# 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 handong@fjirsm.ac.cn _publ_author_name 'Maochun Hong' data_1 _database_code_depnum_ccdc_archive 'CCDC 817980' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C46 H28 N2 O8 Zn2' _chemical_formula_weight 867.44 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' 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' Zn Zn 0.2839 1.4301 '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' _symmetry_cell_setting cubic _symmetry_space_group_name_H-M Pm-3n loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y+1/2, x+1/2, z+1/2' '-x, -y, z' 'y+1/2, -x+1/2, z+1/2' 'x+1/2, -z+1/2, y+1/2' 'x, -y, -z' 'x+1/2, z+1/2, -y+1/2' 'z+1/2, y+1/2, -x+1/2' '-x, y, -z' '-z+1/2, y+1/2, x+1/2' 'z, x, y' 'y, z, x' '-y, -z, x' 'z, -x, -y' '-y, z, -x' '-z, -x, y' '-z, x, -y' 'y, -z, -x' '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' 'z+1/2, -y+1/2, x+1/2' '-z+1/2, -y+1/2, -x+1/2' '-x, -y, -z' 'y-1/2, -x-1/2, -z-1/2' 'x, y, -z' '-y-1/2, x-1/2, -z-1/2' '-x-1/2, z-1/2, -y-1/2' '-x, y, z' '-x-1/2, -z-1/2, y-1/2' '-z-1/2, -y-1/2, x-1/2' 'x, -y, z' 'z-1/2, -y-1/2, -x-1/2' '-z, -x, -y' '-y, -z, -x' 'y, z, -x' '-z, x, y' 'y, -z, x' 'z, x, -y' 'z, -x, y' '-y, z, x' '-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' '-z-1/2, y-1/2, -x-1/2' 'z-1/2, y-1/2, x-1/2' _cell_length_a 27.7364(11) _cell_length_b 27.7364(11) _cell_length_c 27.7364(11) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 21337.8(15) _cell_formula_units_Z 6 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 37135 _cell_measurement_theta_min 2.0772 _cell_measurement_theta_max 27.4797 _exptl_crystal_description Prism _exptl_crystal_colour Colorless _exptl_crystal_size_max 0.2 _exptl_crystal_size_mid 0.2 _exptl_crystal_size_min 0.2 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 0.405 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2652 _exptl_absorpt_coefficient_mu 0.353 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.5896 _exptl_absorpt_correction_T_max 1.0000 _exptl_absorpt_process_details ? _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 'Saturn70 (4x4 bin mode)' _diffrn_measurement_method dtprofit.ref _diffrn_detector_area_resol_mean 28.5714 _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 4301 _diffrn_reflns_av_R_equivalents 0.0000 _diffrn_reflns_av_sigmaI/netI 0.0193 _diffrn_reflns_limit_h_min 0 _diffrn_reflns_limit_h_max 20 _diffrn_reflns_limit_k_min -25 _diffrn_reflns_limit_k_max 0 _diffrn_reflns_limit_l_min -35 _diffrn_reflns_limit_l_max -2 _diffrn_reflns_theta_min 2.08 _diffrn_reflns_theta_max 27.44 _reflns_number_total 4301 _reflns_number_gt 3498 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear (Rigaku, 2000)' _computing_cell_refinement 'CrystalClear (Rigaku, 2000)' _computing_data_reduction 'CrystalClear (Rigaku, 2000)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'SHELXL-97 (Sheldrick, 1997)' _computing_publication_material 