# Supplementary Material (ESI) for Dalton Transactions # This journal is (c) The Royal Society of Chemistry 2009 data_global _journal_name_full 'Dalton Trans.' _journal_coden_Cambridge 0222 _journal_volume ? _journal_page_first ? _journal_year ? _publ_contact_author_name 'En-Qing Gao' _publ_contact_author_email EQGAO@CHEM.ECNU.EDU.CN _publ_section_title ; Novel manganese(II) and cobalt(II) 3D polymers with mixed cyanate and carboxylate bridges: crystal structure and magnetic properties ; loop_ _publ_author_name 'En-Qing Gao.' 'You Song.' 'Qian Sun.' 'Hua Tian.' 'Yanqin Wang.' 'Kun Wang.' # Attachment '739971.cif' data_1 _database_code_depnum_ccdc_archive 'CCDC 739971' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C9 H8 Mn N2 O6' _chemical_formula_weight 295.11 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' Mn Mn 0.3368 0.7283 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Orthorhombic _symmetry_space_group_name_H-M 'Pnma ' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-x, y+1/2, -z' 'x+1/2, -y+1/2, -z+1/2' '-x, -y, -z' 'x-1/2, y, -z-1/2' 'x, -y-1/2, z' '-x-1/2, y-1/2, z-1/2' _cell_length_a 7.621(5) _cell_length_b 7.519(5) _cell_length_c 18.177(13) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1041.7(13) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 1183 _cell_measurement_theta_min 2.20 _cell_measurement_theta_max 25.21 _exptl_crystal_description plate _exptl_crystal_colour yellow _exptl_crystal_size_max 0.10 _exptl_crystal_size_mid 0.08 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.882 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 596 _exptl_absorpt_coefficient_mu 1.291 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8829 _exptl_absorpt_correction_T_max 0.9389 _exptl_absorpt_process_details 'SADABS (Bruker, 1999)' _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 'CCD area detector' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% 2.5 _diffrn_reflns_number 4917 _diffrn_reflns_av_R_equivalents 0.0991 _diffrn_reflns_av_sigmaI/netI 0.0942 _diffrn_reflns_limit_h_min -7 _diffrn_reflns_limit_h_max 9 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 9 _diffrn_reflns_limit_l_min -23 _diffrn_reflns_limit_l_max 23 _diffrn_reflns_theta_min 2.24 _diffrn_reflns_theta_max 27.15 _reflns_number_total 1243 _reflns_number_gt 718 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker SMART' _computing_cell_refinement 'Bruker SMART' _computing_data_reduction 'Bruker SHELXTL' _computing_structure_solution 'Bruker SHELXTL' _computing_structure_refinement 'Bruker SHELXTL' _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^)+(0.0390P)^2^+4.3982P] 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 ? _refine_ls_number_reflns 1243 _refine_ls_number_parameters 102 _refine_ls_number_restraints 3 _refine_ls_R_factor_all 0.1437 _refine_ls_R_factor_gt 0.0779 _refine_ls_wR_factor_ref 0.1676 _refine_ls_wR_factor_gt 0.1486 _refine_ls_goodness_of_fit_ref 1.170 _refine_ls_restrained_S_all 1.168 _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 Mn1 Mn 0.5000 0.0000 0.5000 0.0270(4) Uani 1 2 d S . . C1 C 0.5440(10) 0.2500 0.6394(5) 0.031(2) Uani 1 2 d S . . C2 C 0.5275(9) 0.2500 0.7219(5) 0.028(2) Uani 1 2 d S . . C3 C 0.5151(10) 0.0940(9) 0.7603(3) 0.0480(18) Uani 1 1 d . . . H3A H 0.5191 -0.0140 0.7354 0.058 Uiso 1 1 calc R . . C4 C 0.4967(11) 0.0960(8) 0.8353(3) 0.0483(18) Uani 1 1 d . . . H4A H 0.4900 -0.0105 0.8611 0.058 Uiso 1 1 calc R . . C5 C 0.4761(10) 0.2500 0.9521(4) 0.0278(19) Uani 