the hexa­gons shown in Fig. 6.

Figure 6.

Figure 6

Side view of the extended structure of [(THF)Cs(μ-η55-Cp′)3Yb]n, 1. Magenta, Yb; brown, Cs; green, Si; red, O.

Database survey  

The 3.159 (1), 3.197 (1), and 3.268 (2) Å Cs⋯Cp′(centroid) distances in 1 are shorter than the 3.278 and 3.435 Å Cs⋯Cp′′(centroid) distances in [(THF)2Cs][(μ-η55-Cp′′)2UII5-Cp′′)]n, (Huh et al., 2018), the 3.396 Å Cs⋯C5H5(centroid) distances in {[(Me3Si)2NCs]2·[(C5H5)2Fe)] 0.5·(C6H5Me)}n, (Morris et al., 2007) and the 3.337 Å Cs⋯C5Me5(centroid) distances in [(THF)2Cs(μ3-O)3{[Ti(C5Me5)]3-(μ3-CCH2)}] (González-del Moral et al., 2005). The 3.095 (3) Å Cs—O(THF) bond distance is consistent with the Cs—O(THF) distances of 3.081 (7) to 3.119 (8) Å in [(THF)2Cs][(μ-η55-Cp′′)2UII5-Cp′′)]n (Huh et al., 2018) and 3.034 (9)–3.06 (1) Å in [(THF)2Cs(μ3-O)3{[Ti(C5Me5)]33-CCH2)}] (González-del Moral et al., 2005).

The extended structure of 1 differs from that of the [(THF)2Cs][(μ-η55-Cp′′)2 M II5-Cp′′)]n, complexes (M = La, U), which comprise zigzag chains of –M–(μ-Cp′′)–Cs–(μ-Cp′′)– repeat units with a terminal Cp′′ attached to M and two terminal THF ligands attached to Cs (Huh et al., 2018). These were obtained by reduction of Cp′′3 M III compounds with Cs in THF. In those structures, La and U have a trigonal–planar tris­(cyclo­penta­dien­yl) coordination like Yb in 1, but the Cs is coordinated by only two cyclo­penta­dienyl ligands to give a bent metallocene Cp′′2Cs(THF)2 sub-structure with these larger rings.

A survey of the Cambridge Structural Database (CSD, version 5.41, March 2020; Groom et al., 2016) also revealed four oligomeric complexes containing Yb–Cpx moieties with various types of cyclo­penta­dienyl rings (Cpx): [Na(μ-η55-C5H5)3YbII]n (Apostolidis et al., 1997), [Na(μ-η55-Cp′′)2YbII 2(μ-η55-Cp′′)2]n (Voskoboynikov et al., 1997), [(C5Me5)Yb(μ-I)(μ-η55-C5Me5)Yb(C5Me5)]n (Evans et al., 2006) and [Yb(μ-η55-C5H5)(Ph2Pz)(THF)]n (Ph2Pz = 3,5–di­phenyl­pyrazolate) (Ali et al., 2018). The [Na(μ-η55-C5H5)3YbII]n (Apostolidis et al., 1997) complex adopts a hexa­gonal net extended structure similar to that in 1 except the alkali metal does not have a coordinated solvent. The structure of [Na(μ-η55-CptBu)3SmII] is similar (Bel’sky et al., 1990). Three oligomeric complexes containing Cs–cyclo­penta­dienyl moieties have previously been reported: [(THF)2Cs][(μ-η55-Cp′′)2UII5-Cp′′)]n (Huh et al., 2018), {[(Me3Si)2NCs]2[(C5H5)2Fe)]·0.5(C6H5Me)}n (Morris et al., 2007) and [(THF)2Cs(μ3-O)3{[Ti(C5Me5)]33-CCH2)}] (Gon­zález-del Moral et al., 2005). An oligomeric, base-free Li–Cp′ compound was also previously reported in the literature, [(μ-η55-Cp′)Li]n (Evans et al., 1992).

Synthesis and crystallization  

In an argon-filled glovebox, addition of a red solution of Cp′3Yb (50 mg, 0.085 mmol) in THF (2 mL) to excess Cs as a smear produced a green solution. This was stirred for 15 min at room temperature and then layered at the bottom of a vial below an Et2O (10 mL) layer for crystallization at −35°C. After 1 d, X-ray quality dark-green crystals of [(THF)Cs(μ-η55-Cp′)3YbII]n were isolated. A small number of crystals were obtained and used for crystallographic analysis. Too little sample was available for other characterization.

Refinement  

Crystal data and structure refinement for [(THF)Cs(μ-η55-Cp′)3YbII]n, 1 are summarized in Table 3. Hydrogen atoms were included using a riding model with U iso(H) values of 1.2U eq(C) for CH2 and aromatic hydrogens and 1.5U eq(C) for CH3 hydrogens with C—H distances of 0.99 (CH2), 0.95 (aromatic), and 0.98 Å (CH3).

Table 3. Experimental details.

Crystal data
Chemical formula [CsYb(C8H13Si)3(C4H8O)]
M r 789.87
Crystal system, space group Monoclinic, P21/n
Temperature (K) 88
a, b, c (Å) 9.4401 (4), 16.8718 (8), 21.0246 (10)
β (°) 92.0668 (6)
V3) 3346.4 (3)
Z 4
Radiation type Mo Kα
μ (mm−1) 3.99
Crystal size (mm) 0.15 × 0.09 × 0.08
 
Data collection
Diffractometer Bruker SMART APEXII CCD
Absorption correction Multi-scan (SADABS; Bruker, 2014)
T min, T max 0.374, 0.432
No. of measured, independent and observed [I > 2σ(I)] reflections 40586, 8223, 6580
R int 0.055
(sin θ/λ)max−1) 0.667
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.032, 0.056, 1.02
No. of reflections 8223
No. of parameters 316
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.14, −0.62

