# Supplementary Material (ESI) for Chemical Communications # This journal is (c) The Royal Society of Chemistry 2007 data_global _journal_name_full Chem.Commun. _journal_coden_Cambridge 0182 _publ_contact_author_name 'Xian-He Bu' _publ_contact_author_address ; Department of Chemistry Nankai University Tianjin 300071 CHINA ; _publ_contact_author_email BUXH@NANKAI.EDU.CN _publ_section_title ; An Azido-CuII-triazolate Complex with utp-Type Topological Network, Showing Spin-canted Antiferromagnetism ; loop_ _publ_author_name 'Xian-He Bu.' 'Jian-Rong Li.' 'E. Carolina Sanudo' 'Ying Tao.' 'Qun Yu.' # Attachment 'Revised_Crystallographic_Data-B702988H.cif' data_1 _database_code_depnum_ccdc_archive 'CCDC 635768' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C2 H2 Cu N6' _chemical_formula_sum 'C2 H2 Cu N6' _chemical_formula_weight 173.64 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' Cu Cu 0.3201 1.2651 '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' H H 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M Pna21 _symmetry_space_group_name_Hall 'P 2c -2n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z+1/2' '-x+1/2, y+1/2, z+1/2' 'x+1/2, -y+1/2, z' _cell_length_a 6.7054(13) _cell_length_b 9.0818(18) _cell_length_c 8.1187(16) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 494.41(17) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 3885 _cell_measurement_theta_min 3.04 _cell_measurement_theta_max 27.47 _exptl_crystal_description Block _exptl_crystal_colour 'Black Green' _exptl_crystal_size_max 0.10 _exptl_crystal_size_mid 0.08 _exptl_crystal_size_min 0.08 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.333 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 340 _exptl_absorpt_coefficient_mu 4.306 _exptl_absorpt_correction_type Multi-Scan _exptl_absorpt_correction_T_min 0.9102 _exptl_absorpt_correction_T_max 1.0000 _exptl_absorpt_process_details 'ABSCOR (Higashi, 1995)' _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 'Rigaku R-AXIS RAPID IP' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean 10.000 _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 4548 _diffrn_reflns_av_R_equivalents 0.0412 _diffrn_reflns_av_sigmaI/netI 0.0434 _diffrn_reflns_limit_h_min -8 _diffrn_reflns_limit_h_max 8 _diffrn_reflns_limit_k_min -11 _diffrn_reflns_limit_k_max 11 _diffrn_reflns_limit_l_min -10 _diffrn_reflns_limit_l_max 10 _diffrn_reflns_theta_min 3.37 _diffrn_reflns_theta_max 27.47 _reflns_number_total 1128 _reflns_number_gt 1025 _reflns_threshold_expression I>2sigma(I) _computing_data_collection 'RAPID-AUTO (Rigaku, 2004)' _computing_cell_refinement RAPID-AUTO _computing_data_reduction "CrystalStructure (Rigaku/MSC'2004)" _computing_structure_solution SHELXS-97 _computing_structure_refinement SHELXL-97 _computing_molecular_graphics 'SHELXTL (Bruker, 1998)' _computing_publication_material 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^)+(0.0180P)^2^+0.1909P] 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_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.02(3) _refine_ls_number_reflns 1128 _refine_ls_number_parameters 91 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.0266 _refine_ls_R_factor_gt 0.0234 _refine_ls_wR_factor_ref 0.0560 _refine_ls_wR_factor_gt 0.0537 _refine_ls_goodness_of_fit_ref 1.041 _refine_ls_restrained_S_all 1.041 _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 0.24593(4) 0.16089(3) 0.49974(13) 0.01141(11) Uani 1 1 d . . . N1 N 0.3419(3) 0.3189(2) 0.3407(3) 0.0140(4) Uani 1 1 d . . . N2 N 0.5255(3) 0.3857(2) 0.3424(3) 0.0134(4) Uani 1 1 d . . . N3 N 0.3421(3) 0.4968(2) 0.1529(3) 0.0140(4) Uani 1 1 d . . . N4 N 0.5004(4) 0.1876(3) 0.6218(3) 0.0176(5) Uani 1 1 d . . . N5 N 0.5071(4) 0.1617(3) 0.7663(4) 0.0301(7) Uani 1 1 d . . . N6 N 0.498(3) 0.1638(16) 0.908(2) 0.059(4) Uani 0.50 1 d P A 1 N6' N 0.541(3) 0.1073(15) 0.899(2) 0.051(4) Uani 0.50 1 d P A 2 C1 C 0.5202(4) 0.4898(3) 0.2299(4) 0.0172(7) Uani 1 1 d . . . H1A H 0.6270 0.5516 0.2062 0.021 Uiso 1 1 calc R . . C2 C 0.2372(4) 0.3893(4) 0.2262(4) 0.0173(6) Uani 1 1 d . . . H2A H 0.1058 0.3666 0.1997 0.021 Uiso 1 1 calc R . . 