Literature DB >> 25484731

Crystal structure of [(1,2,3,4,11,12-η)-anthracene]tris-(tri-methyl-stann-yl)cobalt(III).

William W Brennessel1, John E Ellis2.   

Abstract

The asymmetric unit of the title structure, [Co(η(6)-C14H10){Sn(CH3)3}3], contains two independent mol-ecules. Each anthracene ligand is η(6)-coordinating to a Co(III) cation and is nearly planar [fold angles of 5.4 (3) and 9.7 (3)°], as would be expected for its behaving almost entirely as a donor to a high-oxidation-state metal center. The slight fold in each anthracene ligand gives rise to slightly longer Co-C bond lengths to the ring junction carbon atoms than to the other four. Each Co(III) cation is further coordinated by three Sn(CH3)3 ligands, giving each mol-ecule a three-legged piano-stool geometry. In each of the two independent mol-ecules, the trio of SnMe3 ligands are modeled as disordered over two positions, rotated by approximately 30%, such that the C atoms nearly overlap. In one mol-ecule, the disorder ratio refined to 0.9365 (8):0.0635 (8), while that for the other refined to 0.9686 (8):0.0314 (8). The mol-ecules are well separated, and thus no significant inter-molecular inter-actions are observed. The compound is of inter-est as the first structure report of an η(6)-anthracene cobalt(III) complex.

Entities:  

Keywords:  NMR data; anthracene; cobalt; crystal structure; flat-slipped coordination mode; tri­methyl­stannyl ligands

Year:  2014        PMID: 25484731      PMCID: PMC4257331          DOI: 10.1107/S1600536814021709

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


Chemical context

Oxidation derivatives of unstable low-valent species often provide indirect support for their formulations. For example, thermally unstable alkyl isocyanide complexes of formally M(−II) that were proposed to be ‘K2[M(CNtBu)4],’ M = Fe (Brennessel et al., 2007 ▶), Ru (Corella et al., 1992 ▶), were reacted at low temperature in situ with SnPh3Cl to afford isolable and readily characterizable derivatives, trans-M(SnPh3)2(CNtBu)4. Similarly, it was planned to derivatize the formally Co(−I) anion [Co(C10H8)2]−, C10H8 = naphthalene, which is the analog of the well-characterized and isolable anthracene cobaltate [Co(C14H10)2]− (C14H10 = anthracene; Brennessel et al., 2002 ▶). To date, the only established instance of [Co(C10H8)2]− is as part of the highly specific triple salt [K(18-crown-6)]3[Co(C10H8)(C2H4)2]2[Co(C10H8)2] (Brennes­sel et al., 2006 ▶). But before applying this procedure to the naphthalene system, we chose to first apply it to the well-behaved anthracene system to test the feasibility of the deriv­atization. Thus, one equivalent of SnMe3Cl was added in situ to a THF solution of [K(THF)][Co(C14H10)2] (Brennessel et al., 2002 ▶), which produced an intense violet, pentane-soluble species. Rather than being the expected ‘[Co(C14H10)2(SnMe3)]’ formally Co(I) species, however, after further investigation it was determined to be the title compound, [Co(η6-C14H10)(SnMe3)3] (I), based on single-crystal X-ray diffraction. Similar reactions using SnPh3 and Sn(cyclo­hex­yl)3 produced only intra­ctable mixtures. Filtration of the reaction mixture left a very reactive dark-gray filter cake, which appeared to be from the deposition of Co metal. A tentative balanced equation has been proposed based on the initial evidence (see equation below). No yield was obtained, but if the equation holds, a qu­anti­tative yield would only be 33.3% based on cobalt. Single crystals were grown from a saturated pentane solution in a 243 K freezer and NMR experiments (see Synthesis and crystallization) were performed on the single crystals, which corroborated the structure analysis from diffraction data.

Structural Commentary

The structure contains two independent mol­ecules of (I) (Fig. 1 ▶) that are metrically very similar. Each mol­ecule contains one anthracene and three SnMe3 ligands in a three-legged-piano-stool geometry. In each of the two independent mol­ecules, the trio of tin ligands are disordered with a 30° rotation of the set, although the minor component of the disorder is very small (<10% by mass in both cases). The anthracene ligands in both mol­ecules are coordinated in an η6 mode and are nearly planar, with only the slightest bends at the imaginary lines joining atoms C1 and C4 [5.4 (3)°] and C24 and C27 [9.7 (3)°]. The CoC distances to the ring junction carbon atoms are slightly longer by 0.17 Å than those to the metal-coordinating non-ring junction atoms (Table 1 ▶). This has been referred to as a ‘flat-slipped’ coordination mode, and is likely due to an anti­bonding component of the anthracene HOMO at the ring-junction carbon atoms (Zhu et al., 2006 ▶). Thus the anthracene ligand is displaced slightly from the symmetric coordination mode found in η6-benzene metal complexes, in order to maximize the bonding overlaps with the four non-ring-junction carbon atoms. Because the metal is formally d 6 CoIII, the π-donation from the anthracene ligand is likely the most important contribution to its bonding.
Figure 1

The two independent mol­ecules of (I), showing the atom numbering. The minor components of the disorder are shown with dashed lines and boundary ellipsoids. The two orientations of the SnMe3 ligand set fit in essentially the same volume because the methyl groups are overlapped. Displacement ellipsoids are drawn at the 50% probability level and hydrogen atoms have been omitted.

Table 1

Comparison of (I) with free anthracene and selected ‘flat-slipped’ structures (, )

The numbering is according to Fig.2 ▶. For (I) and the molybdenum complex, only one of the two independent molecules for each is listed because they are metrically similar.

Feature(I)Anthracenea [(Cp")Ru(An)][PF6]b MoAn(PMe3)3 c
MC12.101(5) 2.207(4)2.297(3)
MC22.102(5) 2.217(4)2.261(3)
MC32.098(5) 2.223(4)2.285(3)
MC42.132(5) 2.210(4)2.268(3)
MC112.273(5) 2.289(4)2.405(3)
MC212.274(5) 2.283(4)2.424(3)
     
Increase (avg.)0.165 0.0720.137
     
C1C21.387(7)1.3675(9)1.399(6)1.407(6)
C2C31.423(8)1.4264(10)1.415(7)1.419(7)
C3C41.393(9)1.3674(9)1.398(7)1.408(7)
C1C111.438(7)1.4297(8)1.431(6)1.434(6)
C4C121.436(7)1.4295(8)1.441(6)1.452(6)
C11C121.449(7)1.4384(8)1.449(5)1.455(6)
     
Fold angle5.4(3) 4.45.4

Notes: (a) unpublished structure determined locally; (b) Konovalov et al. (2011 ▶), Cp = C5Me4(CH2OMe), An = anthracene; (c) Zhu et al. (2006 ▶).

Database Survey

Structures of η6-coordinated anthracene transition metal complexes are few [Cambridge Structural Database, Version 5.35, update No. 3, May 2014; Groom & Allen, 2014 ▶], but range from Ti (Seaburg et al., 1998 ▶) to Co (this work). Although one ligand in the titanium complex, [Ti(dmpe)(η4-C14H10)(η6-C14H10)] [dmpe = 1,2-bis(dimethylphosphino), is considered η6-coordinating based on TiC bond lengths, the fold angle between the plane consisting of non-ring-junction metal-coordinating carbon atoms and the rest of the ligand is nearly 20°, very likely placing it on the cusp of an η4 coordination mode. However, both [Cr(C14H10)(CO)3] (Hanic & Mills, 1968 ▶) and [Mo(C14H10)(PMe3)3] (Zhu et al., 2006 ▶) have nearly planar anthracene ligands (6.6 and 5.5–5.8°, respectively). The small fold angles and the M—C(ring junction) bond lengths that are slightly longer than the M—C(non-ring junction) ones exemplify the ‘flat-slipped’ coordination mode (Table 1 ▶). For these cases of early transition metals, the π-donation of anthracene is supplemented by δ-backbonding to the anthracene LUMO; however, the CC bond lengths are not all that different from those seen in normal-valent late transition metal complexes, and all are elongated relative to those in free anthracene (Table 1 ▶). In the structures of later transition metal compounds, the η6 ‘flat-slipped’ coordination mode is found in normal- or slightly sub-valent metal complexes, and the fold angle appears to be sensitive to oxidation state. In structures with RuII coordination centers (Garcia et al., 2010 ▶; Konovalov et al., 2011 ▶) the fold angles are 3.1 and 4.4°, respectively. As the oxidation state decreases, as in the cases of FeI (Schnöckelborg et al., 2012 ▶; Hatanaka et al., 2012 ▶) and RhI (Woolf et al., 2011 ▶), the fold angles increase slightly to 15.8, 9.1, 9.2, and 13.8°, respectively. Although fold angles may be subject to a variety of additional effects, including packing and sterics, in general the trend is that these angles increase with greater electron-acceptor behavior. This has been examined for the series Cp*Fe(C14H10)(−/0/+) and Cp*Fe(C10H8)(−/0/+), Cp* = C5Me5, by a combination of X-ray crystallography and DFT methods (Schnöckelborg et al., 2012 ▶). In low oxidation states, the fold angles are significant and the ring-junction carbon atoms are bent away from the metal, thus making the coordination η4. Whereas the folds become almost non-existent (<10°) for normal valent oxidation states and the coordination is η6, consistent with what is observed in (I), a formally CoIII, d 6 metal atom. The 1H NMR data trends are in agreement with those reported for the isoelectronic species, [RuCp(η6-C14H10)](PF6) (McNair & Mann, 1986 ▶) and [OsCp(η6-C14H10)](PF6) (Freedman et al., 1997 ▶), and for the cationic cobalt complex [(η4-C4Me4)Co(η6-C14H10)](PF6) (Mutseneck et al., 2007 ▶). The most upfield anthracene 1H NMR resonances of δ = 5.98 (I), 6.33 (Ru), 6.62 (Os), and 6.65 (Co cation) p.p.m. demonstrate that the ligand is behaving almost entirely as a donor. The slightly upfield shifts from those of free anthracene may be due to a synergistic effect caused by the donation from the other ligands present, especially three SnMe3 − anions, for which the shift is most pronounced. To date, the analogous reaction using naphthalene instead of anthracene has not been performed.

