# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2012 data_global _journal_name_full Chem.Commun. _journal_coden_cambridge 0182 _journal_year ? _journal_volume ? _journal_page_first ? loop_ _publ_author_name 'Jinhee Park' 'Jian-Rong Li' 'Ying-Pin Chen' 'Linbing Sun' 'Hong-Cai Zhou' _publ_contact_author_name 'Ying-Pin Chen' _publ_contact_author_email ying-pin.chen@mail.chem.tamu.edu data_cubici_sq _database_code_depnum_ccdc_archive 'CCDC 858820' #TrackingRef '- cubici_sq_final.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C23 H11 Cu2 N3 O11' _chemical_formula_sum 'C23 H11 Cu2 N3 O11' _chemical_formula_weight 632.43 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0033 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' 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 'I m -3 m' 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+1/2, y+1/2, z+1/2' '-x+1/2, -y+1/2, z+1/2' '-x+1/2, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z+1/2' 'z+1/2, x+1/2, y+1/2' 'z+1/2, -x+1/2, -y+1/2' '-z+1/2, -x+1/2, y+1/2' '-z+1/2, x+1/2, -y+1/2' 'y+1/2, z+1/2, x+1/2' '-y+1/2, z+1/2, -x+1/2' 'y+1/2, -z+1/2, -x+1/2' '-y+1/2, -z+1/2, x+1/2' 'y+1/2, x+1/2, -z+1/2' '-y+1/2, -x+1/2, -z+1/2' 'y+1/2, -x+1/2, z+1/2' '-y+1/2, x+1/2, z+1/2' 'x+1/2, z+1/2, -y+1/2' '-x+1/2, z+1/2, y+1/2' '-x+1/2, -z+1/2, -y+1/2' 'x+1/2, -z+1/2, y+1/2' 'z+1/2, y+1/2, -x+1/2' 'z+1/2, -y+1/2, x+1/2' '-z+1/2, y+1/2, x+1/2' '-z+1/2, -y+1/2, -x+1/2' '-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+1/2, -y+1/2, -z+1/2' 'x+1/2, y+1/2, -z+1/2' 'x+1/2, -y+1/2, z+1/2' '-x+1/2, y+1/2, z+1/2' '-z+1/2, -x+1/2, -y+1/2' '-z+1/2, x+1/2, y+1/2' 'z+1/2, x+1/2, -y+1/2' 'z+1/2, -x+1/2, y+1/2' '-y+1/2, -z+1/2, -x+1/2' 'y+1/2, -z+1/2, x+1/2' '-y+1/2, z+1/2, x+1/2' 'y+1/2, z+1/2, -x+1/2' '-y+1/2, -x+1/2, z+1/2' 'y+1/2, x+1/2, z+1/2' '-y+1/2, x+1/2, -z+1/2' 'y+1/2, -x+1/2, -z+1/2' '-x+1/2, -z+1/2, y+1/2' 'x+1/2, -z+1/2, -y+1/2' 'x+1/2, z+1/2, y+1/2' '-x+1/2, z+1/2, -y+1/2' '-z+1/2, -y+1/2, x+1/2' '-z+1/2, y+1/2, -x+1/2' 'z+1/2, -y+1/2, -x+1/2' 'z+1/2, y+1/2, x+1/2' _cell_length_a 30.585(12) _cell_length_b 30.585(12) _cell_length_c 30.585(12) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 28611(19) _cell_formula_units_Z 24 _cell_measurement_temperature 110(2) _cell_measurement_reflns_used 9919 _cell_measurement_theta_min 2.307 _cell_measurement_theta_max 21.644 _exptl_crystal_description block _exptl_crystal_colour blue _exptl_crystal_size_max 0.11 _exptl_crystal_size_mid 0.09 _exptl_crystal_size_min 0.07 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 0.881 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 7584 _exptl_absorpt_coefficient_mu 0.927 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.9049 _exptl_absorpt_correction_T_max 0.9380 _exptl_absorpt_process_details 'SADABS (Sheldrick, 2008)' _exptl_special_details ; ? ; _diffrn_ambient_temperature 110(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 SMART APEX II CCD area detector' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 180466 _diffrn_reflns_av_R_equivalents 0.1305 _diffrn_reflns_av_sigmaI/netI 0.0325 _diffrn_reflns_limit_h_min -40 _diffrn_reflns_limit_h_max 41 _diffrn_reflns_limit_k_min -41 _diffrn_reflns_limit_k_max 40 _diffrn_reflns_limit_l_min -41 _diffrn_reflns_limit_l_max 41 _diffrn_reflns_theta_min 1.63 _diffrn_reflns_theta_max 28.70 _reflns_number_total 3484 _reflns_number_gt 2829 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'APEX2 (Bruker, 2008)' _computing_cell_refinement 'SAINT+ ver. (Bruker, 2001)' _computing_data_reduction 'SAINT+ ver. (Bruker, 2001)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'SHELXTL (Sheldrick, 2008)' _computing_publication_material 'SHELXTL (Sheldrick, 2008)' _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^)+(0.0520P)^2^+300.0000P] 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 constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 3484 _refine_ls_number_parameters 93 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.1186 _refine_ls_R_factor_gt 0.0914 _refine_ls_wR_factor_ref 0.2125 _refine_ls_wR_factor_gt 0.1966 _refine_ls_goodness_of_fit_ref 1.029 _refine_ls_restrained_S_all 1.029 _refine_ls_shift/su_max 0.001 _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 0.18402(2) 0.18402(2) 0.0000 0.0381(3) Uani 1 4 d S . . Cu2 Cu 0.5000 0.25497(2) 0.25497(2) 0.0404(3) Uani 1 4 d S . . O1 O 0.27236(12) 0.20895(12) 0.04484(13) 0.0604(10) Uani 1 1 d . . . O1S O 0.13450(19) 0.13450(19) 0.0000 0.116(4) Uani 1 4 d S . . O2 O 0.22016(11) 0.15729(11) 0.04498(12) 0.0560(9) Uani 1 1 d . . . O3 O 0.4146(3) 0.1642(4) 0.0813(3) 0.0924(16) Uani 0.50 1 d P . . N1 N 0.5000 0.2055(3) 0.2055(3) 0.0924(16) Uani 1 4 d SD . . N2 N 0.3859(2) 0.15190(19) 0.15190(19) 0.0924(16) Uani 1 2 d S . . H2A H 0.3926 0.1520 0.1805 0.111 Uiso 0.50 1 d PR . . C1 C 0.25534(17) 0.17408(17) 0.05872(15) 0.0487(11) Uani 1 1 d . . . C2 C 0.2580(2) 0.11520(16) 0.11520(16) 0.0447(15) Uani 1 2 d S . . H2B H 0.2297 0.1056 0.1056 0.054 Uiso 1 2 d SR . . C3 C 0.27847(16) 0.14981(18) 0.09450(17) 0.0524(12) Uani 1 1 d . . . C4 C 0.3206(2) 0.1621(2) 0.1063(2) 0.0723(17) Uani 1 1 d . . . H4A H 0.3345 0.1863 0.0921 0.087 Uiso 1 1 d R . . C5 C 0.3415(3) 0.1394(2) 0.1394(2) 0.077(3) Uani 1 2 d S . . C6 C 0.4180(4) 0.1629(6) 0.1221(4) 0.0924(16) Uani 0.50 1 d P . . C7 C 0.4631(3) 0.1965(5) 0.1844(4) 0.0924(16) Uani 0.50 1 d PD . . H7A H 0.4361 0.2027 0.2027 0.111 Uiso 1 2 d SR . . C8 C 0.4614(4) 0.1758(5) 0.1435(4) 0.0924(16) Uani 0.50 1 d PD . . C9 C 0.5000 0.1636(8) 0.1238(6) 0.0924(16) Uani 0.50 2 d SPD . . H9A H 0.5000 0.1508 0.0951 0.111 Uiso 0.50 2 d SPR . . 