'SHELXL-97 (Sheldrick, 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^)+(0.1900P)^2^+0.0000P] 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 4301 _refine_ls_number_parameters 82 _refine_ls_number_restraints 30 _refine_ls_R_factor_all 0.0719 _refine_ls_R_factor_gt 0.0688 _refine_ls_wR_factor_ref 0.2230 _refine_ls_wR_factor_gt 0.2125 _refine_ls_goodness_of_fit_ref 1.031 _refine_ls_restrained_S_all 1.036 _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 Zn1 Zn 0.0000 0.198741(10) 0.5000 0.0409(2) Uani 1 4 d S . . O1 O 0.05162(4) 0.21039(5) 0.44858(4) 0.0660(4) Uani 1 1 d . . . N1 N 0.0000 0.12589(9) 0.5000 0.0575(6) Uani 1 4 d SD . . C1 C 0.06663(6) 0.2500 0.43337(6) 0.0561(5) Uani 1 2 d S . . C2 C 0.10427(6) 0.2500 0.39573(6) 0.0618(6) Uani 1 2 d S . . C7 C 0.2500 0.21509(7) 0.28491(7) 0.0722(7) Uani 1 2 d S . . H7 H 0.2500 0.1914 0.3086 0.087 Uiso 1 2 calc SR . . C5 C 0.17615(7) 0.2500 0.32385(7) 0.0707(7) Uani 1 2 d S . . C4 C 0.15727(7) 0.29204(8) 0.34154(8) 0.0840(6) Uani 1 1 d . . . H4 H 0.1682 0.3212 0.3291 0.101 Uiso 1 1 calc R . . C3 C 0.12257(7) 0.29279(8) 0.37718(7) 0.0738(5) Uani 1 1 d . . . H3 H 0.1113 0.3221 0.3889 0.089 Uiso 1 1 calc R . . C6 C 0.21414(7) 0.2500 0.28586(7) 0.0740(7) Uani 1 2 d S . . C10 C 0.0000 0.02621(14) 0.5000 0.0776(10) Uani 1 4 d SD . . C8 C 0.0408(2) 0.1020(3) 0.5000 0.239(4) Uani 0.80 2 d SPD . . C9 C 0.0431(2) 0.0506(2) 0.5000 0.239(4) Uani 0.80 2 d SPD . . C12 C 0.0000 0.0521(4) 0.4582(3) 0.159(9) Uani 0.20 2 d SPD . . C11 C 0.0000 0.1010(4) 0.4584(3) 0.159(9) Uani 0.20 2 d SPD . . 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 Zn1 0.0443(2) 0.0350(2) 0.0436(2) 0.000 0.000 0.000 O1 0.0712(8) 0.0612(7) 0.0654(7) 0.0034(5) 0.0130(6) -0.0011(5) N1 0.0637(15) 0.0404(12) 0.0684(16) 0.000 0.000 0.000 C1 0.0586(8) 0.0509(12) 0.0586(8) 0.0021(6) 0.0039(10) 0.0021(6) C2 0.0629(8) 0.0598(13) 0.0629(8) 0.0041(7) 0.0079(10) 0.0041(7) C7 0.0739(16) 0.0713(10) 0.0713(10) 0.0112(12) 0.0128(11) 0.0128(11) C5 0.0763(10) 0.0593(13) 0.0763(10) 0.0063(8) 0.0149(13) 0.0063(8) C4 0.0930(14) 0.0700(12) 0.0889(14) 0.0081(10) 0.0236(13) -0.0011(10) C3 0.0783(12) 0.0616(10) 0.0816(12) 0.0008(9) 0.0168(10) 0.0067(8) C6 0.0754(11) 0.0711(16) 0.0754(11) 0.0132(11) 0.0165(13) 0.0132(11) C10 0.095(3) 0.052(2) 0.086(3) 0.000 0.000 0.000 C8 0.196(7) 0.112(4) 0.409(15) 0.000 0.000 0.009(4) C9 0.196(7) 0.112(4) 0.409(15) 0.000 0.000 0.009(4) C12 0.28(3) 0.119(12) 0.079(9) 0.007(9) 0.000 0.000 C11 0.28(3) 0.119(12) 0.079(9) 0.007(9) 0.000 0.000 _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 Zn1 N1 2.021(3) . ? Zn1 O1 2.0465(12) 30 ? Zn1 O1 2.0465(12) . ? Zn1 O1 2.0465(12) 27_556 ? Zn1 O1 2.0465(12) 9_556 ? Zn1 Zn1 2.8435(5) 32_666 ? O1 C1 1.2483(16) . ? N1 C8 1.312(6) 9_556 ? N1 C8 1.312(6) . ? N1 C11 1.345(9) . ? N1 C11 1.345(9) 9_556 ? C1 O1 1.2483(16) 24 ? C1 C2 1.477(3) . ? C2 C3 1.390(2) 24 ? C2 C3 1.390(2) . ? C7 C6 1.3883(18) 11 ? C7 C6 