Synthesis and crystallization

A clear blue solution of CoBr2 (0.500 g, 2.29 mmol) in THF (60 ml, 195 K) was added to a deep-blue solution of K[C14H10] (6.86 mmol) in THF (60 ml, 195 K). To the resulting deep pinkish-red solution was added SnMe3Cl (0.455 g, 2.29 mmol) in THF (20 ml, 195 K), which dulled the color. After slow warming to room temperature, the solution was filtered to remove KBr and KCl. The solvent was removed under vacuum, and the product was extracted into pentane (25 ml) and filtered to give an intense violet solution. After the filtrate was cooled to and kept at 273 K for one h, the violet supernatant was carefully transferred to another vessel and placed in a freezer (243 K) for two days, during which time big purple–black crystals of the title complex formed. No attempts to establish the yield or obtain bulk elemental analyses were carried out. However, the product was characterized using the single crystals in solution by NMR and in the solid state by single-crystal X-ray diffraction. 1H NMR (300 MHz, CDCl3, 293 K, δ, p.p.m.): 8.32 (s, 2H, H9,10), 7.90 (m, 2H, H5,8 or H6,7), 7.48 (m, 2H, H5,8 or H6,7), 7.27 (CDCl3), 6.79 (m, 2H, H1,4 or H2,3), 5.98 (m, 2H, H1,4 or H2,3), 0.01 [s, 27H, 2 J(1H119Sn) = 20.6 Hz, CH 3], 13C{1H} NMR (75.5 MHz, CDCl3, 293 K, δ, p.p.m.): 127.8 (An), 127.4 (An), 126.9 (An), 93.3 (An), 86.3 (An), 77.2 (t, CDCl3), −2.9 (CH3). Quaternary carbon resonances were not resolved.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▶. In each of the two independent mol­ecules, the trio of SnMe3 ligands are modeled as disordered over two positions, such that the carbon atoms nearly overlap. In the mol­ecule containing Co1 the disorder ratio refined to 0.9366 (8):0.0634 (8). That for the other mol­ecule refined to 0.9685 (8):0.0315 (8). Despite the small fraction of the minor components, when the disorders are not modeled, the R1 residual increases from 0.0375 to 0.0538. For each disorder model, analogous bond lengths and angles were heavily restrained to be similar. Anisotropic displacement parameters for pairs of near-isopositional carbon atoms were constrained to be equivalent.
Table 2

Experimental details

Crystal data
Chemical formula[CoSn3(CH3)9(C14H10)]
M r 728.52
Crystal system, space groupTriclinic, P
Temperature (K)173
a, b, c ()12.9784(18), 13.0834(18), 16.734(2)
, , ()72.754(2), 75.891(2), 89.551(2)
V (3)2625.5(6)
Z 4
Radiation typeMo K
(mm1)3.45
Crystal size (mm)0.28 0.24 0.06
 
Data collection
DiffractometerSiemens SMART CCD platform
Absorption correctionMulti-scan (SADABS; Sheldrick, 2012)
T min, T max 0.493, 0.746
No. of measured, independent and observed [I > 2(I)] reflections30588, 11891, 9564
R int 0.032
(sin /)max (1)0.650
 
Refinement
R[F 2 > 2(F 2)], wR(F 2), S 0.038, 0.086, 1.08
No. of reflections11891
No. of parameters639
No. of restraints42
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
max, min (e 3)1.93, 0.79

Computer programs: SMART and SAINT (Bruker, 2003 ▶), SHELXS97, SHELXL2014 and SHELXTL (Sheldrick, 2008 ▶).