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 0.01080(15) 0.01255(17) 0.01089(16) 0.00320(19) -0.00195(13) -0.00223(10) N1 0.0102(10) 0.0159(11) 0.0159(12) 0.0038(9) -0.0031(10) -0.0028(8) N2 0.0107(10) 0.0121(11) 0.0173(12) 0.0019(9) -0.0009(10) -0.0013(8) N3 0.0107(10) 0.0161(11) 0.0152(11) 0.0040(9) -0.0005(9) 0.0002(9) N4 0.0171(12) 0.0194(13) 0.0165(14) 0.0034(10) -0.0037(10) -0.0041(9) N5 0.0239(15) 0.0421(17) 0.024(2) 0.0099(12) -0.0102(12) -0.0133(12) N6 0.071(11) 0.076(12) 0.029(6) 0.028(8) -0.023(6) -0.011(7) N6' 0.049(7) 0.072(11) 0.031(5) 0.032(7) -0.024(5) -0.015(7) C1 0.0126(14) 0.0168(14) 0.0221(18) 0.0066(11) -0.0009(12) -0.0012(10) C2 0.0150(14) 0.0189(15) 0.0181(15) 0.0064(12) -0.0026(11) -0.0023(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 Cu1 N4 1.988(2) . ? Cu1 N2 1.999(2) 4_455 ? Cu1 N3 2.028(2) 3_545 ? Cu1 N1 2.035(2) . ? Cu1 N4 2.363(3) 4_455 ? N1 C2 1.329(4) . ? N1 N2 1.372(3) . ? N2 C1 1.315(4) . ? N2 Cu1 1.999(2) 4 ? N3 C2 1.342(4) . ? N3 C1 1.350(4) . ? N3 Cu1 2.028(2) 3_554 ? N4 N5 1.197(4) . ? N4 Cu1 2.363(3) 4 ? N5 N6 1.15(2) . ? N5 N6' 1.209(16) . ? C1 H1A 0.9300 . ? C2 H2A 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 N4 Cu1 N2 168.24(12) . 4_455 ? N4 Cu1 N3 91.94(10) . 3_545 ? N2 Cu1 N3 91.22(9) 4_455 3_545 ? N4 Cu1 N1 87.62(10) . . ? N2 Cu1 N1 88.71(10) 4_455 . ? N3 Cu1 N1 177.44(10) 3_545 . ? N4 Cu1 N4 108.54(10) . 4_455 ? N2 Cu1 N4 82.88(9) 4_455 4_455 ? N3 Cu1 N4 88.17(10) 3_545 4_455 ? N1 Cu1 N4 94.36(9) . 4_455 ? C2 N1 N2 105.5(2) . . ? C2 N1 Cu1 128.03(17) . . ? N2 N1 Cu1 126.11(18) . . ? C1 N2 N1 106.7(2) . . ? C1 N2 Cu1 128.02(19) . 4 ? N1 N2 Cu1 125.17(18) . 4 ? C2 N3 C1 102.9(2) . . ? C2 N3 Cu1 130.83(19) . 3_554 ? C1 N3 Cu1 125.2(2) . 3_554 ? N5 N4 Cu1 119.8(2) . . ? N5 N4 Cu1 119.9(2) . 4 ? Cu1 N4 Cu1 117.39(13) . 4 ? N6 N5 N4 166.7(7) . . ? N6 N5 N6' 29.0(11) . . ? N4 N5 N6' 164.1(8) . . ? N2 C1 N3 112.3(3) . . ? N2 C1 H1A 123.9 . . ? N3 C1 H1A 123.9 . . ? N1 C2 N3 112.6(2) . . ? N1 C2 H2A 123.7 . . ? N3 C2 H2A 123.7 . . ? loop_ _geom_torsion_atom_site_label_1 _geom_torsion_atom_site_label_2 _geom_torsion_atom_site_label_3 _geom_torsion_atom_site_label_4 _geom_torsion _geom_torsion_site_symmetry_1 _geom_torsion_site_symmetry_2 _geom_torsion_site_symmetry_3 _geom_torsion_site_symmetry_4 _geom_torsion_publ_flag N4 Cu1 N1 C2 -167.7(3) . . . . ? N2 Cu1 N1 C2 23.5(3) 4_455 . . . ? N3 Cu1 N1 C2 112(2) 3_545 . . . ? N4 Cu1 N1 C2 -59.2(3) 4_455 . . . ? N4 Cu1 N1 N2 4.9(2) . . . . ? N2 Cu1 N1 N2 -163.9(2) 4_455 . . . ? N3 Cu1 N1 N2 -75(2) 3_545 . . . ? N4 Cu1 N1 N2 113.3(2) 4_455 . . . ? C2 N1 N2 C1 -0.3(3) . . . . ? Cu1 N1 N2 C1 -174.26(19) . . . . ? C2 N1 N2 Cu1 175.5(2) . . . 4 ? Cu1 N1 N2 Cu1 1.6(3) . . . 4 ? N2 Cu1 N4 N5 -135.6(5) 4_455 . . . ? N3 Cu1 N4 N5 -30.1(3) 3_545 . . . ? N1 Cu1 N4 N5 152.5(3) . . . . ? N4 Cu1 N4 N5 58.7(2) 4_455 . . . ? N2 Cu1 N4 Cu1 63.7(6) 4_455 . . 4 ? N3 Cu1 N4 Cu1 169.22(13) 3_545 . . 4 ? N1 Cu1 N4 Cu1 -8.26(14) . . . 4 ? N4 Cu1 N4 Cu1 -102.06(19) 4_455 . . 4 ? Cu1 N4 N5 N6 -82(5) . . . . ? Cu1 N4 N5 N6 78(5) 4 . . . ? Cu1 N4 N5 N6' 110(4) . . . . ? Cu1 N4 N5 N6' -90(4) 4 . . . ? N1 N2 C1 N3 0.2(3) . . . . ? Cu1 N2 C1 N3 -175.6(2) 4 . . . ? C2 N3 C1 N2 0.1(3) . . . . ? Cu1 N3 C1 N2 169.33(19) 3_554 . . . ? N2 N1 C2 N3 0.4(4) . . . . ? Cu1 N1 C2 N3 174.2(2) . . . . ? C1 N3 C2 N1 -0.3(4) . . . . ? Cu1 N3 C2 N1 -168.7(2) 3_554 . . . ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 27.47 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.277 _refine_diff_density_min -0.409 _refine_diff_density_rms 0.071