1 2 d S . . H5A H 0.4151 0.3567 0.9692 0.033 Uiso 1 1 d R . . C6 C 0.6665(11) 0.2500 0.9812(4) 0.0253(19) Uani 1 2 d S . . N2 N 0.5918(10) 0.2500 0.4459(4) 0.0327(18) Uani 1 2 d S . . C7 C 0.6734(15) 0.2500 0.3928(6) 0.048(3) Uani 1 2 d S . . O4 O 0.7545(16) 0.2500 0.3369(5) 0.106(4) Uani 1 2 d S . . N1 N 0.4884(10) 0.2500 0.8712(4) 0.0292(16) Uani 1 2 d S . . O1 O 0.5562(8) 0.1025(6) 0.6092(2) 0.0530(15) Uani 1 1 d . . . O2 O 0.7366(6) 0.1029(6) 0.9901(3) 0.0538(14) Uani 1 1 d . . . O3 O 0.2625(19) -0.2500 0.8339(8) 0.138(5) Uani 1 2 d SD . . H3WA H 0.24(3) -0.2500 0.788(3) 0.207 Uiso 1 2 d SD . . H3WB H 0.167(16) -0.2500 0.859(9) 0.207 Uiso 1 2 d SD . . 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 Mn1 0.0279(6) 0.0227(6) 0.0304(6) -0.0015(6) 0.0043(7) 0.0006(7) C1 0.014(4) 0.044(6) 0.035(5) 0.000 -0.004(3) 0.000 C2 0.005(4) 0.042(5) 0.038(5) 0.000 0.001(3) 0.000 C3 0.078(5) 0.029(4) 0.037(3) -0.007(3) -0.007(4) 0.005(5) C4 0.082(6) 0.023(3) 0.040(3) 0.004(3) -0.006(4) 0.003(5) C5 0.010(4) 0.041(5) 0.033(4) 0.000 0.001(4) 0.000 C6 0.022(4) 0.031(5) 0.024(5) 0.000 0.002(3) 0.000 N2 0.037(4) 0.020(4) 0.041(4) 0.000 0.009(4) 0.000 C7 0.054(7) 0.027(6) 0.062(7) 0.000 0.025(6) 0.000 O4 0.151(10) 0.070(6) 0.096(7) 0.000 0.092(7) 0.000 N1 0.025(4) 0.030(4) 0.032(4) 0.000 0.000(4) 0.000 O1 0.093(4) 0.035(3) 0.032(2) -0.008(2) 0.002(3) -0.010(3) O2 0.032(2) 0.030(2) 0.099(4) 0.002(3) -0.016(3) 0.000(2) O3 0.131(11) 0.125(10) 0.158(12) 0.000 -0.001(10) 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 Mn1 O2 2.159(5) 6_557 ? Mn1 O2 2.159(5) 2_654 ? Mn1 O1 2.172(4) . ? Mn1 O1 2.172(4) 5_656 ? Mn1 N2 2.234(4) 5_656 ? Mn1 N2 2.234(4) . ? C1 O1 1.241(6) . ? C1 O1 1.241(6) 7_565 ? C1 C2 1.504(12) . ? C2 C3 1.368(8) 7_565 ? C2 C3 1.368(8) . ? C3 C4 1.371(8) . ? C3 H3A 0.9300 . ? C4 N1 1.331(7) . ? C4 H4A 0.9300 . ? C5 N1 1.472(10) . ? C5 C6 1.544(11) . ? C5 H5A 0.9778 . ? C6 O2 1.239(6) 7_565 ? C6 O2 1.239(6) . ? N2 C7 1.148(12) . ? N2 Mn1 2.234(4) 3_656 ? C7 O4 1.190(13) . ? N1 C4 1.331(7) 7_565 ? O2 Mn1 2.159(5) 2_655 ? O3 H3WA 0.87(4) . ? O3 H3WB 0.86(4) . ? 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 Mn1 O2 180.000(1) 6_557 2_654 ? O2 Mn1 O1 88.9(2) 6_557 . ? O2 Mn1 O1 91.1(2) 2_654 . ? O2 Mn1 O1 91.1(2) 6_557 5_656 ? O2 Mn1 O1 88.9(2) 2_654 5_656 ? O1 Mn1 O1 180.000(1) . 5_656 ? O2 Mn1 N2 88.5(2) 6_557 5_656 ? O2 Mn1 N2 91.5(2) 2_654 5_656 ? O1 Mn1 N2 87.6(2) . 5_656 ? O1 Mn1 N2 92.4(2) 5_656 5_656 ? O2 Mn1 N2 91.5(2) 6_557 . ? O2 Mn1 N2 88.5(2) 2_654 . ? O1 Mn1 N2 92.4(2) . . ? O1 Mn1 N2 87.6(2) 5_656 . ? N2 Mn1 N2 180.000(1) 5_656 . ? O1 C1 O1 126.7(9) . 7_565 ? O1 C1 C2 116.6(4) . . ? O1 C1 C2 116.6(4) 7_565 . ? C3 C2 C3 118.1(8) 7_565 . ? C3 C2 C1 120.9(4) 7_565 . ? C3 C2 C1 120.9(4) . . ? C2 C3 C4 120.3(7) . . ? C2 C3 H3A 119.8 . . ? C4 C3 H3A 119.8 . . ? N1 C4 C3 120.2(6) . . ? N1 C4 H4A 119.9 . . ? C3 C4 H4A 119.9 . . ? N1 C5 C6 106.4(6) . . ? N1 C5 H5A 110.3 . . ? C6 C5 H5A 109.7 . . ? O2 C6 O2 126.4(8) 7_565 . ? O2 C6 C5 116.8(4) 7_565 . ? O2 C6 C5 116.8(4) . . ? C7 N2 Mn1 122.66(17) . 3_656 ? C7 N2 Mn1 122.66(17) . . ? Mn1 N2 Mn1 114.6(3) 3_656 . ? N2 C7 O4 178.5(14) . . ? C4 N1 C4 120.9(7) . 7_565 ? C4 N1 C5 119.5(4) . . ? C4 N1 C5 119.5(4) 7_565 . ? C1 O1 Mn1 135.0(5) . . ? C6 O2 Mn1 137.0(5) . 2_655 ? H3WA O3 H3WB 109(7) . . ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 27.15 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.604 _refine_diff_density_min -0.614 _refine_diff_density_rms 0.119