1.3883(18) . ? C7 H7 0.9300 . ? C5 C4 1.369(3) 24 ? C5 C4 1.369(3) . ? C5 C6 1.490(4) . ? C4 C3 1.380(3) . ? C4 H4 0.9300 . ? C3 H3 0.9300 . ? C6 C7 1.3883(18) 12 ? C10 C12 1.363(9) 9_556 ? C10 C12 1.363(9) . ? C10 C9 1.375(7) . ? C10 C9 1.375(7) 9_556 ? C10 C10 1.454(8) 25_556 ? C8 C9 1.426(8) . ? C8 C11 1.618(7) . ? C8 C11 1.618(7) 9_556 ? C9 C12 1.666(7) . ? C9 C12 1.666(7) 9_556 ? C12 C11 1.357(11) . ? C12 C9 1.666(7) 9_556 ? C11 C8 1.618(7) 9_556 ? 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 N1 Zn1 O1 99.08(4) . 30 ? N1 Zn1 O1 99.08(4) . . ? O1 Zn1 O1 88.79(6) 30 . ? N1 Zn1 O1 99.08(4) . 27_556 ? O1 Zn1 O1 161.84(8) 30 27_556 ? O1 Zn1 O1 88.36(6) . 27_556 ? N1 Zn1 O1 99.08(4) . 9_556 ? O1 Zn1 O1 88.36(6) 30 9_556 ? O1 Zn1 O1 161.84(8) . 9_556 ? O1 Zn1 O1 88.79(6) 27_556 9_556 ? N1 Zn1 Zn1 180.0 . 32_666 ? O1 Zn1 Zn1 80.92(4) 30 32_666 ? O1 Zn1 Zn1 80.92(4) . 32_666 ? O1 Zn1 Zn1 80.92(4) 27_556 32_666 ? O1 Zn1 Zn1 80.92(4) 9_556 32_666 ? C1 O1 Zn1 127.42(13) . . ? C8 N1 C8 119.4(6) 9_556 . ? C8 N1 C11 75.0(3) 9_556 . ? C8 N1 C11 75.0(3) . . ? C8 N1 C11 75.0(3) 9_556 9_556 ? C8 N1 C11 75.0(3) . 9_556 ? C11 N1 C11 118.3(9) . 9_556 ? C8 N1 Zn1 120.3(3) 9_556 . ? C8 N1 Zn1 120.3(3) . . ? C11 N1 Zn1 120.9(4) . . ? C11 N1 Zn1 120.9(4) 9_556 . ? O1 C1 O1 123.3(2) . 24 ? O1 C1 C2 118.34(11) . . ? O1 C1 C2 118.34(11) 24 . ? C3 C2 C3 117.3(2) 24 . ? C3 C2 C1 121.34(11) 24 . ? C3 C2 C1 121.34(11) . . ? C6 C7 C6 122.7(3) 11 . ? C6 C7 H7 118.7 11 . ? C6 C7 H7 118.7 . . ? C4 C5 C4 116.8(3) 24 . ? C4 C5 C6 121.59(13) 24 . ? C4 C5 C6 121.59(13) . . ? C5 C4 C3 122.4(2) . . ? C5 C4 H4 118.8 . . ? C3 C4 H4 118.8 . . ? C4 C3 C2 120.47(19) . . ? C4 C3 H3 119.8 . . ? C2 C3 H3 119.8 . . ? C7 C6 C7 117.3(3) . 12 ? C7 C6 C5 121.34(15) . . ? C7 C6 C5 121.34(15) 12 . ? C12 C10 C12 116.5(9) 9_556 . ? C12 C10 C9 75.0(2) 9_556 . ? C12 C10 C9 75.0(2) . . ? C12 C10 C9 75.0(2) 9_556 9_556 ? C12 C10 C9 75.0(2) . 9_556 ? C9 C10 C9 120.9(6) . 9_556 ? C12 C10 C10 121.7(4) 9_556 25_556 ? C12 C10 C10 121.7(4) . 25_556 ? C9 C10 C10 119.5(3) . 25_556 ? C9 C10 C10 119.5(3) 9_556 25_556 ? N1 C8 C9 122.9(6) . . ? N1 C8 C11 53.4(3) . . ? C9 C8 C11 90.8(5) . . ? N1 C8 C11 53.4(3) . 9_556 ? C9 C8 C11 90.8(5) . 9_556 ? C11 C8 C11 91.1(5) . 9_556 ? C10 C9 C8 117.0(5) . . ? C10 C9 C12 52.2(3) . . ? C8 C9 C12 86.8(5) . . ? C10 C9 C12 52.2(3) . 9_556 ? C8 C9 C12 86.8(5) . 9_556 ? C12 C9 C12 88.2(5) . 9_556 ? C11 C12 C10 121.6(7) . . ? C11 C12 C9 91.2(5) . . ? C10 C12 C9 52.8(3) . . ? C11 C12 C9 91.2(5) . 9_556 ? C10 C12 C9 52.8(3) . 9_556 ? C9 C12 C9 91.8(5) . 9_556 ? N1 C11 C12 121.1(7) . . ? N1 C11 C8 51.6(3) . . ? C12 C11 C8 91.1(6) . . ? N1 C11 C8 51.6(3) . 9_556 ? C12 C11 C8 91.1(6) . 9_556 ? C8 C11 C8 88.9(5) . 9_556 ? _diffrn_measured_fraction_theta_max 0.992 _diffrn_reflns_theta_full 27.44 _diffrn_measured_fraction_theta_full 0.992 _refine_diff_density_max 1.885 _refine_diff_density_min -1.068 _refine_diff_density_rms 0.057