# Electronic Supplementary Material (ESI) for CrystEngComm # This journal is © The Royal Society of Chemistry 2011 data_global _journal_name_full CrystEngComm _journal_coden_cambridge 1350 _journal_year ? _journal_volume ? _journal_page_first ? loop_ _publ_author_name 'Yunqi Tian' 'Chun-Jie Jiang' _publ_contact_author_name 'Yan-Tao Li' _publ_contact_author_email 111lyt@163.com data_CdIF-13 _database_code_depnum_ccdc_archive 'CCDC 801236' #TrackingRef '- CdIF-13.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common 'cadmium 2-nitroimidazolate' _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C4.50 H3 Cd0.75 N4.50 O3' _chemical_formula_weight 252.41 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' Cd Cd -0.8075 1.2024 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting tetragonal _symmetry_space_group_name_H-M I-42d loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' 'y, -x, -z' '-y, x, -z' '-x+1/2, y, -z+3/4' 'x+1/2, -y, -z+3/4' '-y+1/2, -x, z+3/4' 'y+1/2, x, z+3/4' 'x+1/2, y+1/2, z+1/2' '-x+1/2, -y+1/2, z+1/2' 'y+1/2, -x+1/2, -z+1/2' '-y+1/2, x+1/2, -z+1/2' '-x+1, y+1/2, -z+5/4' 'x+1, -y+1/2, -z+5/4' '-y+1, -x+1/2, z+5/4' 'y+1, x+1/2, z+5/4' _cell_length_a 18.0847(8) _cell_length_b 18.0847(8) _cell_length_c 9.9217(9) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 3245.0(4) _cell_formula_units_Z 16 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 89 _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description prism _exptl_crystal_colour 'pale yellow' _exptl_crystal_size_max 0.80 _exptl_crystal_size_mid 0.05 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.067 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1944 _exptl_absorpt_coefficient_mu 2.034 _exptl_absorpt_correction_type 'empirical used sadabs' _exptl_absorpt_correction_T_min 0.2930 _exptl_absorpt_correction_T_max 0.9052 _exptl_absorpt_process_details '(SADABS; Bruker, 2000)' _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 'Bruker Apex-II Smart CCDC' _diffrn_measurement_method 'omega scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time '10 sec.' _diffrn_standards_decay_% ? _diffrn_reflns_number 10045 _diffrn_reflns_av_R_equivalents 0.0395 _diffrn_reflns_av_sigmaI/netI 0.0354 _diffrn_reflns_limit_h_min -24 _diffrn_reflns_limit_h_max 14 _diffrn_reflns_limit_k_min -24 _diffrn_reflns_limit_k_max 24 _diffrn_reflns_limit_l_min -13 _diffrn_reflns_limit_l_max 13 _diffrn_reflns_theta_min 2.25 _diffrn_reflns_theta_max 29.17 _reflns_number_total 2072 _reflns_number_gt 1826 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'SMART (Bruker, 1997)' _computing_cell_refinement 'SAINT (Bruker, 1999)' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _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. There are still solvent accessible void of 9.9% of the crystal, which merely the water molecules are accessile