Computer programs: APEX2 (Bruker, 2014), SAINT (Bruker, 2013), SHELXT2014/4 (Sheldrick, 2015a ), SHELXL2014/7 (Sheldrick, 2015b ) and SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989020008051/zl2785sup1.cif

e-76-01131-sup1.cif (1.2MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989020008051/zl2785Isup2.hkl

e-76-01131-Isup2.hkl (653KB, hkl)

CCDC reference: 2010185

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

Acknowledgments

WJE would like to acknowledge the National Science Foundation for continued support.

supplementary crystallographic information

Crystal data

[CsYb(C8H13Si)3(C4H8O)] F(000) = 1560
Mr = 789.87 Dx = 1.568 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
a = 9.4401 (4) Å Cell parameters from 9869 reflections
b = 16.8718 (8) Å θ = 2.3–28.5°
c = 21.0246 (10) Å µ = 3.99 mm1
β = 92.0668 (6)° T = 88 K
V = 3346.4 (3) Å3 Prism, green
Z = 4 0.15 × 0.09 × 0.08 mm

Data collection

Bruker SMART APEXII CCD diffractometer 6580 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.055
φ and ω scans θmax = 28.3°, θmin = 1.6°
Absorption correction: multi-scan (SADABS; Bruker, 2014) h = −12→12
Tmin = 0.374, Tmax = 0.432 k = −22→22
40586 measured reflections l = −27→27
8223 independent reflections