The rather large residual peak in the difference map (1.93 electrons per Å3, located 1.74 Å from atom C4) has no chemical meaning. It (and other similar smaller peaks) is likely due to a very minor twin component whose twin law is [ 0 0 / 0 0 / −0.623 −0.754 1], a 180 degree rotation about [001] (Parsons et al., 2003 ▶). H-atom positions of cobalt-coordinating carbon atoms were refined freely, but with relative displacement parameters. All other H atoms were placed geometrically and treated as riding atoms: sp 2, C—H = 0.95 Å, with U iso(H) = 1.2U eq(C), and methyl, C—H = 0.98 Å with U iso(H) = 1.5U eq(C). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536814021709/bg2536sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814021709/bg2536Isup2.hkl CCDC reference: 1027247 Additional supporting information: crystallographic information; 3D view; checkCIF report
[CoSn3(C14H10)(CH3)9]Z = 4
Mr = 728.52F(000) = 1408
Triclinic, P1Dx = 1.843 Mg m3
a = 12.9784 (18) ÅMo Kα radiation, λ = 0.71073 Å
b = 13.0834 (18) ÅCell parameters from 3885 reflections
c = 16.734 (2) ŵ = 3.45 mm1
α = 72.754 (2)°T = 173 K
β = 75.891 (2)°Plate, dark purple
γ = 89.551 (2)°0.28 × 0.24 × 0.06 mm
V = 2625.5 (6) Å3
Siemens SMART CCD platform diffractometer9564 reflections with I > 2σ(I)
Radiation source: normal-focus sealed tubeRint = 0.032
ω scansθmax = 27.5°, θmin = 1.3°
Absorption correction: multi-scan (SADABS; Sheldrick, 2012)h = −16→16
Tmin = 0.493, Tmax = 0.746k = −16→16
30588 measured reflectionsl = −21→21
11891 independent reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: mixed
wR(F2) = 0.086H atoms treated by a mixture of independent and constrained refinement
S = 1.08w = 1/[σ2(Fo2) + (0.032P)2 + 4.7781P] where P = (Fo2 + 2Fc2)/3
11891 reflections(Δ/σ)max = 0.001
639 parametersΔρmax = 1.93 e Å3
42 restraintsΔρmin = −0.79 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. The largest residual peak of 1.93 electrons per Å3, located 1.74 Å from atom C4, has no chemical meaning. It (and other smaller peaks that likewise having no chemical meaning) is likely due to a very minor twin component whose twin law is [-1 0 0 / 0 - 1 0 / -0.623 - 0.754 1], a 180 degree rotation about [001] (Parsons, 2003).In each of the two independent molecules, the trio of SnMe3 ligands are modeled as disordered over two positions, such that the carbon atoms nearly overlap. In the molecule containing Co1 the disorder ratio refined to 0.9366 (8):0.0634 (8). That for the other molecule refined to 0.9686 (8):0.0314 (8). Despite the small mass of the minor components, when the disorders are not modeled, the R1 residual increases from 0.0375 to 0.0538.For each disorder model, analogous bond lengths and angles were heavily restrained to be similar. Anisotropic displacement parameters for pairs of near-isopositional carbon atoms were constrained to be equivalent.H atom positions of cobalt-coordinated carbon atoms were refined freely, but with relative thermal parameters as described below. All other H atoms were placed geometrically and treated as riding atoms: sp2, C—H = 0.95 Å, with Uiso(H) = 1.2Ueq(C), and methyl, C—H = 0.98 Å with Uiso(H) = 1.5Ueq(C).
xyzUiso*/UeqOcc. (<1)
Co10.37703 (4)0.13516 (5)0.21652 (4)0.02862 (14)
C10.3223 (4)0.0682 (4)0.1335 (4)0.0415 (12)
H10.362 (4)0.067 (4)0.077 (4)0.050*
C20.2640 (4)0.1551 (5)0.1430 (4)0.0461 (13)
H20.260 (5)0.209 (5)0.097 (4)0.055*
C30.2146 (4)0.1582 (5)0.2279 (4)0.0517 (15)
H30.184 (5)0.217 (5)0.238 (4)0.062*
C40.2238 (4)0.0760 (5)0.3005 (4)0.0450 (13)
H40.196 (4)0.083 (4)0.359 (4)0.054*
C50.3347 (6)−0.2885 (5)0.4240 (4)0.0660 (18)
H50.3025−0.28710.48110.079*
C60.3857 (6)−0.3749 (5)0.4118 (5)0.0712 (19)
H60.3891−0.43280.46110.085*
C70.4344 (4)−0.3834 (4)0.3286 (4)0.0463 (13)
H70.4693−0.44550.32190.056*
C80.4293 (4)−0.2988 (4)0.2581 (4)0.0458 (13)
H80.4611−0.30310.20180.055*
C90.3733 (4)−0.1173 (4)0.1964 (3)0.0354 (10)
H90.4048−0.12100.13980.042*
C100.2779 (4)−0.1078 (5)0.3626 (4)0.0506 (14)
H100.2451−0.10560.41940.061*
C110.3238 (3)−0.0242 (4)0.2056 (3)0.0351 (11)
C120.2743 (4)−0.0195 (4)0.2919 (4)0.0418 (12)
C130.3286 (4)−0.1992 (4)0.3520 (3)0.0453 (13)
C140.3777 (4)−0.2042 (4)0.2670 (3)0.0383 (11)
Sn10.55882 (2)0.16207 (3)0.10994 (2)0.03084 (9)0.9365 (8)
C150.7078 (6)0.2100 (7)0.1306 (7)0.0558 (16)0.9365 (8)
H15A0.71290.16890.18870.084*0.9365 (8)
H15B0.71000.28680.12490.084*0.9365 (8)
H15C0.76760.19600.08750.084*0.9365 (8)
C160.6052 (8)0.0186 (5)0.0754 (4)0.0454 (15)0.9365 (8)
H16A0.67830.03050.03900.068*0.9365 (8)
H16B0.55710.00150.04350.068*0.9365 (8)
H16C0.6011−0.04120.12800.068*0.9365 (8)
C170.5498 (5)0.2734 (5)−0.0128 (4)0.0489 (14)0.9365 (8)
H17A0.61210.2687−0.05810.073*0.9365 (8)
H17B0.54830.3466−0.00860.073*0.9365 (8)
H17C0.48480.2553−0.02720.073*0.9365 (8)
Sn20.47432 (3)0.10385 (3)0.33620 (2)0.03731 (10)0.9365 (8)
C180.5817 (5)0.2171 (6)0.3523 (6)0.0574 (18)0.9365 (8)
H18A0.61020.18240.40210.086*0.9365 (8)
H18B0.54320.27880.36200.086*0.9365 (8)
H18C0.64050.24140.30010.086*0.9365 (8)
C190.3608 (8)0.0671 (7)0.4623 (4)0.068 (2)0.9365 (8)
H19A0.3480−0.01090.48790.102*0.9365 (8)
H19B0.29360.09870.45550.102*0.9365 (8)
H19C0.38970.09680.50030.102*0.9365 (8)
C200.5637 (5)−0.0349 (5)0.3326 (5)0.0568 (18)0.9365 (8)
H20A0.6340−0.02310.34140.085*0.9365 (8)
H20B0.5721−0.04670.27620.085*0.9365 (8)
H20C0.5256−0.09800.37840.085*0.9365 (8)
Sn30.39786 (3)0.33197 (3)0.20495 (2)0.03421 (9)0.9365 (8)
C210.5464 (5)0.4278 (4)0.1656 (4)0.0454 (15)0.9365 (8)
H21A0.53200.50260.16090.068*0.9365 (8)
H21B0.58720.42320.10930.068*0.9365 (8)
H21C0.58760.40100.20850.068*0.9365 (8)
C220.3205 (5)0.4202 (5)0.1061 (5)0.0527 (17)0.9365 (8)
H22A0.24600.39270.12170.079*0.9365 (8)
H22B0.35710.41100.05030.079*0.9365 (8)
H22C0.32370.49650.10180.079*0.9365 (8)
C230.3121 (5)0.3570 (5)0.3242 (4)0.0522 (16)0.9365 (8)
H23A0.35520.33740.36640.078*0.9365 (8)
H23B0.24500.31230.34690.078*0.9365 (8)
H23C0.29700.43270.31370.078*0.9365 (8)
Sn1'0.5647 (4)0.0882 (5)0.1893 (4)0.0500 (18)0.0635 (8)
C15'0.697 (7)0.210 (8)0.135 (7)0.0558 (16)0.0635 (8)
H15D0.69060.25790.17090.084*0.0635 (8)
H15E0.76420.17490.13420.084*0.0635 (8)
H15F0.69560.25100.07620.084*0.0635 (8)
C16'0.604 (12)−0.001 (6)0.097 (4)0.0454 (15)0.0635 (8)
H16D0.59010.04180.04190.068*0.0635 (8)
H16E0.6793−0.01540.08750.068*0.0635 (8)
H16F0.5599−0.06850.11910.068*0.0635 (8)
C17'0.601 (7)−0.021 (6)0.303 (3)0.0522 (16)0.0635 (8)
H17D0.58640.01180.34990.078*0.0635 (8)
H17E0.5575−0.08820.32090.078*0.0635 (8)
H17F0.6769−0.03510.28930.078*0.0635 (8)
Sn2'0.3993 (5)0.1957 (6)0.3414 (4)0.065 (2)0.0635 (8)
