# Supplementary Material (ESI) for New Journal of Chemistry # This journal is © The Royal Society of Chemistry and # The Centre National de la Recherche Scientifique, 2002 data_329 _database_code_CSD 189047 _journal_coden_Cambridge 440 _journal_volume ? _journal_year ? _journal_page_first ? _publ_requested_journal 'New Journal of Chemistry' loop_ _publ_author_name 'Chen, Xuetai' 'Li, Yi-Zhi' 'Shi, Yu-Jun' 'Xue, Ziling' 'You, Xiao-Zeng' _publ_contact_author_name 'Dr Xuetai Chen' _publ_contact_author_address ; College of Chemistry and Chemical Engineering Coordination Chemistry Institute Hankou Road 22 Nanjing Jiangsu 210093 CHINA ; _publ_contact_author_email 'XTCHEN@NETRA.NJU.EDU.CN' _publ_section_title ; Pb(dca)2 (dca = dicyanamide): a novel 3D compound with three unprecedented coordination modes of dicyanamide ; _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C4 N6 Pb' _chemical_formula_sum 'C4 N6 Pb' _chemical_formula_weight 339.29 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' 'Pb' 'Pb' -3.3944 10.1111 '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' _symmetry_space_group_name_Hall '-P 2ac 2n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' 'x+1/2, -y+1/2, -z+1/2' '-x, y+1/2, -z' '-x, -y, -z' 'x-1/2, y, -z-1/2' '-x-1/2, y-1/2, z-1/2' 'x, -y-1/2, z' _cell_length_a 13.501(2) _cell_length_b 3.995(1) _cell_length_c 11.980(2) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 646.2(2) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 25 _cell_measurement_theta_min 2.2 _cell_measurement_theta_max 25.0 _exptl_crystal_description ? _exptl_crystal_colour ? _exptl_crystal_size_max 0.15 _exptl_crystal_size_mid 0.11 _exptl_crystal_size_min 0.10 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 3.488 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 592 _exptl_absorpt_coefficient_mu 26.039 _exptl_absorpt_correction_type 'empirical' _exptl_absorpt_correction_T_min 0.044 _exptl_absorpt_correction_T_max 0.075 _exptl_absorpt_process_details 'Bruker SADABS' _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'sealed tube' _diffrn_radiation_monochromator 'graphite' _diffrn_measurement_device_type 'Bruker P4' _diffrn_measurement_method '\w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number 3 _diffrn_standards_interval_count 100 _diffrn_standards_interval_time ? _diffrn_standards_decay_% 0.001 _diffrn_reflns_number 657 _diffrn_reflns_av_R_equivalents 0.0221 _diffrn_reflns_av_sigmaI/netI 0.0227 _diffrn_reflns_limit_h_min 0 _diffrn_reflns_limit_h_max 16 _diffrn_reflns_limit_k_min 0 _diffrn_reflns_limit_k_max 