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)] = 0.032 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.056 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0229P)2 + 0.1327P] where P = (Fo2 + 2Fc2)/3
8223 reflections (Δ/σ)max = 0.001
316 parameters Δρmax = 1.14 e Å3
0 restraints Δρmin = −0.62 e Å3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.
Refinement. A green crystal of approximate dimensions 0.079 x 0.086 x 0.148 mm was mounted in a cryoloop and transferred to a Bruker SMART APEX II diffractometer. The APEX2 program package was used to determine the unit-cell parameters and for data collection (90 sec/frame scan time for a sphere of diffraction data). The raw frame data was processed using SAINT and SADABS to yield the reflection data file. Subsequent calculations were carried out using the SHELXTL program. The diffraction symmetry was 2/m and the systematic absences were consistent with the monoclinic space group P21/n that was later determined to be correct. The structure was solved by dual space methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. The structure is polymeric. Least-squares analysis yielded wR2 = 0.0562 and Goof = 1.017 for 316 variables refined against 8223 data (0.75 Å), R1 = 0.0315 for those 6580 data with I > 2.0sigma(I).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
Yb1 0.48657 (2) 0.44122 (2) 0.25290 (2) 0.01341 (4)
Cs1 0.99437 (2) 0.27157 (2) 0.31696 (2) 0.01493 (5)
Si1 0.69834 (10) 0.29048 (6) 0.15029 (5) 0.0184 (2)
Si2 0.23952 (11) 0.57037 (6) 0.11663 (5) 0.0204 (2)
Si3 0.25791 (10) 0.45182 (6) 0.40988 (5) 0.0187 (2)
O1 0.8795 (3) 0.24593 (16) 0.45145 (12) 0.0285 (6)
C1 0.7108 (3) 0.33895 (19) 0.22942 (16) 0.0161 (7)
C2 0.6551 (3) 0.3115 (2) 0.28743 (17) 0.0174 (8)
H2A 0.6070 0.2626 0.2929 0.021*
C3 0.6826 (3) 0.3680 (2) 0.33517 (17) 0.0196 (8)
H3A 0.6554 0.3643 0.3781 0.024*
C4 0.7575 (4) 0.4310 (2) 0.30831 (17) 0.0194 (8)
H4A 0.7902 0.4774 0.3298 0.023*
C5 0.7751 (3) 0.4129 (2) 0.24430 (17) 0.0184 (8)
H5A 0.8231 0.4453 0.2150 0.022*
C6 0.6270 (4) 0.1878 (2) 0.15741 (18) 0.0257 (9)
H6A 0.6848 0.1582 0.1890 0.039*
H6B 0.6299 0.1611 0.1161 0.039*
H6C 0.5288 0.1902 0.1709 0.039*
C7 0.5764 (4) 0.3487 (2) 0.09635 (17) 0.0276 (9)
H7A 0.6159 0.4017 0.0900 0.041*
H7B 0.4836 0.3533 0.1155 0.041*
H7C 0.5656 0.3216 0.0552 0.041*
C8 0.8767 (4) 0.2878 (2) 0.11484 (18) 0.0263 (9)
H8A 0.9435 0.2601 0.1438 0.039*
H8B 0.9099 0.3421 0.1081 0.039*
H8C 0.8702 0.2599 0.0740 0.039*
C9 0.3846 (3) 0.57009 (19) 0.17806 (16) 0.0162 (7)
C10 0.5320 (4) 0.56244 (19) 0.16482 (17) 0.0173 (7)
H10A 0.5679 0.5462 0.1253 0.021*
C11 0.6148 (4) 0.58254 (19) 0.21886 (17) 0.0171 (8)
H11A 0.7154 0.5833 0.2220 0.021*
C12 0.5224 (4) 0.60152 (19) 0.26788 (17) 0.0190 (8)
H12A 0.5497 0.6163 0.3102 0.023*
C13 0.3823 (4) 0.59465 (19) 0.24280 (16) 0.0180 (8)
H13A 0.2992 0.6048 0.2656 0.022*
C14 0.2553 (5) 0.4858 (2) 0.0598 (2) 0.0380 (11)
H14A 0.2394 0.4358 0.0822 0.057*
H14B 0.3503 0.4856 0.0425 0.057*
H14C 0.1843 0.4916 0.0249 0.057*
C15 0.0612 (4) 0.5700 (3) 0.1518 (2) 0.0379 (11)
H15A 0.0433 0.5178 0.1705 0.057*
H15B −0.0113 0.5811 0.1185 0.057*
H15C 0.0577 0.6107 0.1849 0.057*
C16 0.2543 (4) 0.6620 (2) 0.06760 (17) 0.0230 (8)
H16A 0.3509 0.6665 0.0524 0.034*
H16B 0.2329 0.7085 0.0936 0.034*
H16C 0.1869 0.6593 0.0311 0.034*
C17 0.2651 (3) 0.4025 (2) 0.33118 (16) 0.0151 (7)
C18 0.1959 (3) 0.42821 (19) 0.27347 (17) 0.0169 (7)
H18A 0.1408 0.4751 0.2686 0.020*
C19 0.2216 (3) 0.3741 (2) 0.22535 (17) 0.0187 (8)
H19A 0.1879 0.3780 0.1823 0.022*
C20 0.3061 (4) 0.3127 (2) 0.25131 (17) 0.0206 (8)