C18'0.554 (4)0.231 (8)0.356 (9)0.0574 (18)0.0635 (8)
H18D0.60120.17470.34630.086*0.0635 (8)
H18E0.58500.30030.31390.086*0.0635 (8)
H18F0.54770.23530.41470.086*0.0635 (8)
C19'0.349 (9)0.056 (5)0.455 (4)0.068 (2)0.0635 (8)
H19D0.3899−0.00460.44610.102*0.0635 (8)
H19E0.36070.07240.50580.102*0.0635 (8)
H19F0.27280.03700.46490.102*0.0635 (8)
C20'0.307 (5)0.326 (4)0.364 (5)0.0489 (14)0.0635 (8)
H20D0.23450.31510.35870.073*0.0635 (8)
H20E0.30290.32900.42290.073*0.0635 (8)
H20F0.34020.39390.32210.073*0.0635 (8)
Sn3'0.4487 (5)0.3255 (5)0.1205 (4)0.0535 (18)0.0635 (8)
C21'0.542 (6)0.450 (5)0.137 (5)0.0454 (15)0.0635 (8)
H21D0.51460.45610.19520.068*0.0635 (8)
H21E0.61650.43200.12900.068*0.0635 (8)
H21F0.53730.51840.09390.068*0.0635 (8)
C22'0.299 (4)0.400 (6)0.119 (6)0.0527 (17)0.0635 (8)
H22D0.26470.40460.17730.079*0.0635 (8)
H22E0.31200.47290.07820.079*0.0635 (8)
H22F0.25150.35760.10210.079*0.0635 (8)
C23'0.516 (6)0.320 (6)−0.009 (2)0.0568 (18)0.0635 (8)
H23D0.47690.2646−0.02010.085*0.0635 (8)
H23E0.51200.3899−0.05030.085*0.0635 (8)
H23F0.59120.3035−0.01520.085*0.0635 (8)
Co20.00682 (4)0.36883 (5)0.78274 (4)0.02670 (13)
C24−0.0921 (4)0.4357 (4)0.8698 (3)0.0363 (11)
H24−0.090 (4)0.437 (4)0.922 (3)0.044*
C25−0.1491 (4)0.3499 (4)0.8624 (4)0.0395 (11)
H25−0.181 (4)0.292 (4)0.914 (4)0.047*
C26−0.1519 (4)0.3471 (5)0.7790 (4)0.0429 (12)
H26−0.192 (4)0.291 (4)0.778 (3)0.051*
C27−0.1030 (4)0.4293 (4)0.7063 (3)0.0384 (11)
H27−0.103 (4)0.422 (4)0.652 (4)0.046*
C280.0525 (5)0.8050 (5)0.5773 (4)0.0524 (14)
H280.04340.80710.52220.063*
C290.0933 (5)0.8922 (5)0.5886 (4)0.0621 (17)
H290.11270.95570.54080.074*
C300.1081 (5)0.8923 (5)0.6696 (4)0.0637 (17)
H300.13930.95470.67480.076*
C310.0788 (4)0.8054 (4)0.7391 (4)0.0461 (13)
H310.08880.80700.79310.055*
C32−0.0046 (4)0.6209 (4)0.8032 (3)0.0381 (11)
H320.00160.62220.85830.046*
C33−0.0198 (4)0.6166 (4)0.6414 (3)0.0436 (12)
H33−0.02430.61510.58590.052*
C34−0.0510 (4)0.5279 (4)0.7965 (3)0.0347 (10)
C35−0.0569 (4)0.5249 (4)0.7129 (3)0.0358 (11)
C360.0227 (4)0.7085 (4)0.6489 (3)0.0390 (11)
C370.0323 (4)0.7102 (4)0.7325 (3)0.0379 (11)
Sn40.12611 (2)0.33492 (3)0.88667 (2)0.02952 (8)0.9686 (8)
C380.2862 (4)0.2827 (5)0.8632 (4)0.0469 (14)0.9686 (8)
H38A0.31190.27060.91550.070*0.9686 (8)
H38B0.33310.33810.81540.070*0.9686 (8)
H38C0.28620.21590.84820.070*0.9686 (8)
C390.1534 (4)0.4762 (5)0.9231 (4)0.0424 (14)0.9686 (8)
H39A0.20240.46090.96080.064*0.9686 (8)
H39B0.08560.49570.95400.064*0.9686 (8)
H39C0.18460.53570.87110.064*0.9686 (8)
C400.0413 (5)0.2233 (5)1.0099 (4)0.0519 (15)0.9686 (8)
H40A0.08010.22141.05370.078*0.9686 (8)
H40B0.03570.15151.00380.078*0.9686 (8)
H40C−0.03030.24671.02780.078*0.9686 (8)
Sn50.17472 (2)0.40061 (3)0.65953 (2)0.03177 (9)0.9686 (8)
C410.2885 (5)0.2841 (5)0.6367 (4)0.0550 (17)0.9686 (8)
H41A0.34710.31870.58640.083*0.9686 (8)
H41B0.25320.22550.62590.083*0.9686 (8)
H41C0.31660.25550.68770.083*0.9686 (8)
C420.1347 (5)0.4509 (6)0.5354 (4)0.0554 (17)0.9686 (8)
H42A0.18880.42920.49260.083*0.9686 (8)
H42B0.13220.52910.51650.083*0.9686 (8)
H42C0.06500.41720.54130.083*0.9686 (8)
C430.2710 (5)0.5340 (5)0.6633 (4)0.0466 (14)0.9686 (8)
H43A0.33670.54730.61690.070*0.9686 (8)
H43B0.28870.51620.71930.070*0.9686 (8)
H43C0.23080.59840.65550.070*0.9686 (8)
Sn60.01690 (3)0.17235 (3)0.79114 (2)0.03626 (9)0.9686 (8)
C440.1420 (5)0.0721 (5)0.8241 (5)0.0539 (16)0.9686 (8)
H44A0.1251−0.00080.82430.081*0.9686 (8)
H44B0.14830.07060.88160.081*0.9686 (8)
H44C0.20950.10100.78140.081*0.9686 (8)
C45−0.1180 (5)0.0839 (5)0.8929 (5)0.0530 (16)0.9686 (8)
H45A−0.11930.00830.89480.080*0.9686 (8)
H45B−0.18410.11400.88130.080*0.9686 (8)
H45C−0.11160.08940.94870.080*0.9686 (8)
C46−0.0068 (5)0.1551 (5)0.6712 (4)0.0544 (16)0.9686 (8)
H46A−0.02680.07990.67980.082*0.9686 (8)
H46B0.05940.17800.62550.082*0.9686 (8)
H46C−0.06360.19980.65440.082*0.9686 (8)
Sn4'0.1818 (9)0.4147 (9)0.8092 (8)0.053 (4)0.0314 (8)
C38'0.295 (8)0.293 (7)0.830 (8)0.0469 (14)0.0314 (8)
H38D0.29970.25350.78760.070*0.0314 (8)
H38E0.36490.32750.82180.070*0.0314 (8)
H38F0.27110.24370.88830.070*0.0314 (8)
C39'0.191 (11)0.485 (8)0.910 (5)0.0424 (14)0.0314 (8)
H39D0.14230.54300.90860.064*0.0314 (8)
H39E0.16990.42990.96620.064*0.0314 (8)
H39F0.26370.51370.89970.064*0.0314 (8)
C40'0.264 (10)0.540 (6)0.693 (4)0.0466 (14)0.0314 (8)
H40D0.21680.59800.67970.070*0.0314 (8)
H40E0.32840.56770.70210.070*0.0314 (8)
H40F0.28330.50990.64440.070*0.0314 (8)
Sn5'0.1087 (11)0.3209 (11)0.6522 (7)0.061 (4)0.0314 (8)
C41'0.279 (2)0.305 (11)0.619 (11)0.0550 (17)0.0314 (8)
H41D0.29740.24800.66540.083*0.0314 (8)
H41E0.29940.28720.56490.083*0.0314 (8)
H41F0.31630.37300.61240.083*0.0314 (8)
C42'0.096 (12)0.450 (7)0.539 (6)0.0554 (17)0.0314 (8)
H42D0.02120.46720.54480.083*0.0314 (8)
H42E0.13870.51410.53460.083*0.0314 (8)
H42F0.12180.42830.48710.083*0.0314 (8)
C43'0.040 (11)0.176 (6)0.641 (9)0.0544 (16)0.0314 (8)
H43D−0.03750.17650.65490.082*0.0314 (8)
H43E0.06670.17290.58160.082*0.0314 (8)
H43F0.06100.11280.68110.082*0.0314 (8)
Sn6'0.0243 (11)0.1762 (9)0.8696 (8)0.067 (5)0.0314 (8)
C44'0.152 (7)0.078 (9)0.838 (9)0.0539 (16)0.0314 (8)
H44D0.22010.11430.83200.081*0.0314 (8)
H44E0.14200.00890.88340.081*0.0314 (8)
H44F0.15170.06520.78270.081*0.0314 (8)
C45'−0.111 (6)0.074 (9)0.877 (9)0.0530 (16)0.0314 (8)
H45D−0.17670.10880.89120.080*0.0314 (8)
H45E−0.10330.06130.82070.080*0.0314 (8)
H45F−0.11300.00510.92140.080*0.0314 (8)
C46'0.012 (11)0.178 (11)1.001 (3)0.0519 (15)0.0314 (8)
H46D−0.04540.22221.01790.078*0.0314 (8)
H46E−0.00300.10451.04070.078*0.0314 (8)
H46F0.07960.20771.00440.078*0.0314 (8)
U11U22U33U12U13U23
Co10.0235 (3)0.0335 (3)0.0337 (3)0.0020 (2)−0.0095 (2)−0.0155 (3)
C10.033 (3)0.057 (3)0.048 (3)0.001 (2)−0.018 (2)−0.030 (3)
C20.033 (3)0.054 (3)0.068 (4)0.009 (2)−0.032 (3)−0.026 (3)
C30.022 (2)0.061 (4)0.084 (5)0.006 (2)−0.014 (3)−0.040 (4)
C40.031 (3)0.050 (3)0.054 (3)−0.006 (2)0.000 (2)−0.025 (3)
C50.094 (5)0.048 (4)0.042 (3)−0.011 (3)0.000 (3)−0.006 (3)
C60.090 (5)0.048 (4)0.061 (4)−0.007 (3)−0.009 (4)−0.002 (3)
C70.044 (3)0.045 (3)0.048 (3)−0.001 (2)−0.004 (2)−0.018 (3)
C80.040 (3)0.050 (3)0.051 (3)0.003 (2)−0.008 (2)−0.023 (3)
C90.032 (2)0.044 (3)0.035 (3)0.000 (2)−0.0075 (19)−0.019 (2)
C100.050 (3)0.051 (3)0.044 (3)−0.017 (3)0.008 (2)−0.020 (3)
C110.026 (2)0.041 (3)0.045 (3)−0.0019 (19)−0.011 (2)−0.021 (2)
C120.029 (2)0.048 (3)0.051 (3)−0.007 (2)0.001 (2)−0.026 (3)
C130.045 (3)0.043 (3)0.042 (3)−0.012 (2)0.001 (2)−0.012 (2)
C140.033 (2)0.043 (3)0.042 (3)−0.006 (2)−0.008 (2)−0.018 (2)
Sn10.02348 (16)0.03726 (19)0.03407 (19)0.00299 (13)−0.00831 (13)−0.01343 (15)