4 _diffrn_reflns_limit_l_min 0 _diffrn_reflns_limit_l_max 14 _diffrn_reflns_theta_min 2.27 _diffrn_reflns_theta_max 24.97 _reflns_number_total 657 _reflns_number_gt 537 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker XSCANS' _computing_cell_refinement 'Bruker XSCANS' _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^)+(0.1180P)^2^+1.9900P] 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 657 _refine_ls_number_parameters 68 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0478 _refine_ls_R_factor_gt 0.0380 _refine_ls_wR_factor_ref 0.1366 _refine_ls_wR_factor_gt 0.1240 _refine_ls_goodness_of_fit_ref 1.002 _refine_ls_restrained_S_all 1.002 _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 Pb1 Pb 0.71407(5) 1.2500 0.38005(5) 0.0177(4) Uani 1 2 d S . . N1 N 1.0669(15) 0.7500 0.1109(12) 0.026(4) Uani 1 2 d S . . N2 N 0.8864(12) 0.7500 0.0866(14) 0.026(4) Uani 1 2 d S . . N3 N 0.7644(12) 0.7500 0.2478(14) 0.026(4) Uani 1 2 d S . . N5 N 1.0927(11) 1.2500 0.3433(14) 0.026(4) Uani 1 2 d S . . N4 N 0.9097(12) 1.2500 0.3573(14) 0.026(4) Uani 1 2 d S . . N6 N 0.7824(10) 0.7500 0.5051(15) 0.026(4) Uani 1 2 d S . . C1 C 0.9797(15) 0.7500 0.1116(15) 0.026(5) Uani 1 2 d S . . C2 C 0.8274(14) 0.7500 0.1734(16) 0.026(4) Uani 1 2 d S . . C3 C 0.9959(16) 1.2500 0.3597(16) 0.026(4) Uani 1 2 d S . . C4 C 0.8467(14) 0.7500 0.5684(16) 0.026(4) Uani 1 2 d S . . 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 Pb1 0.0223(6) 0.0251(6) 0.0056(5) 0.000 0.0013(2) 0.000 N1 0.024(8) 0.047(11) 0.007(7) 0.000 0.004(6) 0.000 N2 0.023(9) 0.047(11) 0.008(8) 0.000 0.005(6) 0.000 N3 0.023(8) 0.047(11) 0.008(8) 0.000 0.004(6) 0.000 N5 0.022(8) 0.045(10) 0.011(8) 0.000 -0.010(6) 0.000 N4 0.022(9) 0.045(11) 0.012(7) 0.000 -0.010(6) 0.000 N6 0.022(8) 0.045(12) 0.011(8) 0.000 -0.010(6) 0.000 C1 0.023(11) 0.047(14) 0.007(9) 0.000 0.005(7) 0.000 C2 0.023(9) 0.047(13) 0.008(9) 0.000 0.004(7) 0.000 C3 0.022(9) 0.045(12) 0.011(9) 0.000 -0.010(8) 0.000 C4 0.022(10) 0.045(12) 0.011(9) 0.000 -0.009(8) 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 Pb1 N3 2.639(11) . ? Pb1 N3 2.639(11) 1_565 ? Pb1 N4 2.655(17) . ? Pb1 N6 2.662(11) 1_565 ? Pb1 N6 2.662(11) . ? Pb1 N1 2.820(14) 6_556 ? Pb1 N1 2.820(14) 6_566 ? Pb1 N2 2.822(17) 2_675 ? Pb1 N5 3.138(17) 6_556 ? Pb1 Pb1 3.9950(10) 1_545 ? Pb1 Pb1 3.9950(10) 1_565 ? N1 C1 1.18(3) . ? N1 Pb1 2.820(14) 6_656 ? N1 Pb1 2.820(14) 6_646 ? N2 C1 1.29(2) . ? N2 C2 1.31(3) . ? N2 Pb1 2.822(17) 2_674 ? N3 C2 1.23(3) . ? N3 Pb1 2.639(11) 1_545 ? N5 C3 1.32(3) . ? N5 C4 1.34(2) 5_776 ? N5 Pb1 3.138(17) 6_656 ? N4 C3 1.16(3) . ? N6 C4 1.15(2) . ? N6 Pb1 2.662(11) 1_545 ? C4 N5 1.34(2) 5_776 ? 