H20A 0.3395 0.2678 0.2291 0.025*
C21 0.3320 (3) 0.3300 (2) 0.31617 (17) 0.0173 (8)
H21A 0.3858 0.2981 0.3453 0.021*
C22 0.2748 (5) 0.3775 (2) 0.47533 (18) 0.0346 (10)
H22A 0.1956 0.3400 0.4718 0.052*
H22B 0.2732 0.4047 0.5165 0.052*
H22C 0.3644 0.3487 0.4721 0.052*
C23 0.4026 (4) 0.5264 (2) 0.42253 (18) 0.0280 (9)
H23A 0.3884 0.5702 0.3923 0.042*
H23B 0.4944 0.5012 0.4158 0.042*
H23C 0.4008 0.5469 0.4661 0.042*
C24 0.0843 (4) 0.5039 (3) 0.4147 (2) 0.0399 (11)
H24A 0.0071 0.4652 0.4106 0.060*
H24B 0.0748 0.5429 0.3803 0.060*
H24C 0.0798 0.5309 0.4559 0.060*
C25 0.8427 (4) 0.3003 (2) 0.50059 (19) 0.0306 (9)
H25A 0.8093 0.3512 0.4820 0.037*
H25B 0.9255 0.3108 0.5296 0.037*
C26 0.7248 (4) 0.2603 (2) 0.53629 (19) 0.0338 (10)
H26A 0.7634 0.2246 0.5700 0.041*
H26B 0.6615 0.2998 0.5555 0.041*
C27 0.6489 (4) 0.2145 (2) 0.4835 (2) 0.0315 (10)
H27A 0.5959 0.1690 0.5005 0.038*
H27B 0.5827 0.2489 0.4585 0.038*
C28 0.7700 (4) 0.1873 (2) 0.44422 (18) 0.0278 (9)
H28A 0.8052 0.1351 0.4593 0.033*
H28B 0.7388 0.1823 0.3989 0.033*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Yb1 0.01020 (7) 0.01233 (7) 0.01766 (8) −0.00136 (6) −0.00014 (6) 0.00251 (6)
Cs1 0.01034 (10) 0.01249 (10) 0.02208 (12) −0.00018 (8) 0.00232 (8) 0.00028 (9)
Si1 0.0150 (5) 0.0213 (5) 0.0190 (5) 0.0031 (4) 0.0009 (4) −0.0011 (4)
Si2 0.0214 (5) 0.0157 (5) 0.0236 (6) −0.0009 (4) −0.0052 (4) 0.0028 (4)
Si3 0.0177 (5) 0.0192 (5) 0.0191 (5) −0.0009 (4) 0.0012 (4) −0.0017 (4)
O1 0.0207 (14) 0.0355 (16) 0.0295 (16) −0.0014 (12) 0.0062 (12) −0.0009 (13)
C1 0.0112 (16) 0.0161 (17) 0.0209 (19) 0.0018 (14) 0.0018 (14) 0.0027 (15)
C2 0.0130 (17) 0.0140 (17) 0.025 (2) 0.0030 (14) 0.0021 (15) 0.0029 (15)
C3 0.0184 (18) 0.024 (2) 0.0162 (19) 0.0082 (15) 0.0003 (15) 0.0016 (15)
C4 0.0151 (17) 0.0177 (19) 0.025 (2) 0.0022 (14) −0.0071 (15) −0.0016 (16)
C5 0.0083 (16) 0.0175 (18) 0.030 (2) −0.0002 (13) 0.0033 (15) 0.0049 (16)
C6 0.027 (2) 0.023 (2) 0.027 (2) 0.0011 (16) −0.0006 (17) −0.0044 (17)
C7 0.029 (2) 0.033 (2) 0.021 (2) 0.0055 (18) −0.0059 (17) 0.0013 (17)
C8 0.023 (2) 0.031 (2) 0.024 (2) 0.0038 (17) 0.0045 (17) −0.0018 (17)
C9 0.0162 (17) 0.0111 (17) 0.0212 (19) 0.0006 (13) 0.0003 (14) 0.0012 (14)
C10 0.0208 (18) 0.0103 (16) 0.0210 (19) 0.0006 (14) 0.0037 (15) 0.0040 (15)
C11 0.0133 (17) 0.0139 (17) 0.024 (2) −0.0047 (13) −0.0014 (15) 0.0047 (15)
C12 0.0241 (19) 0.0118 (17) 0.021 (2) −0.0067 (15) −0.0054 (15) 0.0020 (15)
C13 0.0208 (18) 0.0118 (17) 0.022 (2) −0.0011 (14) 0.0012 (15) 0.0009 (15)
C14 0.056 (3) 0.020 (2) 0.037 (3) 0.004 (2) −0.023 (2) −0.0014 (19)
C15 0.022 (2) 0.049 (3) 0.043 (3) 0.0003 (19) −0.0048 (19) 0.024 (2)
C16 0.028 (2) 0.0204 (19) 0.021 (2) 0.0025 (16) −0.0007 (16) 0.0022 (16)
C17 0.0097 (16) 0.0196 (18) 0.0162 (19) −0.0037 (14) 0.0024 (14) 0.0003 (15)
C18 0.0099 (16) 0.0156 (18) 0.025 (2) −0.0029 (13) 0.0026 (14) 0.0024 (15)
C19 0.0129 (17) 0.028 (2) 0.0149 (19) −0.0086 (15) −0.0025 (14) 0.0029 (15)
C20 0.0165 (18) 0.0192 (19) 0.027 (2) −0.0062 (15) 0.0096 (16) −0.0061 (16)
C21 0.0124 (17) 0.0176 (18) 0.022 (2) −0.0025 (14) 0.0044 (14) 0.0051 (15)
C22 0.056 (3) 0.026 (2) 0.023 (2) −0.009 (2) 0.006 (2) −0.0032 (18)
C23 0.031 (2) 0.029 (2) 0.024 (2) −0.0056 (18) 0.0015 (18) −0.0038 (17)
C24 0.028 (2) 0.044 (3) 0.048 (3) 0.008 (2) 0.002 (2) −0.020 (2)
C25 0.034 (2) 0.030 (2) 0.028 (2) −0.0032 (18) −0.0060 (19) 0.0018 (18)
C26 0.042 (3) 0.032 (2) 0.028 (2) 0.006 (2) 0.012 (2) −0.0031 (19)
C27 0.024 (2) 0.026 (2) 0.044 (3) 0.0008 (17) 0.0085 (19) 0.0089 (19)
C28 0.033 (2) 0.025 (2) 0.026 (2) −0.0010 (17) 0.0071 (18) 0.0006 (17)