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 0.0361(4) 0.0361(4) 0.0421(6) 0.000 0.000 -0.0115(4) Cu2 0.0423(6) 0.0394(4) 0.0394(4) -0.0139(5) 0.000 0.000 O1 0.057(2) 0.055(2) 0.069(2) 0.0193(18) -0.0112(18) -0.0217(17) O1S 0.080(5) 0.080(5) 0.187(12) 0.000 0.000 -0.054(6) O2 0.055(2) 0.051(2) 0.062(2) 0.0164(17) -0.0152(17) -0.0175(17) O3 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) N1 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) N2 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) C1 0.051(3) 0.053(3) 0.042(2) 0.007(2) -0.002(2) -0.004(2) C2 0.041(3) 0.047(2) 0.047(2) 0.002(3) -0.006(2) -0.006(2) C3 0.044(3) 0.060(3) 0.053(3) 0.012(2) -0.009(2) -0.009(2) C4 0.061(3) 0.072(4) 0.083(4) 0.023(3) -0.022(3) -0.019(3) C5 0.058(5) 0.087(4) 0.087(4) 0.018(5) -0.022(4) -0.022(4) C6 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) C7 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) C8 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) C9 0.049(2) 0.159(5) 0.070(3) -0.032(3) -0.011(2) -0.010(3) _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 O2 1.945(3) 62 ? Cu1 O2 1.945(3) 13 ? Cu1 O2 1.945(3) 50 ? Cu1 O2 1.945(3) . ? Cu1 O1S 2.142(8) . ? Cu1 Cu2 2.6391(17) 81 ? Cu2 O1 1.949(4) 95 ? Cu2 O1 1.949(4) 30 ? Cu2 O1 1.949(4) 77 ? Cu2 O1 1.949(4) 48 ? Cu2 N1 2.139(12) . ? Cu2 Cu1 2.6390(17) 77 ? O1 C1 1.261(6) . ? O1 Cu2 1.949(4) 81 ? O2 C1 1.264(6) . ? O3 C6 1.253(15) . ? N1 C7 1.328(11) 67 ? N1 C7 1.328(11) 52_655 ? N1 C7 1.328(11) 18_655 ? N1 C7 1.328(11) . ? N2 C6 1.381(14) 67 ? N2 C6 1.381(14) . ? N2 C5 1.461(10) . ? N2 H2A 0.8975 . ? C1 C3 1.500(7) . ? C2 C3 1.383(6) 67 ? C2 C3 1.383(6) . ? C2 H2B 0.9600 . ? C3 C4 1.389(7) . ? C4 C5 1.383(7) . ? C4 H4A 0.9600 . ? C5 C4 1.383(7) 67 ? C6 C8 1.530(16) . ? C6 C6 1.76(3) 67 ? C7 C7 0.52(4) 67 ? C7 C8 1.407(16) . ? C7 C8 1.646(19) 67 ? C7 H7A 1.0148 . ? C8 C9 1.376(16) . ? C8 C8 1.40(3) 67 ? C8 C7 1.646(19) 67 ? C9 C8 1.377(16) 52_655 ? C9 C9 1.72(4) 18_655 ? C9 H9A 0.9600 . ? 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 O2 Cu1 O2 90.0(2) 62 13 ? O2 Cu1 O2 168.0(2) 62 50 ? O2 Cu1 O2 88.7(2) 13 50 ? O2 Cu1 O2 88.7(2) 62 . ? O2 Cu1 O2 168.0(2) 13 . ? O2 Cu1 O2 90.0(2) 50 . ? O2 Cu1 O1S 96.00(10) 62 . ? O2 Cu1 O1S 96.00(10) 13 . ? O2 Cu1 O1S 96.00(10) 50 . ? O2 Cu1 O1S 96.01(10) . . ? O2 Cu1 Cu2 84.00(10) 62 81 ? O2 Cu1 Cu2 84.00(10) 13 81 ? O2 Cu1 Cu2 84.00(10) 50 81 ? O2 Cu1 Cu2 83.99(10) . 81 ? O1S Cu1 Cu2 180.0(2) . 81 ? O1 Cu2 O1 89.5(2) 95 30 ? O1 Cu2 O1 168.9(2) 95 77 ? O1 Cu2 O1 89.5(2) 30 77 ? O1 Cu2 O1 89.5(2) 95 48 ? O1 Cu2 O1 168.9(2) 30 48 ? O1 Cu2 O1 89.5(2) 77 48 ? O1 Cu2 N1 95.57(10) 95 . ? O1 Cu2 N1 95.57(10) 30 . ? O1 Cu2 N1 95.57(10) 77 . ? O1 Cu2 N1 95.57(10) 48 . ? O1 Cu2 Cu1 84.43(10) 95 77 ? O1 Cu2 Cu1 84.43(10) 30 77 ? O1 Cu2 Cu1 84.43(10) 77 77 ? O1 Cu2 Cu1 84.43(10) 48 77 ? N1 Cu2 Cu1 180.0(3) . 