# Electronic Supplementary Material for CrystEngComm # This journal is (c) The Royal Society of Chemistry 2009 data_global _journal_name_full CrystEngComm _journal_coden_Cambridge 1350 _publ_contact_author_name 'Can-Zhong Lu' _publ_contact_author_email CZLU@FJIRSM.AC.CN _publ_section_title ; New (3, 4)-connected intrinsically chiral topology observed in a homochiral coordination polymer from achiral precursors ; loop_ _publ_author_name 'Can-Zhong Lu' 'Shan-Ci Chen' 'Shu-Mei Chen' 'Fei Wang' 'Xiao-Yuan Wu' 'Yi-Ming Xie' 'Rong-Min Yu' 'Jian Zhang' # Attachment 'check1.CIF' data_1 _database_code_depnum_ccdc_archive 'CCDC 714946' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C7 H4 Cu2 N6' _chemical_formula_sum 'C7 H4 Cu2 N6' _chemical_formula_weight 299.24 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 Orthorhombic _symmetry_space_group_name_H-M P2(1)2(1)2(1) loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-x, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z' _cell_length_a 4.535(3) _cell_length_b 10.913(7) _cell_length_c 17.142(10) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 848.5(9) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 2844 _cell_measurement_theta_min 2.2124 _cell_measurement_theta_max 27.4662 _exptl_crystal_description Prism _exptl_crystal_colour Green _exptl_crystal_size_max 0.12 _exptl_crystal_size_mid 0.10 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.343 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 584 _exptl_absorpt_coefficient_mu 4.979 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.5864 _exptl_absorpt_correction_T_max 0.7889 _exptl_absorpt_process_details 'CrystalClear, Rigaku, 2005' _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 Saturn724 _diffrn_measurement_method CCD_Profile_fitting _diffrn_detector_area_resol_mean 28.5714 _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 7255 _diffrn_reflns_av_R_equivalents 0.0661 _diffrn_reflns_av_sigmaI/netI 0.0500 _diffrn_reflns_limit_h_min -5 _diffrn_reflns_limit_h_max 5 _diffrn_reflns_limit_k_min -14 _diffrn_reflns_limit_k_max 14 _diffrn_reflns_limit_l_min -22 _diffrn_reflns_limit_l_max 21 _diffrn_reflns_theta_min 2.21 _diffrn_reflns_theta_max 27.44 _reflns_number_total 1916 _reflns_number_gt 1757 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear (Rigaku/MSC Inc., 2005)' _computing_cell_refinement 'CrystalClear (Rigaku/MSC Inc., 2005)' _computing_data_reduction 'CrystalClear (Rigaku/MSC Inc., 2005)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _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^)+(0.1210P)^2^+0.0794P] 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 none _refine_ls_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack -0.04(4) _refine_ls_number_reflns 1916 _refine_ls_number_parameters 148 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.0547 _refine_ls_R_factor_gt 0.0498 _refine_ls_wR_factor_ref 0.1594 _refine_ls_wR_factor_gt 0.1528 _refine_ls_goodness_of_fit_ref 0.998 _refine_ls_restrained_S_all 1.002 _refine_ls_shift/su_max 0.064 _refine_ls_shift/su_mean 0.004 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 0.99074(18) 0.63055(7) 0.53754(4) 0.0287(3) Uani 1 1 d . . . Cu2 Cu 1.0397(2) 0.69578(7) 0.17621(5) 0.0321(3) Uani 1 1 d . . . N4 N 0.9903(13) 0.6987(4) 0.2985(3) 0.0267(11) Uani 1 1 d . . . N1 N 0.9573(12) 0.6774(5) 0.4260(3) 0.0246(11) Uani 1 1 d . . . N3 N 0.7932(12) 0.7788(5) 0.3259(3) 0.0271(11) Uani 1 1 d . . . N2 N 0.7726(13) 0.7672(5) 0.4012(4) 0.0284(12) Uani 1 1 d . . . N6 N 