# Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2002 data_1 _database_code_CSD 192733 _audit_creation_method SHELXL-97 _journal_coden_Cambridge 182 loop_ _publ_author_name _publ_author_address 'Marciniec, Bogdan' ; Department of Chemistry Adam Mickiewicz University Grunwaldzka 6 60-780 Poznan Poland ; 'Kubicki, Maciej' ; Department of Chemistry Adam Mickiewicz University Grunwaldzka 6 60-780 Poznan Poland ; 'Kownacki, Ireneusz' ; Department of Chemistry Adam Mickiewicz University Grunwaldzka 6 60-780 Poznan Poland ; _publ_contact_author_name 'Dr Bogdan Marciniec' _publ_contact_author_address ; Faculty of Chemistry Adam Mickiewicz University 60-780 Poznan POLAND ; _publ_contact_author_email 'MARCINB@MAIN.AMU.EDU.PL' _publ_requested_journal 'Chemical Communications' _publ_section_title ; Alkoxy/ siloxy group exchange in the system vinyltrialkoxysilane - iridium(I)siloxide complex ; _chemical_name_systematic ; bis-(1,5-cyclooctadiene)-di-\m-(ethoxy)diirydium (I) ; _chemical_formula_sum 'C20 H34 Ir2 O2' _chemical_formula_weight 690.87 _symmetry_cell_setting monoclinic _symmetry_space_group_name_H-M 'P2/n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, y, -z+1/2' '-x, -y, -z' 'x-1/2, -y, z-1/2' _cell_length_a 12.5233(9) _cell_length_b 6.4252(4) _cell_length_c 12.5949(9) _cell_angle_alpha 90.00 _cell_angle_beta 93.558(6) _cell_angle_gamma 90.00 _cell_volume 1011.49(12) _cell_formula_units_Z 2 _exptl_crystal_density_diffrn 2.268 _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _cell_measurement_reflns_used 650 _cell_measurement_theta_min 4 _cell_measurement_theta_max 17 _diffrn_ambient_temperature 293(2) _exptl_crystal_F_000 648 _exptl_absorpt_coefficient_mu 13.152 _exptl_crystal_description block _exptl_crystal_size_max 0.3 _exptl_crystal_size_mid 0.2 _exptl_crystal_size_min 0.2 _exptl_crystal_colour colourless _diffrn_measurement_device_type ; four-circle diffractometer with CCD detector ; _diffrn_measurement_method \w-scan _exptl_absorpt_correction_type 'psi-scan' _exptl_absorpt_correction_T_min 0.14 _exptl_absorpt_correction_T_max 0.20 _exptl_absorpt_process_details ? _diffrn_radiation_monochromator graphite _diffrn_reflns_number 7276 _reflns_number_total 1758 _diffrn_reflns_theta_max 25.00 _diffrn_reflns_av_R_equivalents 0.080 _diffrn_reflns_limit_h_min -14 _diffrn_reflns_limit_h_max 14 _diffrn_reflns_limit_k_min -7 _diffrn_reflns_limit_k_max 7 _diffrn_reflns_limit_l_min -14 _diffrn_reflns_limit_l_max 14 _computing_data_collection 'CrysAlisCCD (Oxford Diffraction, 2001)' _computing_cell_refinement 'CrysAlisCCD (Oxford Diffraction, 2000)' _computing_data_reduction 'CrysAlisRed (Oxford Diffraction, 2000)' _computing_structure_solution ; SHELXS-97 (G.M. Sheldrick, Acta Cryst A46 (1990), 467) ; _computing_structure_refinement ; SHELXL-97 (Program for the Refinement of Crystal Structures. University of Göttingen, Germany (1997)) ; _refine_special_details ; Refinement of F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > 2sigma(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. ; _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_weighting_scheme calc _refine_ls_weighting_details 'calc w==1/[\s^2^(Fo^2^)+(0.0300P)^2^+30.0000P] where P==(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens geom _refine_ls_hydrogen_treatment riding _refine_ls_extinction_method none _refine_ls_number_reflns 1758 _refine_ls_number_parameters 109 _refine_ls_number_restraints 24 _refine_ls_R_factor_all 0.0580 _refine_ls_R_factor_gt 0.0555 _refine_ls_wR_factor_ref 0.1319 _refine_ls_wR_factor_gt 0.1303 _refine_ls_goodness_of_fit_ref 1.132 _refine_ls_restrained_S_all 1.131 _refine_ls_shift/su_max 0.000 _refine_ls_shift/su_mean 0.000 loop_ _atom_site_label _atom_site_type_symbol _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_U_iso_or_equiv _atom_site_adp_type _atom_site_occupancy _atom_site_symetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group Ir1 Ir 0.25515(4) 0.88456(8) 0.13547(4) 0.0324(2) Uani 1 1 d . . . O1 O 0.1491(7) 0.7615(15) 0.2390(8) 0.036(2) Uani 1 1 d . . . C11 C 0.0338(12) 0.761(3) 0.2250(16) 0.054(4) Uani 1 1 d . . . H11A H 0.0117 0.8071 0.1537 0.064 Uiso 1 1 d R . . H11B H 0.0042 0.8559 0.2752 0.064 Uiso 1 1 d R . . C12 C -0.008(2) 0.550(4) 0.244(2) 0.086(7) Uani 1 1 d U . . H12A H -0.0846 0.5506 0.2337 0.104 Uiso 1 1 d R . . H12B H 0.0121 0.5060 0.3156 0.104 Uiso 1 1 d R . . H12C H 0.0215 0.4559 0.1947 0.104 Uiso 1 1 d R . . C1 C 0.3659(13) 1.091(2) 0.0783(15) 0.051(4) Uani 1 1 d . . . H1 H 0.3921 1.0967 0.1490 0.061 Uiso 1 1 d R . . C2 C 0.3721(13) 0.906(3) 0.0234(13) 0.046(4) Uani 1 1 d . . . H2 H 0.4074 0.7961 0.0582 0.055 Uiso 1 1 d R . . C3 C 0.3266(19) 0.871(4) -0.0874(19) 0.081(6) Uani 1 1 d U . . H3A H 0.3584 0.9711 -0.1337 0.098 Uiso 1 1 d R . . H3B H 0.3478 0.7335 -0.1099 0.098 Uiso 1 1 d R . . C4 C 0.2144(17) 0.885(4) -0.1040(13) 0.068(6) Uani 1 1 d . . . H4A H 0.1886 0.7635 -0.1434 0.081 Uiso 1 1 d R . . H4B H 0.1978 1.0059 -0.1481 0.081 Uiso 1 1 d R . . C5 C 0.1507(11) 0.906(3) 0.0000(12) 0.046(4) Uani 1 1 d . . . H5 H 0.1147 0.7900 0.0240 0.055 Uiso 1 1 d R . . C6 C 0.1477(14) 1.091(3) 0.0553(16) 0.056(4) Uani 1 1 d . . . H6 H 0.1081 1.0924 0.1153 0.067 Uiso 1 1 d R . . C7 C 0.2011(17) 1.291(4) 0.028(2) 0.077(6) Uani 1 1 d U . . H7A H 0.1721 1.3331 -0.0414 0.093 Uiso 1 1 d R . . H7B H 0.1816 1.3969 0.0784 0.093 Uiso 1 1 d R . . C8 C 0.3174(16) 1.289(3) 0.0263(19) 0.069(5) Uani 1 1 d U . . H8A H 0.3461 1.4106 0.0639 0.083 Uiso 1 1 d R . . H8B H 0.3373 1.2978 -0.0468 0.083 Uiso 1 1 d R . . loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_23 _atom_site_aniso_U_13 _atom_site_aniso_U_12 Ir1 0.0282(3) 0.0321(3) 0.0363(4) -0.0011(2) -0.0019(2) -0.0007(2) O1 0.031(5) 0.041(5) 0.035(5) 0.003(4) -0.007(4) 0.002(4) C11 0.028(7) 0.062(10) 0.070(12) -0.003(9) -0.005(8) -0.005(7) C12 0.078(10) 0.081(9) 0.099(10) 0.004(8) 0.000(8) -0.015(8) C1 0.039(8) 0.046(9) 0.066(11) 0.012(8) -0.004(8) -0.002(7) C2 0.042(8) 0.054(9) 0.044(9) 0.009(7) 0.011(7) 0.005(7) C3 0.077(9) 0.091(10) 0.077(9) 0.004(8) 0.008(8) 0.007(8) C4 0.084(14) 0.096(15) 0.024(8) -0.016(9) 0.005(8) -0.009(12) C5 0.021(6) 0.078(11) 0.039(8) 0.006(8) 0.002(6) 0.002(7) C6 0.049(10) 0.052(10) 0.065(12) 0.011(9) -0.008(8) 0.009(8) C7 0.072(9) 0.069(9) 0.092(10) 0.029(8) 0.007(8) -0.001(7) C8 0.064(8) 0.062(8) 0.082(9) 0.013(7) 0.004(7) 0.005(7) _geom_special_details ; 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. ; loop_ _geom_bond_atom_site_label_1 _geom_bond_atom_site_label_2 _geom_bond_distance _geom_bond_site_symmetry_2 _geom_bond_publ_flag Ir1 O1 2.075(10) . ? Ir1 O1 2.080(9) 2 ? Ir1 Ir1 2.8958(11) 2 ? O1 C11 1.444(17) . ? O1 Ir1 2.080(9) 2 ? C11 C12 1.48(3) . ? C1 C2 1.37(2) . ? C1 C8 1.54(2) . ? C2 C3 1.49(3) . ? C3 C4 1.41(3) . ? C4 C5 1.58(2) . ? C5 C6 1.38(2) . ? C6 C7 1.50(3) . ? C7 C8 1.46(3) . ? loop_ _geom_angle_atom_site_label_1 _geom_angle_atom_site_label_2 _geom_angle_atom_site_label_3 _geom_angle _geom_angle_site_symmetry_1 _geom_angle_site_symmetry_3 _geom_angle_publ_flag O1 Ir1 O1 74.9(4) . 2 ? O1 Ir1 Ir1 45.9(3) . 2 ? O1 Ir1 Ir1 45.7(3) 2 2 ? C11 O1 Ir1 126.8(10) . . ? C11 O1 Ir1 128.3(10) . 2 ? Ir1 O1 Ir1 88.4(4) . 2 ? O1 C11 C12 110.2(16) . . ? C2 C1 C8 122.1(17) . . ? C1 C2 C3 124.8(17) . . ? C4 C3 C2 116.6(18) . . ? C3 C4 C5 115.6(15) . . ? C6 C5 C4 121.5(16) . . ? C5 C6 C7 126.8(19) . . ? C8 C7 C6 117.4(17) . . ? C7 C8 C1 111.4(16) . . ? loop_ _geom_torsion_atom_site_label_1 _geom_torsion_atom_site_label_2 _geom_torsion_atom_site_label_3 _geom_torsion_atom_site_label_4 _geom_torsion _geom_torsion_site_symmetry_1 _geom_torsion_site_symmetry_2 _geom_torsion_site_symmetry_3 _geom_torsion_site_symmetry_4 _geom_torsion_publ_flag O1 Ir1 O1 C11 -179.3(11) 2 . . . ? Ir1 Ir1 O1 C11 138.8(13) 2 . . . ? O1 Ir1 O1 Ir1 41.9(4) 2 . . 2 ? Ir1 O1 C11 C12 131.0(15) . . . . ? Ir1 O1 C11 C12 -106.0(17) 2 . . . ? C8 C1 C2 C3 -5(3) . . . . ? C1 C2 C3 C4 -64(3) . . . . ? C2 C3 C4 C5 -8(3) . . . . ? C3 C4 C5 C6 76(2) . . . . ? C4 C5 C6 C7 0(3) . . . . ? C5 C6 C7 C8 -61(3) . . . . ? C6 C7 C8 C1 -13(3) . . . . ? C2 C1 C8 C7 83(2) . . . . ? _diffrn_measured_fraction_theta_max 0.985 _diffrn_reflns_theta_full 25.00 _diffrn_measured_fraction_theta_full 0.985 _refine_diff_density_max 3.716 _refine_diff_density_min -2.199 _refine_diff_density_rms 0.299