# 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_name 'Jian Zhang' _publ_contact_author_email zhj@fjirsm.ac.cn loop_ _publ_author_name 'Jian Zhang' 'Yan-Xi Tan' 'Yan-Ping He' data_a _database_code_depnum_ccdc_archive 'CCDC 833721' #TrackingRef '- A.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C24 H8 Cl Cu4 O16' _chemical_formula_weight 841.95 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0033 0.0016 '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 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Cl Cl 0.1484 0.1585 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Cu Cu 0.3201 1.2651 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M Pm-3m loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' '-x, y, -z' 'x, -y, -z' 'z, x, y' 'z, -x, -y' '-z, -x, y' '-z, x, -y' 'y, z, x' '-y, z, -x' 'y, -z, -x' '-y, -z, x' 'y, x, -z' '-y, -x, -z' 'y, -x, z' '-y, x, z' 'x, z, -y' '-x, z, y' '-x, -z, -y' 'x, -z, y' 'z, y, -x' 'z, -y, x' '-z, y, x' '-z, -y, -x' '-x, -y, -z' 'x, y, -z' 'x, -y, z' '-x, y, z' '-z, -x, -y' '-z, x, y' 'z, x, -y' 'z, -x, y' '-y, -z, -x' 'y, -z, x' '-y, z, x' 'y, z, -x' '-y, -x, z' 'y, x, z' '-y, x, -z' 'y, -x, -z' '-x, -z, y' 'x, -z, -y' 'x, z, y' '-x, z, -y' '-z, -y, x' '-z, y, -x' 'z, -y, -x' 'z, y, x' _cell_length_a 15.3840(11) _cell_length_b 15.3840(11) _cell_length_c 15.3840(11) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 3640.9(5) _cell_formula_units_Z 3 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 827 _cell_measurement_theta_min 3.18 _cell_measurement_theta_max 27.440 _exptl_crystal_description block _exptl_crystal_colour blue _exptl_crystal_size_max .25 _exptl_crystal_size_mid .18 _exptl_crystal_size_min .15 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.152 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1239.0 _exptl_absorpt_coefficient_mu 1.859 _exptl_absorpt_correction_type none _exptl_absorpt_correction_T_min ? _exptl_absorpt_correction_T_max ? _exptl_absorpt_process_details none _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker P4' _diffrn_measurement_method '\w scans' _diffrn_detector_area_resol_mean none _diffrn_standards_number none _diffrn_standards_interval_count none _diffrn_standards_interval_time none _diffrn_standards_decay_% none _diffrn_reflns_number 23178 _diffrn_reflns_av_R_equivalents 0.0631 _diffrn_reflns_av_sigmaI/netI 0.0313 _diffrn_reflns_limit_h_min -19 _diffrn_reflns_limit_h_max 15 _diffrn_reflns_limit_k_min -15 _diffrn_reflns_limit_k_max 19 _diffrn_reflns_limit_l_min -19 _diffrn_reflns_limit_l_max 15 _diffrn_reflns_theta_min 2.29 _diffrn_reflns_theta_max 27.44 _reflns_number_total 893 _reflns_number_gt 878 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker XSCANS' _computing_cell_refinement 'Bruker XSCANS' _computing_data_reduction 'Bruker SHELXTL' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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^)+(0.1708P)^2^+3.8263P] 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 none _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef none _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 893 _refine_ls_number_parameters 35 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0558 _refine_ls_R_factor_gt 0.0533 _refine_ls_wR_factor_ref 0.2307 _refine_ls_wR_factor_gt 0.2285 _refine_ls_goodness_of_fit_ref 1.154 _refine_ls_restrained_S_all 1.154 _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 Cu1 Cu 0.33601(6) 0.5000 0.0000 0.0163(5) Uani 1 4 d S . . Cl1 Cl 0.5000 0.5000 0.0000 0.0336(11) Uani 1 16 d S . . O1 O 0.3134(3) 0.4145(3) -0.0899(3) 0.0489(12) Uani 1 1 d . . . C1 C 0.3483(3) 0.3483(3) -0.1175(4) 0.0250(12) Uani 1 2 d S . . C2 C 0.3069(3) 0.3069(3) -0.1964(4) 0.0277(14) Uani 1 2 d S . . C3 C 0.3438(4) 0.2334(3) -0.2334(3) 0.0296(13) Uani 1 2 d S . . H3A H 0.3933 0.2089 -0.2089 0.036 Uiso 1 2 calc SR . . 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 Cu1 0.0226(6) 0.0138(6) 0.0124(6) 0.000 0.000 0.000 Cl1 0.0171(11) 0.0171(11) 0.066(3) 0.000 0.000 0.000 O1 0.046(2) 0.051(2) 0.051(2) -0.0355(19) -0.0253(17) 0.0218(17) C1 0.0272(17) 0.0272(17) 0.021(3) -0.0043(15) -0.0043(15) 0.001(2) C2 0.0287(19) 0.0287(19) 0.026(3) -0.0110(18) -0.0110(18) 0.010(2) C3 0.029(3) 0.0301(19) 0.0301(19) -0.010(3) -0.0111(18) 0.0111(18) _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 Cu1 O1 1.940(3) . ? Cu1 O1 1.940(3) 4_565 ? Cu1 O1 1.940(3) 27_565 ? Cu1 O1 1.940(3) 26 ? Cu1 Cl1 2.5228(9) . ? Cl1 Cu1 2.5228(9) 37_665 ? Cl1 Cu1 2.5228(9) 25_665 ? Cl1 Cu1 2.5228(9) 13 ? O1 C1 1.227(4) . ? C1 O1 1.227(4) 38 ? C1 C2 1.512(8) . ? C2 C3 1.387(4) . ? C2 C3 1.387(4) 8 ? C3 C2 1.387(4) 11 ? C3 H3A 0.9300 . ? 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 Cu1 O1 159.4(2) . 4_565 ? O1 Cu1 O1 85.4(3) . 27_565 ? O1 Cu1 O1 90.9(3) 4_565 27_565 ? O1 Cu1 O1 90.9(3) . 26 ? O1 Cu1 O1 85.4(3) 4_565 26 ? O1 Cu1 O1 159.4(2) 27_565 26 ? O1 Cu1 Cl1 100.32(12) . . ? O1 Cu1 Cl1 100.32(12) 4_565 . ? O1 Cu1 Cl1 100.32(12) 27_565 . ? O1 Cu1 Cl1 100.32(12) 26 . ? Cu1 Cl1 Cu1 90.0 37_665 25_665 ? Cu1 Cl1 Cu1 90.0 37_665 . ? Cu1 Cl1 Cu1 180.0 25_665 . ? Cu1 Cl1 Cu1 180.0 37_665 13 ? Cu1 Cl1 Cu1 90.0 25_665 13 ? Cu1 Cl1 Cu1 90.0 . 13 ? C1 O1 Cu1 137.0(4) . . ? O1 C1 O1 127.3(6) 38 . ? O1 C1 C2 116.3(3) 38 . ? O1 C1 C2 116.3(3) . . ? C3 C2 C3 120.0(6) . 8 ? C3 C2 C1 120.0(3) . . ? C3 C2 C1 120.0(3) 8 . ? C2 C3 C2 120.0(6) 11 . ? C2 C3 H3A 120.0 11 . ? C2 C3 H3A 120.0 . . ? _diffrn_measured_fraction_theta_max 0.984 _diffrn_reflns_theta_full 27.44 _diffrn_measured_fraction_theta_full 0.984 _refine_diff_density_max 1.986 _refine_diff_density_min -0.409 _refine_diff_density_rms 0.145