Geometric parameters (Å, º)

Yb1—Cnt1 2.510 C7—H7B 0.9800
Yb1—Cnt2 2.513 C7—H7C 0.9800
Yb1—Cnt3 2.504 C8—H8A 0.9800
Cs1—Cnt1 3.197 C8—H8B 0.9800
Cs1—Cnt2 3.268 C8—H8C 0.9800
Cs1—Cnt3 3.159 C9—C13 1.424 (5)
Yb1—C12 2.742 (3) C9—C10 1.434 (5)
Yb1—C21 2.750 (3) C9—Cs1iii 3.587 (3)
Yb1—C20 2.757 (3) C10—C11 1.398 (5)
Yb1—C13 2.775 (3) C10—Cs1iii 3.559 (3)
Yb1—C3 2.777 (3) C10—H10A 0.9500
Yb1—C4 2.778 (3) C11—C12 1.410 (5)
Yb1—C5 2.778 (3) C11—Cs1iii 3.427 (3)
Yb1—C11 2.779 (3) C11—H11A 0.9500
Yb1—C17 2.785 (3) C12—C13 1.411 (5)
Yb1—C2 2.787 (3) C12—Cs1iii 3.379 (3)
Yb1—C19 2.787 (3) C12—H12A 0.9500
Yb1—C1 2.788 (3) C13—Cs1iii 3.457 (3)
Yb1—C18 2.802 (3) C13—H13A 0.9500
Yb1—C10 2.802 (3) C14—H14A 0.9800
Yb1—C9 2.832 (3) C14—H14B 0.9800
Cs1—O1 3.095 (3) C14—H14C 0.9800
Cs1—C2 3.309 (3) C15—H15A 0.9800
Cs1—C21i 3.337 (3) C15—H15B 0.9800
Cs1—C20i 3.367 (3) C15—H15C 0.9800
Cs1—C12ii 3.379 (3) C16—Cs1iii 3.810 (4)
Cs1—C17i 3.383 (3) C16—H16A 0.9800
Cs1—C1 3.390 (3) C16—H16B 0.9800
Cs1—C3 3.396 (3) C16—H16C 0.9800
Cs1—C18i 3.401 (3) C17—C21 1.417 (5)
Cs1—C19i 3.407 (3) C17—C18 1.425 (5)
Cs1—C11ii 3.427 (3) C17—Cs1iv 3.383 (3)
Cs1—C13ii 3.457 (3) C18—C19 1.390 (5)
Cs1—C5 3.475 (3) C18—Cs1iv 3.401 (3)
Cs1—C4 3.499 (3) C18—H18A 0.9500
Cs1—C10ii 3.559 (3) C19—C20 1.406 (5)
Cs1—C9ii 3.587 (3) C19—Cs1iv 3.407 (3)
Si1—C1 1.854 (4) C19—H19A 0.9500
Si1—C8 1.866 (4) C20—C21 1.407 (5)
Si1—C7 1.866 (4) C20—Cs1iv 3.367 (3)
Si1—C6 1.867 (4) C20—H20A 0.9500
Si2—C9 1.848 (4) C21—Cs1iv 3.337 (3)
Si2—C15 1.863 (4) C21—H21A 0.9500
Si2—C16 1.867 (3) C22—H22A 0.9800
Si2—C14 1.871 (4) C22—H22B 0.9800
Si3—C17 1.856 (3) C22—H22C 0.9800
Si3—C22 1.864 (4) C23—H23A 0.9800
Si3—C24 1.865 (4) C23—H23B 0.9800
Si3—C23 1.869 (4) C23—H23C 0.9800
O1—C25 1.434 (5) C24—H24A 0.9800
O1—C28 1.435 (4) C24—H24B 0.9800
C1—C5 1.418 (5) C24—H24C 0.9800
C1—C2 1.423 (5) C25—C26 1.522 (5)
C2—C3 1.402 (5) C25—H25A 0.9900
C2—H2A 0.9500 C25—H25B 0.9900
C3—C4 1.407 (5) C26—C27 1.511 (6)
C3—H3A 0.9500 C26—H26A 0.9900
C4—C5 1.396 (5) C26—H26B 0.9900
C4—H4A 0.9500 C27—C28 1.507 (5)
C5—H5A 0.9500 C27—H27A 0.9900
C6—H6A 0.9800 C27—H27B 0.9900
C6—H6B 0.9800 C28—H28A 0.9900
C6—H6C 0.9800 C28—H28B 0.9900
C7—H7A 0.9800
Cnt1—Yb1—Cnt2 120.1 C15—Si2—C14 110.1 (2)
Cnt1—Yb1—Cnt3 116.6 C16—Si2—C14 105.67 (18)
Cnt2—Yb1—Cnt3 122.8 C17—Si3—C22 110.60 (16)
Cnt1—Cs1—O1 88.8 C17—Si3—C24 108.68 (17)
Cnt2—Cs1—O1 94.1 C22—Si3—C24 109.2 (2)
Cnt3—Cs1—O1 127.8 C17—Si3—C23 112.26 (16)
Cnt1—Cs1—Cnt3 109.0 C22—Si3—C23 107.77 (19)
Cnt1—Cs1—Cnt2 121.4 C24—Si3—C23 108.32 (19)
Cnt2—Cs1—Cnt3 114.3 C25—O1—C28 109.0 (3)
Yb1—Cnt1—Cs1 175.3 C25—O1—Cs1 132.2 (2)
Yb1—Cnt2—Cs1 172.5 C28—O1—Cs1 105.9 (2)
Yb1—Cnt3—Cs1 176.7 C5—C1—C2 105.4 (3)
C12—Yb1—C21 133.07 (10) C5—C1—Si1 126.8 (3)
C12—Yb1—C20 148.28 (10) C2—C1—Si1 127.7 (3)
C21—Yb1—C20 29.62 (10) C5—C1—Yb1 74.82 (18)
C12—Yb1—C13 29.63 (10) C2—C1—Yb1 75.16 (18)
C21—Yb1—C13 118.73 (10) Si1—C1—Yb1 114.08 (15)
C20—Yb1—C13 121.02 (10) C5—C1—Cs1 81.47 (19)
C12—Yb1—C3 106.89 (10) C2—C1—Cs1 74.58 (18)
C21—Yb1—C3 75.43 (10) Si1—C1—Cs1 111.25 (13)
C20—Yb1—C3 93.17 (11) Yb1—C1—Cs1 134.51 (12)
C13—Yb1—C3 133.57 (10) C3—C2—C1 109.1 (3)
C12—Yb1—C4 84.54 (10) C3—C2—Yb1 75.02 (19)
C21—Yb1—C4 104.58 (10) C1—C2—Yb1 75.27 (19)
C20—Yb1—C4 121.05 (10) C3—C2—Cs1 81.44 (19)
C13—Yb1—C4 114.11 (10) C1—C2—Cs1 80.94 (19)
C3—Yb1—C4 29.34 (10) Yb1—C2—Cs1 138.44 (12)
C12—Yb1—C5 93.42 (10) C3—C2—H2A 125.4
C21—Yb1—C5 116.94 (10) C1—C2—H2A 125.4