0.7835(17) 0.4987(6) 0.5867(4) 0.0378(15) Uani 1 1 d . . . N5 N 1.6911(14) 0.3376(6) 0.3409(3) 0.0310(12) Uani 1 1 d . . . C2 C 1.4482(16) 0.5135(6) 0.2864(3) 0.0292(14) Uani 1 1 d . . . H2 H 1.42(2) 0.563(8) 0.229(6) 0.06(3) Uiso 1 1 d . . . C5 C 1.5534(19) 0.3606(6) 0.4083(4) 0.0354(16) Uani 1 1 d D . . H5 H 1.5915 0.3094 0.4505 0.042 Uiso 1 1 calc RD . . C4 C 1.3593(18) 0.4553(7) 0.4186(4) 0.0366(16) Uani 1 1 d . . . H3 H 1.23(2) 0.438(9) 0.471(6) 0.06(3) Uiso 1 1 d . . . C3 C 1.2997(15) 0.5348(6) 0.3556(4) 0.0250(13) Uani 1 1 d . . . C1 C 1.6399(18) 0.4162(6) 0.2807(5) 0.0306(14) Uani 1 1 d . . . H1 H 1.76(2) 0.396(9) 0.241(6) 0.06(3) Uiso 1 1 d . . . C6 C 1.0889(15) 0.6350(6) 0.3610(4) 0.0253(13) Uani 1 1 d . . . C7 C 0.6592(18) 0.4217(6) 0.6170(4) 0.0320(15) Uani 1 1 d . . . 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 0.0332(5) 0.0279(4) 0.0250(4) 0.0020(3) 0.0012(4) -0.0026(4) Cu2 0.0346(5) 0.0281(4) 0.0337(5) -0.0043(3) -0.0033(4) -0.0042(4) N4 0.033(3) 0.026(2) 0.021(2) 0.0029(18) 0.001(2) 0.003(3) N1 0.019(3) 0.029(2) 0.025(2) 0.0009(19) -0.001(2) 0.003(2) N3 0.028(3) 0.029(3) 0.024(3) 0.002(2) -0.003(2) 0.002(2) N2 0.029(3) 0.025(3) 0.031(3) 0.003(2) -0.002(2) 0.007(2) N6 0.052(4) 0.031(3) 0.031(3) 0.001(3) -0.002(3) -0.008(3) N5 0.037(3) 0.031(3) 0.025(3) 0.004(2) -0.005(2) 0.007(2) C2 0.032(4) 0.032(3) 0.024(3) 0.001(3) 0.003(3) 0.008(3) C5 0.048(4) 0.032(3) 0.027(3) 0.007(3) 0.002(3) 0.010(3) C4 0.041(4) 0.044(4) 0.025(3) 0.010(3) 0.003(3) 0.013(4) C3 0.027(3) 0.022(3) 0.025(3) 0.001(2) -0.003(2) -0.001(3) C1 0.033(4) 0.026(3) 0.032(3) 0.001(3) 0.004(3) 0.005(3) C6 0.026(3) 0.025(3) 0.024(3) -0.002(2) 0.004(2) -0.001(3) C7 0.041(4) 0.028(3) 0.027(3) 0.004(3) -0.001(3) -0.004(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 N6 1.914(7) . ? Cu1 N1 1.985(5) . ? Cu1 N2 1.996(6) 4_566 ? Cu2 C7 1.867(7) 2_664 ? Cu2 N5 1.993(6) 3_855 ? Cu2 N4 2.109(5) . ? N4 N3 1.336(8) . ? N4 C6 1.352(8) . ? N1 C6 1.346(8) . ? N1 N2 1.358(7) . ? N3 N2 1.299(8) . ? N2 Cu1 1.996(6) 4_466 ? N6 C7 1.138(10) . ? N5 C5 1.338(9) . ? N5 C1 1.361(9) . ? N5 Cu2 1.993(6) 3_845 ? C2 C1 1.376(9) . ? C2 C3 1.384(9) . ? C2 H2 1.13(10) . ? C5 C4 1.369(10) . ? C5 H5 0.9300 . ? C4 C3 1.412(9) . ? C4 H3 1.08(11) . ? C3 C6 1.456(9) . ? C1 H1 0.91(11) . ? C7 Cu2 1.867(7) 2_665 ? 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 N6 Cu1 N1 125.4(3) . . ? N6 Cu1 N2 120.2(3) . 4_566 ? N1 Cu1 N2 114.3(2) . 4_566 ? C7 Cu2 N5 138.5(3) 2_664 3_855 ? C7 Cu2 N4 119.9(3) 2_664 . ? N5 Cu2 N4 101.5(2) 3_855 . ? N3 N4 C6 106.2(5) . . ? N3 N4 Cu2 115.5(4) . . ? C6 N4 Cu2 138.1(4) . . ? C6 N1 N2 105.2(5) . . ? C6 N1 Cu1 132.5(4) . . ? N2 N1 Cu1 122.4(4) . . ? N2 N3 N4 109.5(5) . . ? N3 N2 N1 109.7(5) . . ? N3 N2 Cu1 120.9(4) . 4_466 ? N1 N2 Cu1 129.3(5) . 4_466 ? C7 N6 Cu1 178.7(6) . . ? C5 N5 C1 117.2(6) . . ? C5 N5 Cu2 124.0(5) . 3_845 ? C1 N5 Cu2 118.8(5) . 3_845 ? C1 C2 C3 119.8(6) . . ? C1 C2 H2 112(5) . . ? C3 C2 H2 128(5) . . ? N5 C5 C4 123.6(6) . . ? N5 C5 H5 118.2 . . ? C4 C5 H5 118.2 . . ? C5 C4 C3 119.2(7) . . ? C5 C4 H3 109(6) . . ? C3 C4 H3 130(6) . . ? C2 C3 C4 117.4(6) . . ? C2 C3 C6 120.1(5) . . ? C4 C3 C6 122.6(6) . . ? N5 C1 C2 122.8(7) . . ? N5 C1 H1 107(7) . . ? C2 C1 H1 130(6) . . ? N1 C6 N4 109.4(5) . . ? N1 C6 C3 127.0(6) . . ? N4 C6 C3 123.5(5) . . ? N6 C7 Cu2 174.2(7) . 2_665 ? _diffrn_measured_fraction_theta_max 0.994 _diffrn_reflns_theta_full 27.44 _diffrn_measured_fraction_theta_full 0.994 _refine_diff_density_max 0.750 _refine_diff_density_min -1.009 _refine_diff_density_rms 0.224