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 N3 Pb1 N3 98.4(5) . 1_565 ? N3 Pb1 N4 71.5(4) . . ? N3 Pb1 N4 71.5(4) 1_565 . ? N3 Pb1 N6 144.8(5) . 1_565 ? N3 Pb1 N6 71.4(5) 1_565 1_565 ? N4 Pb1 N6 73.3(4) . 1_565 ? N3 Pb1 N6 71.4(5) . . ? N3 Pb1 N6 144.8(5) 1_565 . ? N4 Pb1 N6 73.3(4) . . ? N6 Pb1 N6 97.3(5) 1_565 . ? N3 Pb1 N1 70.6(4) . 6_556 ? N3 Pb1 N1 137.8(5) 1_565 6_556 ? N4 Pb1 N1 134.8(3) . 6_556 ? N6 Pb1 N1 139.0(5) 1_565 6_556 ? N6 Pb1 N1 72.0(4) . 6_556 ? N3 Pb1 N1 137.8(5) . 6_566 ? N3 Pb1 N1 70.6(4) 1_565 6_566 ? N4 Pb1 N1 134.8(3) . 6_566 ? N6 Pb1 N1 72.0(4) 1_565 6_566 ? N6 Pb1 N1 139.0(5) . 6_566 ? N1 Pb1 N1 90.2(6) 6_556 6_566 ? N3 Pb1 N2 130.6(3) . 2_675 ? N3 Pb1 N2 130.6(3) 1_565 2_675 ? N4 Pb1 N2 124.6(5) . 2_675 ? N6 Pb1 N2 70.9(4) 1_565 2_675 ? N6 Pb1 N2 70.9(4) . 2_675 ? N1 Pb1 N2 68.1(4) 6_556 2_675 ? N1 Pb1 N2 68.1(4) 6_566 2_675 ? N3 Pb1 N5 67.8(4) . 6_556 ? N3 Pb1 N5 67.8(4) 1_565 6_556 ? N4 Pb1 N5 115.6(5) . 6_556 ? N6 Pb1 N5 131.4(3) 1_565 6_556 ? N6 Pb1 N5 131.4(3) . 6_556 ? N1 Pb1 N5 70.4(3) 6_556 6_556 ? N1 Pb1 N5 70.4(3) 6_566 6_556 ? N2 Pb1 N5 119.8(5) 2_675 6_556 ? N3 Pb1 Pb1 40.8(3) . 1_545 ? N3 Pb1 Pb1 139.2(3) 1_565 1_545 ? N4 Pb1 Pb1 90.0 . 1_545 ? N6 Pb1 Pb1 138.6(3) 1_565 1_545 ? N6 Pb1 Pb1 41.4(3) . 1_545 ? N1 Pb1 Pb1 44.9(3) 6_556 1_545 ? N1 Pb1 Pb1 135.1(3) 6_566 1_545 ? N2 Pb1 Pb1 90.000(1) 2_675 1_545 ? N5 Pb1 Pb1 90.000(1) 6_556 1_545 ? N3 Pb1 Pb1 139.2(3) . 1_565 ? N3 Pb1 Pb1 40.8(3) 1_565 1_565 ? N4 Pb1 Pb1 90.0 . 1_565 ? N6 Pb1 Pb1 41.4(3) 1_565 1_565 ? N6 Pb1 Pb1 138.6(3) . 1_565 ? N1 Pb1 Pb1 135.1(3) 6_556 1_565 ? N1 Pb1 Pb1 44.9(3) 6_566 1_565 ? N2 Pb1 Pb1 90.000(1) 2_675 1_565 ? N5 Pb1 Pb1 90.000(1) 6_556 1_565 ? Pb1 Pb1 Pb1 180.0 1_545 1_565 ? C1 N1 Pb1 134.8(3) . 6_656 ? C1 N1 Pb1 134.8(3) . 6_646 ? Pb1 N1 Pb1 90.2(6) 6_656 6_646 ? C1 N2 C2 114.1(18) . . ? C1 N2 Pb1 132.1(13) . 2_674 ? C2 N2 Pb1 113.8(13) . 2_674 ? C2 N3 Pb1 127.7(5) . . ? C2 N3 Pb1 127.7(5) . 1_545 ? Pb1 N3 Pb1 98.4(5) . 1_545 ? C3 N5 C4 119.2(18) . 5_776 ? C3 N5 Pb1 130.0(13) . 6_656 ? C4 N5 Pb1 110.8(12) 5_776 6_656 ? C3 N4 Pb1 172.7(15) . . ? C4 N6 Pb1 129.1(4) . 1_545 ? C4 N6 Pb1 129.1(4) . . ? Pb1 N6 Pb1 97.3(5) 1_545 . ? N1 C1 N2 166.2(19) . . ? N3 C2 N2 174(2) . . ? N4 C3 N5 170(2) . . ? N6 C4 N5 169(2) . 5_776 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 24.97 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 2.781 _refine_diff_density_min -2.319 _refine_diff_density_rms 0.349