C20—Yb1—C5 118.11 (10) Yb1—C2—H2A 116.2
C13—Yb1—C5 120.08 (10) Cs1—C2—H2A 105.3
C3—Yb1—C5 48.02 (10) C2—C3—C4 108.0 (3)
C4—Yb1—C5 29.10 (10) C2—C3—Yb1 75.79 (19)
C12—Yb1—C11 29.58 (10) C4—C3—Yb1 75.34 (19)
C21—Yb1—C11 162.49 (10) C2—C3—Cs1 74.48 (18)
C20—Yb1—C11 161.12 (11) C4—C3—Cs1 82.34 (19)
C13—Yb1—C11 48.43 (10) Yb1—C3—Cs1 134.71 (12)
C3—Yb1—C11 104.80 (10) C2—C3—H3A 126.0
C4—Yb1—C11 76.00 (10) C4—C3—H3A 126.0
C5—Yb1—C11 72.15 (10) Yb1—C3—H3A 115.1
C12—Yb1—C17 104.81 (10) Cs1—C3—H3A 110.0
C21—Yb1—C17 29.67 (9) C5—C4—C3 107.5 (3)
C20—Yb1—C17 49.15 (10) C5—C4—Yb1 75.45 (19)
C13—Yb1—C17 89.55 (10) C3—C4—Yb1 75.31 (19)
C3—Yb1—C17 91.45 (10) C5—C4—Cs1 77.52 (19)
C4—Yb1—C17 115.93 (10) C3—C4—Cs1 74.17 (18)
C5—Yb1—C17 139.21 (10) Yb1—C4—Cs1 130.28 (12)
C11—Yb1—C17 134.15 (10) C5—C4—H4A 126.3
C12—Yb1—C2 132.66 (10) C3—C4—H4A 126.3
C21—Yb1—C2 69.27 (10) Yb1—C4—H4A 115.3
C20—Yb1—C2 74.47 (10) Cs1—C4—H4A 114.4
C13—Yb1—C2 161.85 (10) C4—C5—C1 109.9 (3)
C3—Yb1—C2 29.18 (10) C4—C5—Yb1 75.44 (19)
C4—Yb1—C2 48.21 (10) C1—C5—Yb1 75.66 (18)
C5—Yb1—C2 47.93 (10) C4—C5—Cs1 79.4 (2)
C11—Yb1—C2 119.41 (10) C1—C5—Cs1 74.73 (19)
C17—Yb1—C2 95.49 (10) Yb1—C5—Cs1 131.24 (12)
C12—Yb1—C19 122.04 (10) C4—C5—H5A 125.0
C21—Yb1—C19 48.35 (10) C1—C5—H5A 125.0
C20—Yb1—C19 29.37 (10) Yb1—C5—H5A 115.8
C13—Yb1—C19 92.85 (10) Cs1—C5—H5A 112.9
C3—Yb1—C19 121.44 (10) Si1—C6—H6A 109.5
C4—Yb1—C19 150.23 (10) Si1—C6—H6B 109.5
C5—Yb1—C19 142.33 (10) H6A—C6—H6B 109.5
C11—Yb1—C19 133.69 (10) Si1—C6—H6C 109.5
C17—Yb1—C19 48.72 (10) H6A—C6—H6C 109.5
C2—Yb1—C19 103.58 (10) H6B—C6—H6C 109.5
C12—Yb1—C1 122.63 (10) Si1—C7—H7A 109.5
C21—Yb1—C1 94.75 (10) Si1—C7—H7B 109.5
C20—Yb1—C1 89.08 (10) H7A—C7—H7B 109.5
C13—Yb1—C1 146.41 (10) Si1—C7—H7C 109.5
C3—Yb1—C1 48.85 (10) H7A—C7—H7C 109.5
C4—Yb1—C1 48.90 (10) H7B—C7—H7C 109.5
C5—Yb1—C1 29.52 (9) Si1—C8—H8A 109.5
C11—Yb1—C1 98.33 (10) Si1—C8—H8B 109.5
C17—Yb1—C1 123.39 (10) H8A—C8—H8B 109.5
C2—Yb1—C1 29.57 (9) Si1—C8—H8C 109.5
C19—Yb1—C1 113.15 (10) H8A—C8—H8C 109.5
C12—Yb1—C18 100.20 (10) H8B—C8—H8C 109.5
C21—Yb1—C18 48.09 (10) C13—C9—C10 105.1 (3)
C20—Yb1—C18 48.09 (10) C13—C9—Si2 129.1 (3)
C13—Yb1—C18 74.83 (10) C10—C9—Si2 124.3 (3)
C3—Yb1—C18 120.22 (10) C13—C9—Yb1 73.08 (19)
C4—Yb1—C18 145.35 (10) C10—C9—Yb1 74.11 (18)
C5—Yb1—C18 164.74 (10) Si2—C9—Yb1 128.22 (15)
C11—Yb1—C18 123.02 (10) C13—C9—Cs1iii 73.26 (18)
C17—Yb1—C18 29.55 (9) C10—C9—Cs1iii 77.33 (18)
C2—Yb1—C18 116.83 (10) Si2—C9—Cs1iii 104.19 (12)
C19—Yb1—C18 28.80 (10) Yb1—C9—Cs1iii 127.59 (11)
C1—Yb1—C18 137.11 (10) C11—C10—C9 109.8 (3)
C12—Yb1—C10 48.31 (10) C11—C10—Yb1 74.58 (19)
C21—Yb1—C10 156.10 (10) C9—C10—Yb1 76.40 (19)
C20—Yb1—C10 132.46 (11) C11—C10—Cs1iii 73.21 (18)
C13—Yb1—C10 48.00 (10) C9—C10—Cs1iii 79.51 (18)
C3—Yb1—C10 128.46 (10) Yb1—C10—Cs1iii 129.76 (12)
C4—Yb1—C10 99.32 (10) C11—C10—H10A 125.1
C5—Yb1—C10 84.76 (10) C9—C10—H10A 125.1
C11—Yb1—C10 29.00 (10) Yb1—C10—H10A 115.8
C17—Yb1—C10 134.24 (10) Cs1iii—C10—H10A 114.2
C2—Yb1—C10 130.23 (10) C10—C11—C12 107.9 (3)
C19—Yb1—C10 108.45 (10) C10—C11—Yb1 76.42 (18)
C1—Yb1—C10 101.51 (10) C12—C11—Yb1 73.76 (18)
C18—Yb1—C10 109.46 (10) C10—C11—Cs1iii 83.81 (19)
C12—Yb1—C9 49.06 (10) C12—C11—Cs1iii 76.14 (19)
C21—Yb1—C9 128.10 (10) Yb1—C11—Cs1iii 136.45 (12)
C20—Yb1—C9 113.55 (10) C10—C11—H11A 126.1
C13—Yb1—C9 29.39 (9) C12—C11—H11A 126.1
C3—Yb1—C9 153.27 (10) Yb1—C11—H11A 115.9
C4—Yb1—C9 124.75 (10) Cs1iii—C11—H11A 107.2