C150.030 (3)0.064 (4)0.082 (5)0.002 (3)−0.017 (3)−0.034 (3)
C160.037 (3)0.055 (4)0.048 (4)0.011 (3)−0.006 (3)−0.026 (3)
C170.041 (3)0.058 (4)0.040 (3)0.004 (3)−0.008 (2)−0.006 (3)
Sn20.0451 (2)0.0371 (2)0.0365 (2)0.00380 (15)−0.02069 (16)−0.01288 (16)
C180.064 (4)0.062 (4)0.063 (4)0.003 (3)−0.039 (4)−0.027 (3)
C190.092 (5)0.076 (5)0.038 (3)−0.007 (4)−0.020 (3)−0.015 (3)
C200.065 (5)0.054 (4)0.066 (4)0.024 (3)−0.039 (4)−0.021 (3)
Sn30.03129 (18)0.03110 (18)0.0436 (2)0.00540 (13)−0.01187 (15)−0.01455 (15)
C210.040 (3)0.035 (3)0.059 (4)−0.004 (2)−0.018 (3)−0.005 (3)
C220.047 (3)0.047 (4)0.064 (4)0.015 (3)−0.020 (3)−0.012 (3)
C230.055 (4)0.050 (4)0.055 (4)0.013 (3)−0.009 (3)−0.026 (3)
Sn1'0.037 (3)0.061 (4)0.059 (4)0.003 (3)−0.013 (3)−0.027 (3)
C15'0.030 (3)0.064 (4)0.082 (5)0.002 (3)−0.017 (3)−0.034 (3)
C16'0.037 (3)0.055 (4)0.048 (4)0.011 (3)−0.006 (3)−0.026 (3)
C17'0.055 (4)0.050 (4)0.055 (4)0.013 (3)−0.009 (3)−0.026 (3)
Sn2'0.066 (4)0.084 (5)0.051 (4)−0.022 (4)−0.011 (3)−0.034 (4)
C18'0.064 (4)0.062 (4)0.063 (4)0.003 (3)−0.039 (4)−0.027 (3)
C19'0.092 (5)0.076 (5)0.038 (3)−0.007 (4)−0.020 (3)−0.015 (3)
C20'0.041 (3)0.058 (4)0.040 (3)0.004 (3)−0.008 (2)−0.006 (3)
Sn3'0.046 (4)0.060 (4)0.054 (4)0.008 (3)−0.017 (3)−0.012 (3)
C21'0.040 (3)0.035 (3)0.059 (4)−0.004 (2)−0.018 (3)−0.005 (3)
C22'0.047 (3)0.047 (4)0.064 (4)0.015 (3)−0.020 (3)−0.012 (3)
C23'0.065 (5)0.054 (4)0.066 (4)0.024 (3)−0.039 (4)−0.021 (3)
Co20.0242 (3)0.0307 (3)0.0301 (3)0.0025 (2)−0.0111 (2)−0.0132 (3)
C240.032 (2)0.047 (3)0.036 (3)0.015 (2)−0.010 (2)−0.021 (2)
C250.021 (2)0.042 (3)0.051 (3)0.0059 (19)−0.005 (2)−0.010 (2)
C260.027 (2)0.052 (3)0.061 (4)0.003 (2)−0.024 (2)−0.024 (3)
C270.040 (3)0.044 (3)0.044 (3)0.011 (2)−0.027 (2)−0.019 (2)
C280.067 (4)0.047 (3)0.039 (3)0.005 (3)−0.004 (3)−0.014 (3)
C290.073 (4)0.047 (4)0.051 (4)−0.001 (3)0.000 (3)−0.006 (3)
C300.067 (4)0.049 (4)0.071 (4)−0.011 (3)−0.004 (3)−0.023 (3)
C310.040 (3)0.049 (3)0.058 (3)0.004 (2)−0.012 (2)−0.030 (3)
C320.034 (2)0.056 (3)0.035 (3)0.007 (2)−0.012 (2)−0.026 (2)
C330.059 (3)0.044 (3)0.034 (3)0.011 (2)−0.020 (2)−0.015 (2)
C340.029 (2)0.045 (3)0.034 (3)0.009 (2)−0.0116 (19)−0.016 (2)
C350.037 (3)0.040 (3)0.041 (3)0.011 (2)−0.022 (2)−0.020 (2)
C360.041 (3)0.043 (3)0.037 (3)0.012 (2)−0.011 (2)−0.016 (2)
C370.036 (3)0.037 (3)0.051 (3)0.013 (2)−0.022 (2)−0.021 (2)
Sn40.02549 (16)0.03679 (18)0.03028 (17)0.00225 (12)−0.01220 (12)−0.01196 (14)
C380.033 (3)0.059 (4)0.059 (4)0.011 (2)−0.022 (3)−0.024 (3)
C390.038 (3)0.054 (3)0.050 (3)0.004 (2)−0.020 (2)−0.029 (3)
C400.048 (3)0.064 (4)0.036 (3)−0.004 (3)−0.014 (2)0.000 (3)
Sn50.02953 (17)0.03985 (19)0.02961 (17)0.00062 (13)−0.00817 (13)−0.01540 (14)
C410.049 (3)0.059 (4)0.059 (4)0.014 (3)−0.006 (3)−0.027 (3)
C420.052 (4)0.089 (5)0.032 (3)0.002 (3)−0.017 (3)−0.023 (3)
C430.043 (3)0.051 (3)0.045 (3)−0.012 (2)−0.013 (3)−0.012 (3)
Sn60.03465 (18)0.03089 (18)0.0499 (2)0.00055 (13)−0.01780 (15)−0.01638 (16)
C440.060 (4)0.035 (3)0.076 (5)0.014 (3)−0.031 (3)−0.019 (3)
C450.042 (3)0.046 (3)0.070 (4)−0.009 (2)−0.021 (3)−0.009 (3)
C460.060 (4)0.055 (4)0.066 (4)0.004 (3)−0.029 (3)−0.036 (3)
Sn4'0.038 (6)0.074 (9)0.062 (9)0.009 (6)−0.026 (6)−0.032 (7)
C38'0.033 (3)0.059 (4)0.059 (4)0.011 (2)−0.022 (3)−0.024 (3)
C39'0.038 (3)0.054 (3)0.050 (3)0.004 (2)−0.020 (2)−0.029 (3)
C40'0.043 (3)0.051 (3)0.045 (3)−0.012 (2)−0.013 (3)−0.012 (3)
Sn5'0.059 (8)0.082 (10)0.064 (9)0.016 (7)−0.026 (7)−0.046 (8)
C41'0.049 (3)0.059 (4)0.059 (4)0.014 (3)−0.006 (3)−0.027 (3)
C42'0.052 (4)0.089 (5)0.032 (3)0.002 (3)−0.017 (3)−0.023 (3)
C43'0.060 (4)0.055 (4)0.066 (4)0.004 (3)−0.029 (3)−0.036 (3)
Sn6'0.067 (9)0.053 (9)0.072 (10)0.000 (7)−0.021 (8)−0.005 (7)
C44'0.060 (4)0.035 (3)0.076 (5)0.014 (3)−0.031 (3)−0.019 (3)
C45'0.042 (3)0.046 (3)0.070 (4)−0.009 (2)−0.021 (3)−0.009 (3)
C46'0.048 (3)0.064 (4)0.036 (3)−0.004 (3)−0.014 (2)0.000 (3)
Co1—C32.098 (5)Co2—C242.088 (5)
Co1—C12.101 (5)Co2—C262.100 (5)
Co1—C22.102 (5)Co2—C252.104 (5)
Co1—C42.132 (5)Co2—C272.136 (5)
Co1—C112.273 (5)Co2—C342.264 (5)
Co1—C122.274 (5)Co2—C352.291 (5)
Co1—Sn1'2.474 (5)Co2—Sn5'2.512 (11)
Co1—Sn2'2.521 (5)Co2—Sn4'2.526 (10)
Co1—Sn32.5359 (8)Co2—Sn62.5366 (8)
Co1—Sn12.5418 (7)Co2—Sn42.5423 (7)
Co1—Sn22.5518 (7)Co2—Sn52.5471 (7)
Co1—Sn3'2.566 (6)Co2—Sn6'2.549 (12)
C1—C21.387 (7)C24—C251.400 (7)
C1—C111.438 (7)C24—C341.435 (7)
C1—H10.97 (5)C24—H240.89 (5)
C2—C31.423 (8)C25—C261.416 (8)
C2—H20.88 (6)C25—H250.96 (5)
C3—C41.393 (9)C26—C271.377 (8)
C3—H30.91 (6)C26—H260.91 (6)
C4—C121.436 (7)C27—C351.435 (7)
C4—H40.99 (6)C27—H270.94 (5)
C5—C61.348 (9)C28—C291.343 (8)
C5—C131.425 (8)C28—C361.437 (7)
C5—H50.9500C28—H280.9500
C6—C71.418 (8)C29—C301.417 (9)
C6—H60.9500C29—H290.9500
C7—C81.373 (8)C30—C311.340 (8)
C7—H70.9500C30—H300.9500
C8—C141.431 (7)C31—C371.434 (7)
C8—H80.9500C31—H310.9500
C9—C141.388 (7)C32—C371.382 (7)
C9—C111.403 (7)C32—C341.406 (7)
C9—H90.9500C32—H320.9500
C10—C131.397 (8)C33—C361.378 (7)
C10—C121.398 (8)C33—C351.407 (7)
C10—H100.9500C33—H330.9500
C11—C121.449 (7)C34—C351.432 (6)
C13—C141.431 (7)C36—C371.440 (7)
Sn1—C162.162 (5)Sn4—C382.163 (5)
Sn1—C172.167 (6)Sn4—C392.167 (5)
Sn1—C152.174 (6)Sn4—C402.175 (5)
C15—H15A0.9800C38—H38A0.9800
C15—H15B0.9800C38—H38B0.9800
C15—H15C0.9800C38—H38C0.9800
C16—H16A0.9800C39—H39A0.9800
C16—H16B0.9800C39—H39B0.9800
C16—H16C0.9800C39—H39C0.9800
C17—H17A0.9800C40—H40A0.9800
C17—H17B0.9800C40—H40B0.9800
C17—H17C0.9800C40—H40C0.9800
Sn2—C202.155 (6)Sn5—C412.164 (6)
Sn2—C182.159 (6)Sn5—C422.174 (5)
Sn2—C192.179 (7)Sn5—C432.179 (5)
C18—H18A0.9800C41—H41A0.9800
C18—H18B0.9800C41—H41B0.9800
C18—H18C0.9800C41—H41C0.9800
C19—H19A0.9800C42—H42A0.9800
C19—H19B0.9800C42—H42B0.9800
C19—H19C0.9800C42—H42C0.9800
C20—H20A0.9800C43—H43A0.9800
C20—H20B0.9800C43—H43B0.9800
C20—H20C0.9800C43—H43C0.9800
Sn3—C232.151 (6)Sn6—C442.152 (6)
Sn3—C212.157 (5)Sn6—C452.172 (6)
Sn3—C222.176 (6)Sn6—C462.177 (6)
C21—H21A0.9800C44—H44A0.9800
C21—H21B0.9800C44—H44B0.9800
C21—H21C0.9800C44—H44C0.9800
C22—H22A0.9800C45—H45A0.9800
C22—H22B0.9800C45—H45B0.9800
C22—H22C0.9800C45—H45C0.9800
C23—H23A0.9800C46—H46A0.9800
C23—H23B0.9800C46—H46B0.9800
C23—H23C0.9800C46—H46C0.9800
Sn1'—C16'2.162 (7)Sn4'—C38'2.163 (6)
Sn1'—C17'2.167 (7)Sn4'—C39'2.167 (6)
Sn1'—C15'2.174 (7)Sn4'—C40'2.175 (7)
C15'—H15D0.9800C38'—H38D0.9800
C15'—H15E0.9800C38'—H38E0.9800
C15'—H15F0.9800C38'—H38F0.9800
C16'—H16D0.9800C39'—H39D0.9800
C16'—H16E0.9800C39'—H39E0.9800
C16'—H16F0.9800C39'—H39F0.9800
C17'—H17D0.9800C40'—H40D0.9800
C17'—H17E0.9800C40'—H40E0.9800
C17'—H17F0.9800C40'—H40F0.9800
Sn2'—C20'2.155 (7)Sn5'—C41'2.164 (7)
Sn2'—C18'2.159 (7)Sn5'—C42'2.174 (7)
