# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2011 data_global _journal_name_full Chem.Commun. _journal_coden_cambridge 0182 _journal_year ? _journal_volume ? _journal_page_first ? _publ_contact_author_email yongchen@hkucc.hku.hk _publ_author_name 'Chi-Ming Che' data_cheny31 _database_code_depnum_ccdc_archive 'CCDC 817890' #TrackingRef 'cheny31.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C22 H22 Cl2 N4 O3 Pt' _chemical_formula_weight 656.43 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' H H 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' N N 0.0311 0.0180 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0492 0.0322 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Cl Cl 0.3639 0.7018 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Pt Pt -4.5932 6.9264 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting ? _symmetry_space_group_name_H-M ? loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-x, y+1/2, -z' 'x+1/2, -y+1/2, -z+1/2' '-x, -y, -z' 'x-1/2, y, -z-1/2' 'x, -y-1/2, z' '-x-1/2, y-1/2, z-1/2' _cell_length_a 6.7618(2) _cell_length_b 24.1817(7) _cell_length_c 13.4445(4) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 2198.33(11) _cell_formula_units_Z 4 _cell_measurement_temperature 100(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description ? _exptl_crystal_colour ? _exptl_crystal_size_max ? _exptl_crystal_size_mid ? _exptl_crystal_size_min ? _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.983 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1272 _exptl_absorpt_coefficient_mu 14.461 _exptl_absorpt_correction_type ? _exptl_absorpt_correction_T_min ? _exptl_absorpt_correction_T_max ? _exptl_absorpt_process_details ? _exptl_special_details ; ? ; _diffrn_ambient_temperature 100(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type ? _diffrn_measurement_method ? _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 10564 _diffrn_reflns_av_R_equivalents 0.0516 _diffrn_reflns_av_sigmaI/netI 0.0446 _diffrn_reflns_limit_h_min -7 _diffrn_reflns_limit_h_max 6 _diffrn_reflns_limit_k_min -27 _diffrn_reflns_limit_k_max 27 _diffrn_reflns_limit_l_min -14 _diffrn_reflns_limit_l_max 15 _diffrn_reflns_theta_min 3.66 _diffrn_reflns_theta_max 65.40 _reflns_number_total 1872 _reflns_number_gt 1606 _reflns_threshold_expression >2sigma(I) _computing_data_collection ? _computing_cell_refinement ? _computing_data_reduction ? _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics ? _computing_publication_material ? _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^)+(0.0301P)^2^+18.8103P] 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 mixed _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 1872 _refine_ls_number_parameters 155 _refine_ls_number_restraints 3 _refine_ls_R_factor_all 0.0517 _refine_ls_R_factor_gt 0.0421 _refine_ls_wR_factor_ref 0.0968 _refine_ls_wR_factor_gt 0.0939 _refine_ls_goodness_of_fit_ref 1.191 _refine_ls_restrained_S_all 1.190 _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_symmetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group Pt1 Pt 0.07305(8) 0.2500 -0.71170(3) 0.01577(17) Uani 1 2 d S . . O1 O 0.0643(9) 0.3089(2) -0.6017(4) 0.0200(13) Uani 1 1 d . . . N1 N 0.1344(10) 0.3609(2) -0.7988(5) 0.0173(15) Uani 1 1 d . . . N2 N 0.0764(11) 0.2998(2) -0.9110(4) 0.0156(14) Uani 1 1 d . . . C1 C 0.1193(12) 0.3619(3) -0.6136(6) 0.0188(19) Uani 1 1 d . . . C2 C 0.1360(13) 0.3941(3) -0.5277(6) 0.0202(19) Uani 1 1 d . . . H2A H 0.1096 0.3774 -0.4651 0.024 Uiso 1 1 calc R . . C3 C 0.1890(14) 0.4489(3) -0.5301(6) 0.027(2) Uani 1 1 d . . . H3A H 0.1955 0.4692 -0.4698 0.033 Uiso 1 1 calc R . . C4 C 0.2329(14) 0.4748(3) -0.6189(6) 0.025(2) Uani 1 1 d . . . C5 C 0.2190(13) 0.4439(3) -0.7032(6) 0.0221(19) Uani 1 1 d . . . H5A H 0.2512 0.4611 -0.7647 0.027 Uiso 1 1 calc R . . C6 C 0.1600(12) 