C5—Yb1—C9 114.22 (10) C11—C12—C13 107.7 (3)
C11—Yb1—C9 48.76 (10) C11—C12—Yb1 76.66 (19)
C17—Yb1—C9 105.13 (10) C13—C12—Yb1 76.46 (19)
C2—Yb1—C9 158.00 (10) C11—C12—Cs1iii 79.95 (19)
C19—Yb1—C9 84.94 (10) C13—C12—Cs1iii 81.20 (19)
C1—Yb1—C9 128.44 (10) Yb1—C12—Cs1iii 140.67 (13)
C18—Yb1—C9 80.25 (10) C11—C12—H12A 126.1
C10—Yb1—C9 29.49 (9) C13—C12—H12A 126.1
O1—Cs1—C2 80.28 (8) Yb1—C12—H12A 113.2
O1—Cs1—C21i 114.33 (8) Cs1iii—C12—H12A 106.1
C2—Cs1—C21i 148.98 (8) C12—C13—C9 109.6 (3)
O1—Cs1—C20i 138.03 (8) C12—C13—Yb1 73.92 (19)
C2—Cs1—C20i 137.32 (9) C9—C13—Yb1 77.53 (19)
C21i—Cs1—C20i 24.23 (8) C12—C13—Cs1iii 75.02 (18)
O1—Cs1—C12ii 110.63 (8) C9—C13—Cs1iii 83.51 (19)
C2—Cs1—C12ii 92.69 (8) Yb1—C13—Cs1iii 135.26 (12)
C21i—Cs1—C12ii 105.96 (8) C12—C13—H13A 125.2
C20i—Cs1—C12ii 89.07 (8) C9—C13—H13A 125.2
O1—Cs1—C17i 107.40 (7) Yb1—C13—H13A 115.3
C2—Cs1—C17i 127.34 (8) Cs1iii—C13—H13A 108.8
C21i—Cs1—C17i 24.34 (8) Si2—C14—H14A 109.5
C20i—Cs1—C17i 39.93 (8) Si2—C14—H14B 109.5
C12ii—Cs1—C17i 128.47 (8) H14A—C14—H14B 109.5
O1—Cs1—C1 104.30 (7) Si2—C14—H14C 109.5
C2—Cs1—C1 24.49 (8) H14A—C14—H14C 109.5
C21i—Cs1—C1 129.35 (8) H14B—C14—H14C 109.5
C20i—Cs1—C1 113.14 (8) Si2—C15—H15A 109.5
C12ii—Cs1—C1 88.68 (8) Si2—C15—H15B 109.5
C17i—Cs1—C1 114.09 (8) H15A—C15—H15B 109.5
O1—Cs1—C3 68.30 (8) Si2—C15—H15C 109.5
C2—Cs1—C3 24.09 (8) H15A—C15—H15C 109.5
C21i—Cs1—C3 133.69 (8) H15B—C15—H15C 109.5
C20i—Cs1—C3 136.14 (9) Si2—C16—Cs1iii 96.16 (13)
C12ii—Cs1—C3 116.22 (8) Si2—C16—H16A 109.5
C17i—Cs1—C3 109.40 (8) Cs1iii—C16—H16A 66.8
C1—Cs1—C3 39.65 (8) Si2—C16—H16B 109.5
O1—Cs1—C18i 124.90 (8) Cs1iii—C16—H16B 52.7
C2—Cs1—C18i 109.78 (8) H16A—C16—H16B 109.5
C21i—Cs1—C18i 39.23 (8) Si2—C16—H16C 109.5
C20i—Cs1—C18i 39.10 (8) Cs1iii—C16—H16C 153.3
C12ii—Cs1—C18i 122.27 (8) H16A—C16—H16C 109.5
C17i—Cs1—C18i 24.24 (8) H16B—C16—H16C 109.5
C1—Cs1—C18i 91.83 (8) C21—C17—C18 105.5 (3)
C3—Cs1—C18i 98.84 (8) C21—C17—Si3 128.0 (3)
O1—Cs1—C19i 146.73 (8) C18—C17—Si3 126.4 (3)
C2—Cs1—C19i 114.55 (8) C21—C17—Yb1 73.79 (18)
C21i—Cs1—C19i 39.29 (8) C18—C17—Yb1 75.89 (18)
C20i—Cs1—C19i 23.95 (8) Si3—C17—Yb1 118.31 (14)
C12ii—Cs1—C19i 98.71 (9) C21—C17—Cs1iv 75.99 (18)
C17i—Cs1—C19i 39.57 (8) C18—C17—Cs1iv 78.58 (18)
C1—Cs1—C19i 91.36 (8) Si3—C17—Cs1iv 108.65 (13)
C3—Cs1—C19i 112.73 (8) Yb1—C17—Cs1iv 132.98 (11)
C18i—Cs1—C19i 23.56 (8) C19—C18—C17 109.5 (3)
O1—Cs1—C11ii 87.61 (8) C19—C18—Yb1 75.02 (19)
C2—Cs1—C11ii 82.35 (8) C17—C18—Yb1 74.57 (18)
C21i—Cs1—C11ii 123.61 (8) C19—C18—Cs1iv 78.45 (19)
C20i—Cs1—C11ii 111.22 (8) C17—C18—Cs1iv 77.18 (18)
C12ii—Cs1—C11ii 23.90 (8) Yb1—C18—Cs1iv 131.52 (11)
C17i—Cs1—C11ii 147.92 (8) C19—C18—H18A 125.3
C1—Cs1—C11ii 88.14 (8) C17—C18—H18A 125.3
C3—Cs1—C11ii 102.45 (8) Yb1—C18—H18A 117.0
C18i—Cs1—C11ii 146.18 (8) Cs1iv—C18—H18A 111.4
C19i—Cs1—C11ii 122.61 (8) C18—C19—C20 108.2 (3)
O1—Cs1—C13ii 110.19 (8) C18—C19—Yb1 76.18 (19)
C2—Cs1—C13ii 116.34 (8) C20—C19—Yb1 74.12 (19)
C21i—Cs1—C13ii 85.36 (8) C18—C19—Cs1iv 77.99 (19)
C20i—Cs1—C13ii 73.64 (8) C20—C19—Cs1iv 76.46 (19)
C12ii—Cs1—C13ii 23.79 (8) Yb1—C19—Cs1iv 131.87 (12)
C17i—Cs1—C13ii 109.44 (8) C18—C19—H19A 125.9
C1—Cs1—C13ii 111.22 (8) C20—C19—H19A 125.9
C3—Cs1—C13ii 139.38 (8) Yb1—C19—H19A 115.9
C18i—Cs1—C13ii 111.98 (8) Cs1iv—C19—H19A 112.2
C19i—Cs1—C13ii 90.34 (8) C19—C20—C21 107.4 (3)
C11ii—Cs1—C13ii 38.65 (8) C19—C20—Yb1 76.50 (19)
O1—Cs1—C5 105.94 (7) C21—C20—Yb1 74.91 (19)