Sn2'—C19'2.179 (8)Sn5'—C43'2.179 (7)
C18'—H18D0.9800C41'—H41D0.9800
C18'—H18E0.9800C41'—H41E0.9800
C18'—H18F0.9800C41'—H41F0.9800
C19'—H19D0.9800C42'—H42D0.9800
C19'—H19E0.9800C42'—H42E0.9800
C19'—H19F0.9800C42'—H42F0.9800
C20'—H20D0.9800C43'—H43D0.9800
C20'—H20E0.9800C43'—H43E0.9800
C20'—H20F0.9800C43'—H43F0.9800
Sn3'—C23'2.151 (7)Sn6'—C44'2.152 (7)
Sn3'—C21'2.157 (6)Sn6'—C45'2.172 (7)
Sn3'—C22'2.176 (7)Sn6'—C46'2.177 (7)
C21'—H21D0.9800C44'—H44D0.9800
C21'—H21E0.9800C44'—H44E0.9800
C21'—H21F0.9800C44'—H44F0.9800
C22'—H22D0.9800C45'—H45D0.9800
C22'—H22E0.9800C45'—H45E0.9800
C22'—H22F0.9800C45'—H45F0.9800
C23'—H23D0.9800C46'—H46D0.9800
C23'—H23E0.9800C46'—H46E0.9800
C23'—H23F0.9800C46'—H46F0.9800
C3—Co1—C170.3 (2)C24—Co2—C2670.8 (2)
C3—Co1—C239.6 (2)C24—Co2—C2539.0 (2)
C1—Co1—C238.5 (2)C26—Co2—C2539.4 (2)
C3—Co1—C438.4 (2)C24—Co2—C2783.0 (2)
C1—Co1—C483.1 (2)C26—Co2—C2737.9 (2)
C2—Co1—C470.8 (2)C25—Co2—C2769.9 (2)
C3—Co1—C1180.9 (2)C24—Co2—C3438.24 (18)
C1—Co1—C1138.1 (2)C26—Co2—C3481.00 (19)
C2—Co1—C1168.7 (2)C25—Co2—C3468.77 (19)
C4—Co1—C1168.30 (19)C27—Co2—C3467.99 (18)
C3—Co1—C1268.4 (2)C24—Co2—C3568.27 (19)
C1—Co1—C1268.8 (2)C26—Co2—C3567.7 (2)
C2—Co1—C1281.8 (2)C25—Co2—C3580.68 (19)
C4—Co1—C1237.86 (19)C27—Co2—C3537.62 (17)
C11—Co1—C1237.15 (17)C34—Co2—C3536.63 (16)
C3—Co1—Sn1'170.6 (2)C24—Co2—Sn5'166.4 (3)
C1—Co1—Sn1'100.5 (2)C26—Co2—Sn5'102.3 (3)
C2—Co1—Sn1'132.9 (2)C25—Co2—Sn5'139.3 (3)
C4—Co1—Sn1'141.2 (2)C27—Co2—Sn5'84.6 (3)
C11—Co1—Sn1'90.71 (18)C34—Co2—Sn5'130.5 (3)
C12—Co1—Sn1'107.26 (19)C35—Co2—Sn5'98.4 (3)
C3—Co1—Sn2'98.8 (2)C24—Co2—Sn4'97.6 (3)
C1—Co1—Sn2'165.9 (2)C26—Co2—Sn4'168.4 (3)
C2—Co1—Sn2'135.2 (2)C25—Co2—Sn4'130.4 (3)
C4—Co1—Sn2'82.8 (2)C27—Co2—Sn4'142.9 (3)
C11—Co1—Sn2'133.4 (2)C34—Co2—Sn4'89.6 (3)
C12—Co1—Sn2'99.2 (2)C35—Co2—Sn4'108.3 (3)
Sn1'—Co1—Sn2'90.02 (19)Sn5'—Co2—Sn4'89.0 (3)
C3—Co1—Sn386.04 (17)C24—Co2—Sn6127.92 (15)
C1—Co1—Sn3127.76 (16)C26—Co2—Sn685.08 (15)
C2—Co1—Sn395.20 (16)C25—Co2—Sn694.87 (14)
C4—Co1—Sn3106.55 (15)C27—Co2—Sn6105.56 (14)
C11—Co1—Sn3163.89 (13)C34—Co2—Sn6163.54 (12)
C12—Co1—Sn3143.26 (13)C35—Co2—Sn6142.22 (12)
C3—Co1—Sn1144.16 (19)C24—Co2—Sn485.28 (14)
C1—Co1—Sn186.74 (15)C26—Co2—Sn4141.95 (16)
C2—Co1—Sn1106.42 (17)C25—Co2—Sn4104.72 (15)
C4—Co1—Sn1166.18 (15)C27—Co2—Sn4166.36 (14)
C11—Co1—Sn197.96 (12)C34—Co2—Sn498.44 (12)
C12—Co1—Sn1129.04 (13)C35—Co2—Sn4130.42 (12)
Sn3—Co1—Sn187.09 (2)Sn6—Co2—Sn487.15 (2)
C3—Co1—Sn2126.82 (19)C24—Co2—Sn5145.11 (15)
C1—Co1—Sn2146.16 (16)C26—Co2—Sn5128.37 (16)
C2—Co1—Sn2166.12 (17)C25—Co2—Sn5167.34 (15)
C4—Co1—Sn295.78 (17)C27—Co2—Sn597.77 (15)
C11—Co1—Sn2110.27 (13)C34—Co2—Sn5109.82 (12)
C12—Co1—Sn289.63 (14)C35—Co2—Sn591.08 (13)
Sn3—Co1—Sn285.14 (2)Sn6—Co2—Sn585.73 (2)
Sn1—Co1—Sn287.46 (2)Sn4—Co2—Sn587.95 (2)
C3—Co1—Sn3'97.4 (2)C24—Co2—Sn6'105.7 (4)
C1—Co1—Sn3'103.7 (2)C26—Co2—Sn6'96.5 (3)
C2—Co1—Sn3'84.7 (2)C25—Co2—Sn6'85.8 (4)
C4—Co1—Sn3'130.8 (2)C27—Co2—Sn6'129.0 (3)
C11—Co1—Sn3'140.25 (19)C34—Co2—Sn6'142.7 (3)
C12—Co1—Sn3'165.27 (19)C35—Co2—Sn6'164.1 (3)
Sn1'—Co1—Sn3'86.31 (18)Sn5'—Co2—Sn6'86.5 (3)
Sn2'—Co1—Sn3'86.25 (19)Sn4'—Co2—Sn6'86.8 (3)
C2—C1—C11122.2 (5)C25—C24—C34121.2 (5)
C2—C1—Co170.8 (3)C25—C24—Co271.1 (3)
C11—C1—Co177.4 (3)C34—C24—Co277.5 (3)
C2—C1—H1121 (3)C25—C24—H24119 (3)
C11—C1—H1117 (3)C34—C24—H24119 (3)
Co1—C1—H1126 (3)Co2—C24—H24131 (3)
C1—C2—C3118.6 (6)C24—C25—C26118.9 (5)
C1—C2—Co170.7 (3)C24—C25—Co269.9 (3)
C3—C2—Co170.0 (3)C26—C25—Co270.1 (3)
C1—C2—H2121 (4)C24—C25—H25119 (3)
C3—C2—H2120 (4)C26—C25—H25121 (3)
Co1—C2—H2129 (4)Co2—C25—H25128 (3)
C4—C3—C2121.1 (5)C27—C26—C25120.7 (5)
C4—C3—Co172.1 (3)C27—C26—Co272.5 (3)
C2—C3—Co170.4 (3)C25—C26—Co270.5 (3)
C4—C3—H3116 (4)C27—C26—H26124 (4)
C2—C3—H3122 (4)C25—C26—H26115 (4)
Co1—C3—H3123 (4)Co2—C26—H26134 (4)
C3—C4—C12120.9 (5)C26—C27—C35121.3 (5)
C3—C4—Co169.5 (3)C26—C27—Co269.6 (3)
C12—C4—Co176.5 (3)C35—C27—Co277.1 (3)
C3—C4—H4120 (3)C26—C27—H27118 (3)
C12—C4—H4119 (3)C35—C27—H27120 (3)
Co1—C4—H4126 (3)Co2—C27—H27127 (3)
C6—C5—C13120.6 (6)C29—C28—C36119.7 (6)
C6—C5—H5119.7C29—C28—H28120.1
C13—C5—H5119.7C36—C28—H28120.1
C5—C6—C7122.9 (6)C28—C29—C30121.8 (6)
C5—C6—H6118.5C28—C29—H29119.1
C7—C6—H6118.5C30—C29—H29119.1
C8—C7—C6117.7 (5)C31—C30—C29120.8 (6)
C8—C7—H7121.1C31—C30—H30119.6
C6—C7—H7121.1C29—C30—H30119.6
C7—C8—C14122.0 (5)C30—C31—C37120.4 (6)
C7—C8—H8119.0C30—C31—H31119.8
C14—C8—H8119.0C37—C31—H31119.8
C14—C9—C11122.3 (4)C37—C32—C34122.3 (4)
C14—C9—H9118.9C37—C32—H32118.8
C11—C9—H9118.9C34—C32—H32118.8
C13—C10—C12121.6 (5)C36—C33—C35122.4 (5)
C13—C10—H10119.2C36—C33—H33118.8
C12—C10—H10119.2C35—C33—H33118.8
C9—C11—C1123.0 (5)C32—C34—C35118.6 (4)
C9—C11—C12118.8 (5)C32—C34—C24122.9 (4)
C1—C11—C12118.2 (4)C35—C34—C24118.5 (4)
C9—C11—Co1135.6 (3)C32—C34—Co2135.6 (3)
C1—C11—Co164.4 (3)C35—C34—Co272.7 (3)
C12—C11—Co171.5 (3)C24—C34—Co264.2 (3)
C10—C12—C4123.1 (5)C33—C35—C34118.6 (4)
C10—C12—C11118.7 (5)C33—C35—C27123.0 (4)
C4—C12—C11118.2 (5)C34—C35—C27118.4 (5)
C10—C12—Co1135.5 (4)C33—C35—Co2138.5 (4)
C4—C12—Co165.7 (3)C34—C35—Co270.6 (3)
C11—C12—Co171.4 (3)C27—C35—Co265.3 (3)
C10—C13—C5121.9 (5)C33—C36—C28122.4 (5)
C10—C13—C14119.9 (5)C33—C36—C37119.1 (5)
C5—C13—C14118.2 (5)C28—C36—C37118.5 (5)
C9—C14—C8122.6 (5)C32—C37—C31122.5 (5)
C9—C14—C13118.8 (5)C32—C37—C36119.0 (4)
C8—C14—C13118.6 (5)C31—C37—C36118.5 (5)
C16—Sn1—C17102.3 (2)C38—Sn4—C3999.8 (2)
C16—Sn1—C1599.3 (2)C38—Sn4—C40105.0 (2)
C17—Sn1—C15104.9 (3)C39—Sn4—C40101.9 (2)
C16—Sn1—Co1112.4 (2)C38—Sn4—Co2126.31 (15)
C17—Sn1—Co1109.18 (16)C39—Sn4—Co2112.00 (15)
C15—Sn1—Co1126.0 (3)C40—Sn4—Co2109.04 (16)
Sn1—C15—H15A109.5Sn4—C38—H38A109.5
Sn1—C15—H15B109.5Sn4—C38—H38B109.5
H15A—C15—H15B109.5H38A—C38—H38B109.5
Sn1—C15—H15C109.5Sn4—C38—H38C109.5
H15A—C15—H15C109.5H38A—C38—H38C109.5
H15B—C15—H15C109.5H38B—C38—H38C109.5
Sn1—C16—H16A109.5Sn4—C39—H39A109.5
Sn1—C16—H16B109.5Sn4—C39—H39B109.5
H16A—C16—H16B109.5H39A—C39—H39B109.5
Sn1—C16—H16C109.5Sn4—C39—H39C109.5
H16A—C16—H16C109.5H39A—C39—H39C109.5
H16B—C16—H16C109.5H39B—C39—H39C109.5
Sn1—C17—H17A109.5Sn4—C40—H40A109.5
Sn1—C17—H17B109.5Sn4—C40—H40B109.5
H17A—C17—H17B109.5H40A—C40—H40B109.5
Sn1—C17—H17C109.5Sn4—C40—H40C109.5
H17A—C17—H17C109.5H40A—C40—H40C109.5
H17B—C17—H17C109.5H40B—C40—H40C109.5
C20—Sn2—C18105.1 (3)C41—Sn5—C4299.8 (3)
C20—Sn2—C19108.1 (3)C41—Sn5—C43104.2 (3)
C18—Sn2—C1998.7 (3)C42—Sn5—C43106.4 (2)
C20—Sn2—Co1106.28 (18)C41—Sn5—Co2126.63 (18)
C18—Sn2—Co1127.0 (2)C42—Sn5—Co2110.42 (16)
C19—Sn2—Co1110.5 (3)C43—Sn5—Co2107.81 (16)
Sn2—C18—H18A109.5Sn5—C41—H41A109.5
Sn2—C18—H18B109.5Sn5—C41—H41B109.5
H18A—C18—H18B109.5H41A—C41—H41B109.5