77 ? C1 O1 Cu2 122.6(3) . 81 ? C1 O2 Cu1 123.2(3) . . ? C7 N1 C7 121.4(14) 67 52_655 ? C7 N1 C7 116.3(13) 67 18_655 ? C7 N1 C7 22.7(15) 52_655 18_655 ? C7 N1 C7 22.7(15) 67 . ? C7 N1 C7 116.3(13) 52_655 . ? C7 N1 C7 121.4(14) 18_655 . ? C7 N1 Cu2 119.3(7) 67 . ? C7 N1 Cu2 119.3(7) 52_655 . ? C7 N1 Cu2 119.3(7) 18_655 . ? C7 N1 Cu2 119.3(7) . . ? C6 N2 C6 79.4(14) 67 . ? C6 N2 C5 123.5(7) 67 . ? C6 N2 C5 123.5(7) . . ? C6 N2 H2A 66.5 67 . ? C6 N2 H2A 118.5 . . ? C5 N2 H2A 117.9 . . ? O1 C1 O2 125.7(4) . . ? O1 C1 C3 118.0(4) . . ? O2 C1 C3 116.3(4) . . ? C3 C2 C3 119.7(6) 67 . ? C3 C2 H2B 120.2 67 . ? C3 C2 H2B 120.2 . . ? C2 C3 C4 120.5(5) . . ? C2 C3 C1 119.9(4) . . ? C4 C3 C1 119.6(5) . . ? C5 C4 C3 118.9(6) . . ? C5 C4 H4A 120.9 . . ? C3 C4 H4A 120.2 . . ? C4 C5 C4 121.3(8) 67 . ? C4 C5 N2 119.3(4) 67 . ? C4 C5 N2 119.3(4) . . ? O3 C6 N2 127.2(11) . . ? O3 C6 C8 119.2(12) . . ? N2 C6 C8 113.5(11) . . ? O3 C6 C6 136.6(10) . 67 ? N2 C6 C6 50.3(7) . 67 ? C8 C6 C6 83.1(8) . 67 ? C7 C7 N1 78.6(8) 67 . ? C7 C7 C8 108.1(8) 67 . ? N1 C7 C8 123.9(11) . . ? C7 C7 C8 54.3(8) 67 67 ? N1 C7 C8 108.0(12) . 67 ? C8 C7 C8 53.8(11) . 67 ? C7 C7 H7A 75.1 67 . ? N1 C7 H7A 112.7 . . ? C8 C7 H7A 123.0 . . ? C8 C7 H7A 104.3 67 . ? C9 C8 C8 96.8(11) . 67 ? C9 C8 C7 118.6(12) . . ? C8 C8 C7 71.9(8) 67 . ? C9 C8 C6 119.3(13) . . ? C8 C8 C6 96.9(8) 67 . ? C7 C8 C6 121.9(11) . . ? C9 C8 C7 116.6(12) . 67 ? C8 C8 C7 54.3(8) 67 67 ? C7 C8 C7 17.6(12) . 67 ? C6 C8 C7 119.3(10) . 67 ? C8 C9 C8 118.2(18) . 52_655 ? C8 C9 C9 83.2(11) . 18_655 ? C8 C9 C9 83.2(11) 52_655 18_655 ? C8 C9 H9A 120.6 . . ? C8 C9 H9A 120.6 52_655 . ? C9 C9 H9A 110.9 18_655 . ? _diffrn_measured_fraction_theta_max 0.992 _diffrn_reflns_theta_full 28.70 _diffrn_measured_fraction_theta_full 0.992 _refine_diff_density_max 1.553 _refine_diff_density_min -0.813 _refine_diff_density_rms 0.098 # SQUEEZE RESULTS (APPEND TO CIF) # Note: Data are Listed for all Voids in the P1 Unit Cell # i.e. Centre of Gravity, Solvent Accessible Volume, # Recovered number of Electrons in the Void and # Details about the Squeezed Material loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.019 -0.039 -0.022 15960 3908 ' ' _platon_squeeze_details ; ; _publ_section_references ; Bruker (2001). SAINTP+ for NT. Data Reduction and Correction Program v. 6.2, Bruker AXS, Madison, Wisconsin, USA. Bruker (2005). APEX2 software package. Bruker Molecular Analysis Research Tool, v. 2008.4 Bruker AXS, Madison, Wisconsin, USA. Sheldrick G.M. (2008). SADABS-2008/1, Bruker/Siemens Area Detector Absorption Correction Program, Bruker AXS, Madison, Wisconsin, USA. Sheldrick G.M. (2008). SHELXTL 2008/4, Structure Determination Software Suite, Bruker AXS, Madison, Wisconsin, USA. ;