C2—Cs1—C5 38.83 (8) C19—C20—Cs1iv 79.59 (19)
C21i—Cs1—C5 110.42 (8) C21—C20—Cs1iv 76.66 (18)
C20i—Cs1—C5 101.17 (8) Yb1—C20—Cs1iv 134.91 (12)
C12ii—Cs1—C5 109.56 (8) C19—C20—H20A 126.3
C17i—Cs1—C5 91.53 (8) C21—C20—H20A 126.3
C1—Cs1—C5 23.80 (8) Yb1—C20—H20A 114.7
C3—Cs1—C5 38.38 (8) Cs1iv—C20—H20A 110.3
C18i—Cs1—C5 71.25 (8) C20—C21—C17 109.3 (3)
C19i—Cs1—C5 77.29 (8) C20—C21—Yb1 75.48 (19)
C11ii—Cs1—C5 111.87 (8) C17—C21—Yb1 76.54 (18)
C13ii—Cs1—C5 129.48 (8) C20—C21—Cs1iv 79.11 (19)
O1—Cs1—C4 84.87 (8) C17—C21—Cs1iv 79.67 (18)
C2—Cs1—C4 38.88 (8) Yb1—C21—Cs1iv 136.70 (12)
C21i—Cs1—C4 112.41 (8) C20—C21—H21A 125.3
C20i—Cs1—C4 112.73 (8) C17—C21—H21A 125.3
C12ii—Cs1—C4 127.43 (8) Yb1—C21—H21A 114.7
C17i—Cs1—C4 88.95 (8) Cs1iv—C21—H21A 108.6
C1—Cs1—C4 39.03 (8) Si3—C22—H22A 109.5
C3—Cs1—C4 23.49 (8) Si3—C22—H22B 109.5
C18i—Cs1—C4 75.59 (8) H22A—C22—H22B 109.5
C19i—Cs1—C4 89.67 (8) Si3—C22—H22C 109.5
C11ii—Cs1—C4 121.18 (8) H22A—C22—H22C 109.5
C13ii—Cs1—C4 150.24 (8) H22B—C22—H22C 109.5
C5—Cs1—C4 23.09 (8) Si3—C23—H23A 109.5
O1—Cs1—C10ii 74.63 (7) Si3—C23—H23B 109.5
C2—Cs1—C10ii 98.69 (8) H23A—C23—H23B 109.5
C21i—Cs1—C10ii 111.34 (8) Si3—C23—H23C 109.5
C20i—Cs1—C10ii 108.30 (8) H23A—C23—H23C 109.5
C12ii—Cs1—C10ii 38.08 (8) H23B—C23—H23C 109.5
C17i—Cs1—C10ii 133.90 (8) Si3—C24—H24A 109.5
C1—Cs1—C10ii 109.52 (8) Si3—C24—H24B 109.5
C3—Cs1—C10ii 113.49 (8) H24A—C24—H24B 109.5
C18i—Cs1—C10ii 147.28 (8) Si3—C24—H24C 109.5
C19i—Cs1—C10ii 127.76 (8) H24A—C24—H24C 109.5
C11ii—Cs1—C10ii 22.98 (8) H24B—C24—H24C 109.5
C13ii—Cs1—C10ii 37.70 (8) O1—C25—C26 105.8 (3)
C5—Cs1—C10ii 133.23 (8) O1—C25—H25A 110.6
C4—Cs1—C10ii 136.14 (8) C26—C25—H25A 110.6
O1—Cs1—C9ii 87.86 (7) O1—C25—H25B 110.6
C2—Cs1—C9ii 120.23 (8) C26—C25—H25B 110.6
C21i—Cs1—C9ii 88.67 (8) H25A—C25—H25B 108.7
C20i—Cs1—C9ii 85.71 (8) C27—C26—C25 101.6 (3)
C12ii—Cs1—C9ii 38.69 (8) C27—C26—H26A 111.5
C17i—Cs1—C9ii 112.18 (8) C25—C26—H26A 111.5
C1—Cs1—C9ii 125.32 (8) C27—C26—H26B 111.5
C3—Cs1—C9ii 136.64 (8) C25—C26—H26B 111.5
C18i—Cs1—C9ii 124.31 (8) H26A—C26—H26B 109.3
C19i—Cs1—C9ii 106.95 (8) C28—C27—C26 102.1 (3)
C11ii—Cs1—C9ii 38.49 (8) C28—C27—H27A 111.3
C13ii—Cs1—C9ii 23.23 (8) C26—C27—H27A 111.3
C5—Cs1—C9ii 147.92 (8) C28—C27—H27B 111.3
C4—Cs1—C9ii 158.85 (8) C26—C27—H27B 111.3
C10ii—Cs1—C9ii 23.16 (7) H27A—C27—H27B 109.2
C1—Si1—C8 109.90 (16) O1—C28—C27 106.8 (3)
C1—Si1—C7 109.33 (16) O1—C28—Cs1 52.50 (16)
C8—Si1—C7 108.40 (17) C27—C28—Cs1 137.3 (2)
C1—Si1—C6 110.42 (16) O1—C28—H28A 110.4
C8—Si1—C6 110.06 (17) C27—C28—H28A 110.4
C7—Si1—C6 108.70 (18) Cs1—C28—H28A 112.0
C9—Si2—C15 112.34 (18) O1—C28—H28B 110.4
C9—Si2—C16 108.64 (16) C27—C28—H28B 110.4
C15—Si2—C16 107.99 (17) Cs1—C28—H28B 60.1
C9—Si2—C14 111.75 (17) H28A—C28—H28B 108.6

Symmetry codes: (i) x+1, y, z; (ii) −x+3/2, y−1/2, −z+1/2; (iii) −x+3/2, y+1/2, −z+1/2; (iv) x−1, y, z.

Funding Statement

This work was funded by National Science Foundation, Directorate for Mathematical and Physical Sciences grant CHE-1855328 to William J. Evans.

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. DOI: 10.1107/S2056989020008051/zl2785sup1.cif

e-76-01131-sup1.cif (1.2MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989020008051/zl2785Isup2.hkl

e-76-01131-Isup2.hkl (653KB, hkl)

CCDC reference: 2010185

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


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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