Sn2—C18—H18C109.5Sn5—C41—H41C109.5
H18A—C18—H18C109.5H41A—C41—H41C109.5
H18B—C18—H18C109.5H41B—C41—H41C109.5
Sn2—C19—H19A109.5Sn5—C42—H42A109.5
Sn2—C19—H19B109.5Sn5—C42—H42B109.5
H19A—C19—H19B109.5H42A—C42—H42B109.5
Sn2—C19—H19C109.5Sn5—C42—H42C109.5
H19A—C19—H19C109.5H42A—C42—H42C109.5
H19B—C19—H19C109.5H42B—C42—H42C109.5
Sn2—C20—H20A109.5Sn5—C43—H43A109.5
Sn2—C20—H20B109.5Sn5—C43—H43B109.5
H20A—C20—H20B109.5H43A—C43—H43B109.5
Sn2—C20—H20C109.5Sn5—C43—H43C109.5
H20A—C20—H20C109.5H43A—C43—H43C109.5
H20B—C20—H20C109.5H43B—C43—H43C109.5
C23—Sn3—C21105.8 (3)C44—Sn6—C4599.8 (3)
C23—Sn3—C22106.6 (3)C44—Sn6—C46107.4 (2)
C21—Sn3—C22100.4 (2)C45—Sn6—C46106.1 (2)
C23—Sn3—Co1109.53 (18)C44—Sn6—Co2126.20 (17)
C21—Sn3—Co1125.91 (17)C45—Sn6—Co2107.62 (18)
C22—Sn3—Co1106.98 (19)C46—Sn6—Co2108.02 (17)
Sn3—C21—H21A109.5Sn6—C44—H44A109.5
Sn3—C21—H21B109.5Sn6—C44—H44B109.5
H21A—C21—H21B109.5H44A—C44—H44B109.5
Sn3—C21—H21C109.5Sn6—C44—H44C109.5
H21A—C21—H21C109.5H44A—C44—H44C109.5
H21B—C21—H21C109.5H44B—C44—H44C109.5
Sn3—C22—H22A109.5Sn6—C45—H45A109.5
Sn3—C22—H22B109.5Sn6—C45—H45B109.5
H22A—C22—H22B109.5H45A—C45—H45B109.5
Sn3—C22—H22C109.5Sn6—C45—H45C109.5
H22A—C22—H22C109.5H45A—C45—H45C109.5
H22B—C22—H22C109.5H45B—C45—H45C109.5
Sn3—C23—H23A109.5Sn6—C46—H46A109.5
Sn3—C23—H23B109.5Sn6—C46—H46B109.5
H23A—C23—H23B109.5H46A—C46—H46B109.5
Sn3—C23—H23C109.5Sn6—C46—H46C109.5
H23A—C23—H23C109.5H46A—C46—H46C109.5
H23B—C23—H23C109.5H46B—C46—H46C109.5
C16'—Sn1'—C17'102.3 (5)C38'—Sn4'—C39'99.8 (4)
C16'—Sn1'—C15'99.3 (4)C38'—Sn4'—C40'105.0 (5)
C17'—Sn1'—C15'104.9 (5)C39'—Sn4'—C40'101.9 (5)
C16'—Sn1'—Co1113 (4)C38'—Sn4'—Co2120 (4)
C17'—Sn1'—Co1113 (2)C39'—Sn4'—Co2122 (4)
C15'—Sn1'—Co1122 (3)C40'—Sn4'—Co2106 (4)
Sn1'—C15'—H15D109.5Sn4'—C38'—H38D109.5
Sn1'—C15'—H15E109.5Sn4'—C38'—H38E109.5
H15D—C15'—H15E109.5H38D—C38'—H38E109.5
Sn1'—C15'—H15F109.5Sn4'—C38'—H38F109.5
H15D—C15'—H15F109.5H38D—C38'—H38F109.5
H15E—C15'—H15F109.5H38E—C38'—H38F109.5
Sn1'—C16'—H16D109.5Sn4'—C39'—H39D109.5
Sn1'—C16'—H16E109.5Sn4'—C39'—H39E109.5
H16D—C16'—H16E109.5H39D—C39'—H39E109.5
Sn1'—C16'—H16F109.5Sn4'—C39'—H39F109.5
H16D—C16'—H16F109.5H39D—C39'—H39F109.5
H16E—C16'—H16F109.5H39E—C39'—H39F109.5
Sn1'—C17'—H17D109.5Sn4'—C40'—H40D109.5
Sn1'—C17'—H17E109.5Sn4'—C40'—H40E109.5
H17D—C17'—H17E109.5H40D—C40'—H40E109.5
Sn1'—C17'—H17F109.5Sn4'—C40'—H40F109.5
H17D—C17'—H17F109.5H40D—C40'—H40F109.5
H17E—C17'—H17F109.5H40E—C40'—H40F109.5
C20'—Sn2'—C18'105.1 (5)C41'—Sn5'—C42'99.8 (5)
C20'—Sn2'—C19'108.1 (5)C41'—Sn5'—C43'104.2 (5)
C18'—Sn2'—C19'98.7 (5)C42'—Sn5'—C43'106.4 (5)
C20'—Sn2'—Co1116 (2)C41'—Sn5'—Co2125 (5)
C18'—Sn2'—Co1122 (3)C42'—Sn5'—Co2107 (4)
C19'—Sn2'—Co1105 (3)C43'—Sn5'—Co2112 (4)
Sn2'—C18'—H18D109.5Sn5'—C41'—H41D109.5
Sn2'—C18'—H18E109.5Sn5'—C41'—H41E109.5
H18D—C18'—H18E109.5H41D—C41'—H41E109.5
Sn2'—C18'—H18F109.5Sn5'—C41'—H41F109.5
H18D—C18'—H18F109.5H41D—C41'—H41F109.5
H18E—C18'—H18F109.5H41E—C41'—H41F109.5
Sn2'—C19'—H19D109.5Sn5'—C42'—H42D109.5
Sn2'—C19'—H19E109.5Sn5'—C42'—H42E109.5
H19D—C19'—H19E109.5H42D—C42'—H42E109.5
Sn2'—C19'—H19F109.5Sn5'—C42'—H42F109.5
H19D—C19'—H19F109.5H42D—C42'—H42F109.5
H19E—C19'—H19F109.5H42E—C42'—H42F109.5
Sn2'—C20'—H20D109.5Sn5'—C43'—H43D109.5
Sn2'—C20'—H20E109.5Sn5'—C43'—H43E109.5
H20D—C20'—H20E109.5H43D—C43'—H43E109.5
Sn2'—C20'—H20F109.5Sn5'—C43'—H43F109.5
H20D—C20'—H20F109.5H43D—C43'—H43F109.5
H20E—C20'—H20F109.5H43E—C43'—H43F109.5
C23'—Sn3'—C21'105.8 (5)C44'—Sn6'—C45'99.8 (5)
C23'—Sn3'—C22'106.6 (5)C44'—Sn6'—C46'107.4 (5)
C21'—Sn3'—C22'100.4 (4)C45'—Sn6'—C46'106.1 (5)
C23'—Sn3'—Co1108 (2)C44'—Sn6'—Co2126 (4)
C21'—Sn3'—Co1133 (2)C45'—Sn6'—Co2110 (4)
C22'—Sn3'—Co199 (2)C46'—Sn6'—Co2106 (4)
Sn3'—C21'—H21D109.5Sn6'—C44'—H44D109.5
Sn3'—C21'—H21E109.5Sn6'—C44'—H44E109.5
H21D—C21'—H21E109.5H44D—C44'—H44E109.5
Sn3'—C21'—H21F109.5Sn6'—C44'—H44F109.5
H21D—C21'—H21F109.5H44D—C44'—H44F109.5
H21E—C21'—H21F109.5H44E—C44'—H44F109.5
Sn3'—C22'—H22D109.5Sn6'—C45'—H45D109.5
Sn3'—C22'—H22E109.5Sn6'—C45'—H45E109.5
H22D—C22'—H22E109.5H45D—C45'—H45E109.5
Sn3'—C22'—H22F109.5Sn6'—C45'—H45F109.5
H22D—C22'—H22F109.5H45D—C45'—H45F109.5
H22E—C22'—H22F109.5H45E—C45'—H45F109.5
Sn3'—C23'—H23D109.5Sn6'—C46'—H46D109.5
Sn3'—C23'—H23E109.5Sn6'—C46'—H46E109.5
H23D—C23'—H23E109.5H46D—C46'—H46E109.5
Sn3'—C23'—H23F109.5Sn6'—C46'—H46F109.5
H23D—C23'—H23F109.5H46D—C46'—H46F109.5
H23E—C23'—H23F109.5H46E—C46'—H46F109.5
C11—C1—C2—C37.7 (7)C34—C24—C25—C269.7 (7)
Co1—C1—C2—C3−52.9 (4)Co2—C24—C25—C26−52.0 (4)
C11—C1—C2—Co160.6 (4)C34—C24—C25—Co261.7 (4)
C1—C2—C3—C4−0.2 (7)C24—C25—C26—C27−2.5 (7)
Co1—C2—C3—C4−53.4 (4)Co2—C25—C26—C27−54.4 (4)
C1—C2—C3—Co153.2 (4)C24—C25—C26—Co251.8 (4)
C2—C3—C4—C12−6.4 (8)C25—C26—C27—C35−6.2 (7)
Co1—C3—C4—C12−59.0 (4)Co2—C26—C27—C35−59.6 (4)
C2—C3—C4—Co152.6 (4)C25—C26—C27—Co253.5 (4)
C13—C5—C6—C7−0.8 (11)C36—C28—C29—C300.0 (10)
C5—C6—C7—C80.5 (10)C28—C29—C30—C31−2.0 (10)
C6—C7—C8—C140.4 (8)C29—C30—C31—C370.5 (9)
C14—C9—C11—C1177.3 (4)C37—C32—C34—C352.0 (7)
C14—C9—C11—C12−1.0 (7)C37—C32—C34—C24−178.3 (4)
C14—C9—C11—Co191.4 (6)C37—C32—C34—Co296.2 (6)
C2—C1—C11—C9173.3 (4)C25—C24—C34—C32172.2 (4)
Co1—C1—C11—C9−129.3 (4)Co2—C24—C34—C32−129.2 (4)
C2—C1—C11—C12−8.4 (7)C25—C24—C34—C35−8.1 (7)
Co1—C1—C11—C1249.0 (4)Co2—C24—C34—C3550.4 (4)
C2—C1—C11—Co1−57.4 (4)C25—C24—C34—Co2−58.6 (4)
C13—C10—C12—C4−179.4 (5)C36—C33—C35—C340.6 (8)
C13—C10—C12—C110.6 (8)C36—C33—C35—C27178.9 (5)
C13—C10—C12—Co1−91.6 (7)C36—C33—C35—Co2−92.0 (6)
C3—C4—C12—C10−174.6 (5)C32—C34—C35—C33−2.4 (7)
Co1—C4—C12—C10129.7 (5)C24—C34—C35—C33177.9 (4)
C3—C4—C12—C115.5 (7)Co2—C34—C35—C33−135.4 (4)
Co1—C4—C12—C11−50.2 (4)C32—C34—C35—C27179.1 (4)
C3—C4—C12—Co155.6 (4)C24—C34—C35—C27−0.5 (6)
C9—C11—C12—C100.2 (7)Co2—C34—C35—C2746.1 (4)
C1—C11—C12—C10−178.2 (4)C32—C34—C35—Co2133.0 (4)
Co1—C11—C12—C10−132.3 (5)C24—C34—C35—Co2−46.7 (4)
C9—C11—C12—C4−179.9 (4)C26—C27—C35—C33−170.7 (5)
C1—C11—C12—C41.7 (6)Co2—C27—C35—C33133.2 (5)
Co1—C11—C12—C447.6 (4)C26—C27—C35—C347.6 (7)
C9—C11—C12—Co1132.5 (4)Co2—C27—C35—C34−48.5 (4)
C1—C11—C12—Co1−45.9 (4)C26—C27—C35—Co256.1 (4)
C12—C10—C13—C5178.5 (5)C35—C33—C36—C28−174.8 (5)
C12—C10—C13—C14−0.5 (8)C35—C33—C36—C371.7 (8)
C6—C5—C13—C10−178.9 (6)C29—C28—C36—C33179.8 (6)
C6—C5—C13—C140.2 (9)C29—C28—C36—C373.3 (8)
C11—C9—C14—C8−179.0 (4)C34—C32—C37—C31179.4 (5)
C11—C9—C14—C131.0 (7)C34—C32—C37—C360.2 (7)
C7—C8—C14—C9179.1 (5)C30—C31—C37—C32−176.3 (5)
C7—C8—C14—C13−1.0 (7)C30—C31—C37—C362.9 (8)
C10—C13—C14—C9−0.3 (7)C33—C36—C37—C32−2.1 (7)
C5—C13—C14—C9−179.4 (5)C28—C36—C37—C32174.5 (5)
C10—C13—C14—C8179.8 (5)C33—C36—C37—C31178.7 (5)
C5—C13—C14—C80.7 (7)C28—C36—C37—C31−4.7 (7)
  8 in total