0.3884(3) -0.7049(6) 0.0185(17) Uani 1 1 d . . . C7 C 0.3040(16) 0.5342(3) -0.6236(7) 0.036(2) Uani 1 1 d . . . H7A H 0.3389 0.5435 -0.6923 0.054 Uiso 1 1 calc R . . H7B H 0.4205 0.5386 -0.5809 0.054 Uiso 1 1 calc R . . H7C H 0.1987 0.5589 -0.6005 0.054 Uiso 1 1 calc R . . C8 C 0.1443(14) 0.3866(3) -0.8908(6) 0.024(2) Uani 1 1 d . . . H8A H 0.1719 0.4246 -0.9022 0.029 Uiso 1 1 calc R . . C9 C 0.1083(13) 0.3488(3) -0.9606(6) 0.020(2) Uani 1 1 d . . . H9A H 0.1053 0.3545 -1.0305 0.024 Uiso 1 1 calc R . . C10 C 0.0934(13) 0.3072(3) -0.8115(6) 0.0216(19) Uani 1 1 d . . . C11 C -0.004(2) 0.2500 -0.9591(8) 0.024(3) Uani 1 2 d S . . H11A H -0.1497 0.2500 -0.9539 0.029 Uiso 1 2 calc SR . . H11B H 0.0321 0.2500 -1.0305 0.029 Uiso 1 2 calc SR . . O1W O -0.0675(13) 0.2500 -0.4413(3) 0.031(2) Uani 1 2 d SD . . H1WA H -0.0285 0.2764 -0.4796 0.047 Uiso 1 1 d D . . Cl1 Cl -0.0582(7) 0.33439(12) -0.22405(19) 0.0803(12) Uani 1 1 d . . . C1S C 0.193(3) 0.29263(6) -0.2571(6) 0.040(5) Uani 0.50 1 d PD . . H1SA H 0.1529 0.2730 -0.3158 0.049 Uiso 0.50 1 d PD . . H1SB H 0.2339 0.2692 -0.2033 0.049 Uiso 0.50 1 d PD . . 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 Pt1 0.0172(3) 0.0128(2) 0.0173(2) 0.000 0.0005(3) 0.000 O1 0.024(4) 0.016(2) 0.020(3) 0.000(2) -0.001(3) 0.002(3) N1 0.016(4) 0.012(3) 0.023(3) 0.000(3) 0.005(3) 0.001(3) N2 0.014(4) 0.013(3) 0.020(3) -0.001(2) -0.004(3) 0.000(3) C1 0.005(5) 0.020(4) 0.031(5) 0.001(3) 0.000(4) -0.001(3) C2 0.014(5) 0.024(4) 0.023(4) -0.005(3) -0.001(4) 0.008(4) C3 0.020(6) 0.028(4) 0.033(5) -0.015(4) 0.000(4) -0.001(4) C4 0.018(5) 0.016(4) 0.041(5) -0.004(3) 0.002(4) -0.003(4) C5 0.021(5) 0.017(4) 0.028(4) 0.002(3) -0.001(4) 0.000(4) C6 0.010(5) 0.017(4) 0.028(4) -0.004(3) -0.001(4) 0.007(3) C7 0.034(7) 0.022(4) 0.053(6) -0.013(4) 0.003(6) -0.007(4) C8 0.029(6) 0.015(4) 0.028(5) 0.007(3) 0.000(4) -0.003(4) C9 0.022(6) 0.019(4) 0.019(4) 0.006(3) 0.003(4) -0.005(4) C10 0.011(5) 0.023(4) 0.031(5) -0.009(3) -0.005(4) 0.007(4) C11 0.031(8) 0.028(6) 0.014(6) 0.000 -0.005(5) 0.000 O1W 0.033(6) 0.032(4) 0.029(4) 0.000 0.010(5) 0.000 Cl1 0.145(4) 0.0574(16) 0.0385(16) -0.0076(12) -0.016(2) -0.023(2) C1S 0.062(17) 0.037(9) 0.023(9) 0.002(8) -0.005(10) 0.004(11) _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 Pt1 C10 1.933(8) 7_565 ? Pt1 C10 1.933(8) . ? Pt1 O1 2.053(5) 7_565 ? Pt1 O1 2.053(5) . ? O1 C1 1.345(9) . ? N1 C10 1.339(10) . ? N1 C8 1.385(10) . ? N1 C6 1.436(10) . ? N2 C10 1.355(10) . ? N2 C9 1.376(9) . ? N2 C11 1.469(9) . ? C1 C2 1.398(11) . ? C1 C6 1.412(11) . ? C2 C3 1.372(11) . ? C3 C4 1.381(12) . ? C4 C5 1.361(11) . ? C4 C7 1.515(10) . ? C5 C6 1.402(10) . ? C8 C9 1.333(11) . ? C11 N2 1.469(9) 7_565 ? Cl1 C1S 1.98(2) 6 ? Cl1 C1S 2.03(2) . ? C1S Cl1 1.98(2) 6_655 ? 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 C10 Pt1 C10 91.5(4) 7_565 . ? C10 Pt1 O1 90.3(3) 7_565 7_565 ? C10 Pt1 O1 176.9(3) . 7_565 ? C10 Pt1 O1 176.9(3) 7_565 . ? C10 Pt1 O1 90.3(3) . . ? O1 Pt1 O1 87.8(3) 7_565 . ? C1 O1 Pt1 124.6(5) . . ? C10 N1 C8 109.3(7) . . ? C10 N1 C6 125.8(6) . . ? C8 N1 C6 124.9(6) . . ? C10 N2 C9 110.5(6) . . ? C10 N2 C11 125.1(7) . . ? C9 N2 C11 123.4(7) . . ? O1 C1 C2 117.1(7) . . ? O1 C1 C6 126.1(7) . . ? C2 C1 C6 116.8(7) . . ? C3 C2 C1 122.6(8) . . ? C2 C3 C4 121.1(8) . . ? C5 C4 C3 117.1(7) . . ? C5 C4 C7 120.5(8) . . ? C3 C4 C7 122.4(8) . . ? C4 C5 C6 124.0(8) . . ? C5 C6 C1 118.4(7) . . ? C5 C6 N1 119.4(7) . . ? C1 C6 N1 122.1(6) . . ? C9 C8 N1 108.2(7) . . ? C8 C9 N2 106.2(7) . . ? N1 C10 N2 105.8(7) . . ? N1 C10 Pt1 128.4(6) . . ? N2 C10 Pt1 125.7(6) . . ? N2 C11 N2 110.0(9) 7_565 . ? C1S Cl1 C1S 115.50(16) 6 . ? Cl1 C1S Cl1 119.13(16) 6_655 . ? _diffrn_measured_fraction_theta_max 0.968 _diffrn_reflns_theta_full 65.40 _diffrn_measured_fraction_theta_full 0.968 _refine_diff_density_max 1.364 _refine_diff_density_min -2.386 _refine_diff_density_rms 0.182