# Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2005 data_global _journal_name_full Chem.Commun. _journal_coden_Cambridge 0182 _publ_contact_author_name 'Shilun Qiu' _publ_contact_author_address ; Department of Chemistry Jilin University State Key Lab. of Inorganic Synthesis & Preparative Chemistry Changchun 130012 CHINA ; _publ_contact_author_email sqiu@mail.jlu.edu.cn _publ_contact_author_phone +86-431-5168331 _publ_contact_author_fax +86-431-5168331 _publ_section_title ; A novel chiral layered Co(II) coordination polymer with helical chains from achiral materials ; loop_ _publ_author_name 'Shilun Qiu' 'Qianrong Fang' 'Jinyu Sun' 'Ge Tian' 'Yan Wei' 'Ming Xue' ; Xiaoyu Yang ; 'Guangshan Zhu' data_[Co(PDC)(H2O)2(H2O)] _database_code_depnum_ccdc_archive 'CCDC 252681' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_absolute_configuration unk _chemical_melting_point 'not measured' _chemical_formula_moiety 'C7 H9 Co N O7' _chemical_formula_sum 'C7 H9 Co N O7' _chemical_formula_weight 278.08 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' Co Co 0.3494 0.9721 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M P212121 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 7.363(2) _cell_length_b 9.422(3) _cell_length_c 13.976(4) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 969.6(5) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min 2.61 _cell_measurement_theta_max 23.24 _exptl_crystal_description block _exptl_crystal_colour pink _exptl_crystal_size_max 0.08 _exptl_crystal_size_mid 0.06 _exptl_crystal_size_min 0.04 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.905 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 564 _exptl_absorpt_coefficient_mu 1.792 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.879 _exptl_absorpt_correction_T_max 0.931 _exptl_absorpt_process_details SADABS _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 none _diffrn_standards_interval_count none _diffrn_standards_interval_time none _diffrn_standards_decay_% none _diffrn_reflns_number 2225 _diffrn_reflns_av_R_equivalents 0.0288 _diffrn_reflns_av_sigmaI/netI 0.0405 _diffrn_reflns_limit_h_min -7 _diffrn_reflns_limit_h_max 5 _diffrn_reflns_limit_k_min -9 _diffrn_reflns_limit_k_max 10 _diffrn_reflns_limit_l_min -15 _diffrn_reflns_limit_l_max 9 _diffrn_reflns_theta_min 2.61 _diffrn_reflns_theta_max 23.24 _reflns_number_total 1374 _reflns_number_gt 1300 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker SMART' _computing_cell_refinement 'Bruker SMART' _computing_data_reduction 'Bruker SMART' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'SHELXS-97 (Sheldrick, 1990)' _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^)+(0.0471P)^2^+0.0623P] 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_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.00(3) _refine_ls_number_reflns 1374 _refine_ls_number_parameters 145 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0306 _refine_ls_R_factor_gt 0.0284 _refine_ls_wR_factor_ref 0.0824 _refine_ls_wR_factor_gt 0.0816 _refine_ls_goodness_of_fit_ref 1.113 _refine_ls_restrained_S_all 1.113 _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 C1 C 0.4792(6) 0.7310(5) 0.6754(3) 0.0241(11) Uani 1 1 d . . . H1 H 0.4558 0.8056 0.7172 0.029 Uiso 1 1 calc R . . C2 C 0.6510(7) 0.7209(5) 0.6349(3) 0.0242(11) Uani 1 1 d . . . C3 C 0.6834(7) 0.6098(6) 0.5716(3) 0.0288(11) Uani 1 1 d . . . H3 H 0.7977 0.5986 0.5442 0.035 Uiso 1 1 calc R . . C4 C 0.5441(7) 0.5154(5) 0.5493(4) 0.0283(12) Uani 1 1 d . . . H4 H 0.5623 0.4426 0.5054 0.034 Uiso 1 1 calc R . . C5 C 0.3797(7) 0.5325(5) 0.5937(3) 0.0231(11) Uani 1 1 d . . . C7 C 0.2209(7) 0.4325(5) 0.5782(3) 0.0243(12) Uani 1 1 d . . . C6 C 0.7978(7) 0.8225(5) 0.6636(3) 0.0217(12) Uani 1 1 d . . . N1 N 0.3455(6) 0.6382(4) 0.6571(3) 0.0234(9) Uani 1 1 d . . . O6 O -0.1377(5) 0.5214(4) 0.7926(3) 0.0362(9) Uani 1 1 d . . . O5 O 0.1585(5) 0.7462(3) 0.8439(2) 0.0321(9) Uani 1 1 d . . . O4 O 0.7505(5) 0.9470(3) 0.6833(3) 0.0284(8) Uani 1 1 d . . . O1 O 0.0794(5) 0.4584(3) 0.6257(2) 0.0277(8) Uani 1 1 d . . . O2 O 0.2379(5) 0.3320(3) 0.5205(2) 0.0339(9) Uani 1 1 d . . . O3 O 0.9599(5) 0.7793(3) 0.6658(2) 0.0274(8) Uani 1 1 d . . . O7 O 0.4317(6) 0.0848(5) 0.6105(3) 0.0577(12) Uani 1 1 d . . . Co1 Co 0.09791(8) 0.60542(6) 0.73554(4) 0.0218(2) 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 C1 0.023(3) 0.019(2) 0.030(3) -0.003(2) -0.002(2) -0.005(2) C2 0.024(3) 0.024(3) 0.025(3) 0.001(2) -0.003(2) 0.002(2) C3 0.018(3) 0.034(3) 0.034(3) -0.001(3) 0.006(2) -0.003(3) C4 0.025(3) 0.028(3) 0.031(3) -0.008(2) 0.005(2) -0.001(2) C5 0.026(3) 0.018(2) 0.026(2) -0.0003(19) 0.000(2) 0.003(2) C7 0.027(3) 0.022(3) 0.024(3) 0.001(2) -0.004(2) -0.003(2) C6 0.021(3) 0.023(3) 0.020(2) 0.005(2) 0.001(2) 0.001(2) N1 0.023(2) 0.021(2) 0.026(2) -0.0009(16) 0.0010(17) -0.0001(18) O6 0.029(2) 0.030(2) 0.050(2) 0.0105(16) 0.0111(17) 0.0032(17) O5 0.040(2) 0.0260(18) 0.0304(18) -0.0037(15) -0.0040(16) 0.0076(17) O4 0.0227(19) 0.0192(18) 0.043(2) -0.0040(15) -0.0057(17) 0.0008(16) O1 0.024(2) 0.0245(16) 0.0347(18) -0.0066(14) 0.0038(18) -0.0059(16) O2 0.035(2) 0.0298(19) 0.037(2) -0.0129(17) 0.0051(18) -0.0069(18) O3 0.0194(19) 0.0239(17) 0.0390(19) -0.0007(15) -0.0006(15) 0.0005(16) O7 0.034(2) 0.072(3) 0.067(3) 0.023(2) 0.011(2) -0.004(2) Co1 0.0184(4) 0.0188(3) 0.0280(3) -0.0021(3) 0.0018(3) -0.0001(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 C1 N1 1.341(6) . ? C1 C2 1.389(7) . ? C2 C3 1.391(7) . ? C2 C6 1.498(7) . ? C3 C4 1.393(7) . ? C4 C5 1.370(7) . ? C5 N1 1.357(6) . ? C5 C7 1.517(7) . ? C7 O2 1.249(6) . ? C7 O1 1.260(6) . ? C6 O4 1.255(5) . ? C6 O3 1.261(6) . ? N1 Co1 2.149(4) . ? O6 Co1 2.067(3) . ? O5 Co1 2.062(3) . ? O4 Co1 2.182(3) 3_656 ? O1 Co1 2.072(3) . ? O3 Co1 2.160(3) 1_655 ? Co1 O3 2.160(3) 1_455 ? Co1 O4 2.182(3) 3_646 ? 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 C1 C2 123.1(4) . . ? C1 C2 C3 117.9(4) . . ? C1 C2 C6 120.3(4) . . ? C3 C2 C6 121.8(4) . . ? C2 C3 C4 119.7(4) . . ? C5 C4 C3 118.3(5) . . ? N1 C5 C4 123.1(5) . . ? N1 C5 C7 114.0(4) . . ? C4 C5 C7 122.9(4) . . ? O2 C7 O1 124.7(4) . . ? O2 C7 C5 119.1(4) . . ? O1 C7 C5 116.2(4) . . ? O4 C6 O3 124.0(5) . . ? O4 C6 C2 117.1(4) . . ? O3 C6 C2 118.9(4) . . ? C1 N1 C5 117.8(4) . . ? C1 N1 Co1 128.3(3) . . ? C5 N1 Co1 112.6(3) . . ? C6 O4 Co1 127.7(3) . 3_656 ? C7 O1 Co1 117.7(3) . . ? C6 O3 Co1 134.5(3) . 1_655 ? O5 Co1 O6 98.32(15) . . ? O5 Co1 O1 171.24(14) . . ? O6 Co1 O1 88.53(14) . . ? O5 Co1 N1 95.64(15) . . ? O6 Co1 N1 164.50(14) . . ? O1 Co1 N1 76.97(14) . . ? O5 Co1 O3 86.85(13) . 1_455 ? O6 Co1 O3 93.99(13) . 1_455 ? O1 Co1 O3 98.16(13) . 1_455 ? N1 Co1 O3 93.45(14) . 1_455 ? O5 Co1 O4 86.98(13) . 3_646 ? O6 Co1 O4 88.10(14) . 3_646 ? O1 Co1 O4 87.81(13) . 3_646 ? N1 Co1 O4 85.95(15) . 3_646 ? O3 Co1 O4 173.71(13) 1_455 3_646 ? _diffrn_measured_fraction_theta_max 0.986 _diffrn_reflns_theta_full 23.24 _diffrn_measured_fraction_theta_full 0.986 _refine_diff_density_max 0.372 _refine_diff_density_min -0.186 _refine_diff_density_rms 0.068