1.  Oxidative addition of dihydrogen to (eta6-arene)Mo(PMe3)3 complexes: origin of the naphthalene and anthracene effects.

Authors:  Guang Zhu; Kevin E Janak; Joshua S Figueroa; Gerard Parkin
Journal:  J Am Chem Soc       Date:  2006-04-26       Impact factor: 15.419

2.  Towards homoleptic naphthalenemetalates of the later transition metals: isolation and characterization of naphthalenecobaltates(1-).

Authors:  William W Brennessel; Victor G Young; John E Ellis
Journal:  Angew Chem Int Ed Engl       Date:  2006-11-06       Impact factor: 15.336

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

4.  The Cambridge Structural Database in retrospect and prospect.

Authors:  Colin R Groom; Frank H Allen
Journal:  Angew Chem Int Ed Engl       Date:  2014-01-02       Impact factor: 15.336

5.  Unraveling the electronic structures of low-valent naphthalene and anthracene iron complexes: X-ray, spectroscopic, and density functional theory studies.

Authors:  Eva-Maria Schnöckelborg; Marat M Khusniyarov; Bas de Bruin; František Hartl; Thorsten Langer; Matthias Eul; Stephen Schulz; Rainer Pöttgen; Robert Wolf
Journal:  Inorg Chem       Date:  2012-05-25       Impact factor: 5.165

6.  Naphthalene and anthracene complexes sandwiched by two {(Cp*)Fe(I)} fragments: strong electronic coupling between the Fe(I) centers.

Authors:  Tsubasa Hatanaka; Yasuhiro Ohki; Takashi Kamachi; Tomonori Nakayama; Kazunari Yoshizawa; Motomi Katada; Kazuyuki Tatsumi
Journal:  Chem Asian J       Date:  2012-04-12

7.  Bis(1,2,3,4-eta4-anthracene)ferrate(1-): a paramagnetic homoleptic polyarene transition-metal anion.

Authors:  William W Brennessel; Robert E Jilek; John E Ellis
Journal:  Angew Chem Int Ed Engl       Date:  2007       Impact factor: 15.336

8.  Tris(eta4-naphthalene)- and tris(1-4-eta4-anthracene)tantalate(1-): first homoleptic arene complexes of anionic tantalum.

Authors:  William W Brennessel; John E Ellis; Marie K Pomije; Victor J Sussman; Eugenijus Urnezius; Victor G Young
Journal:  J Am Chem Soc       Date:  2002-09-04       Impact factor: 15.419

  8 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.