to. ; _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^)+(0.0513P)^2^+0.0000P] 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 -0.05(4) _refine_ls_number_reflns 2072 _refine_ls_number_parameters 117 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0338 _refine_ls_R_factor_gt 0.0255 _refine_ls_wR_factor_ref 0.0668 _refine_ls_wR_factor_gt 0.0623 _refine_ls_goodness_of_fit_ref 0.812 _refine_ls_restrained_S_all 0.812 _refine_ls_shift/su_max 0.001 _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 Cd1 Cd 0.5000 0.5000 0.5000 0.03050(13) Uani 1 4 d S . . Cd2 Cd 0.2500 0.63769(2) 0.8750 0.03318(11) Uani 1 2 d S . . O1 O 0.48691(16) 0.57683(17) 0.7510(4) 0.0497(7) Uani 1 1 d . . . O2 O 0.40194(19) 0.5947(2) 0.9010(3) 0.0592(9) Uani 1 1 d . . . O3 O 0.35157(16) 0.78333(18) 0.5341(3) 0.0475(8) Uani 1 1 d . . . N1 N 0.38549(18) 0.51700(18) 0.5817(3) 0.0359(7) Uani 1 1 d . . . N2 N 0.29568(17) 0.55822(19) 0.7207(3) 0.0389(8) Uani 1 1 d . . . N3 N 0.20154(19) 0.7123(2) 0.7163(4) 0.0457(9) Uani 1 1 d . . . N4 N 0.4219(2) 0.57464(19) 0.7894(3) 0.0403(8) Uani 1 1 d . . . C1 C 0.3678(2) 0.5490(2) 0.6974(4) 0.0340(8) Uani 1 1 d . . . C2 C 0.3184(2) 0.5040(3) 0.5250(4) 0.0482(11) Uani 1 1 d . . . H2A H 0.3107 0.4812 0.4422 0.058 Uiso 1 1 calc R . . C3 C 0.2641(2) 0.5295(2) 0.6083(5) 0.0477(10) Uani 1 1 d . . . H3A H 0.2136 0.5276 0.5908 0.057 Uiso 1 1 calc R . . N5 N 0.3190(2) 0.7500 0.6250 0.0342(9) Uani 1 2 d S . . C4 C 0.2404(3) 0.7500 0.6250 0.0356(11) Uani 1 2 d S . . C5 C 0.1312(2) 0.7274(4) 0.6804(6) 0.0693(18) Uani 1 1 d . . . H5A H 0.0892 0.7098 0.7241 0.083 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 Cd1 0.03022(17) 0.03022(17) 0.0311(3) 0.000 0.000 0.000 Cd2 0.0345(2) 0.0370(2) 0.02808(18) 0.000 0.00387(16) 0.000 O1 0.0369(16) 0.0551(18) 0.0570(18) -0.0089(16) -0.0042(15) 0.0011(12) O2 0.063(2) 0.077(2) 0.0380(18) -0.0180(16) -0.0013(15) 0.0128(18) O3 0.0408(16) 0.0489(17) 0.0527(19) 0.0144(15) 0.0117(14) 0.0006(13) N1 0.0349(16) 0.0391(18) 0.0337(17) -0.0052(13) 0.0076(13) -0.0048(14) N2 0.0349(17) 0.0421(18) 0.0397(18) -0.0061(15) 0.0077(15) -0.0015(13) N3 0.0339(17) 0.058(2) 0.045(2) 0.0217(17) 0.0057(15) 0.0030(16) N4 0.046(2) 0.0358(17) 0.0391(19) -0.0040(15) -0.0012(16) 0.0079(15) C1 0.039(2) 0.0315(19) 0.0315(19) 0.0035(15) 0.0047(16) -0.0025(16) C2 0.038(2) 0.061(3) 0.045(2) -0.021(2) 0.0042(18) -0.005(2) C3 0.037(2) 0.057(2) 0.050(3) -0.013(2) 0.006(2) -0.0091(18) N5 0.036(2) 0.033(2) 0.034(2) 0.002(2) 0.000 0.000 C4 0.032(3) 0.040(3) 0.035(3) 0.007(2) 0.000 0.000 C5 0.031(2) 0.090(4) 0.087(4) 0.051(3) 0.007(2) 0.005(2) _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 Cd1 N1 2.245(3) 4_656 ? Cd1 N1 2.245(3) 2_665 ? Cd1 N1 2.245(3) 3_566 ? Cd1 N1 2.245(3) . ? Cd2 N3 2.252(3) 5_556 ? Cd2 N3 2.252(3) . ? Cd2 N2 2.256(3) . ? Cd2 N2 2.256(3) 5_556 ? O1 N4 1.236(5) . ? O2 N4 1.220(4) . ? O3 N5 1.235(3) . ? N1 C1 1.325(5) . ? N1 C2 1.357(5) . ? N2 C1 1.335(5) . ? N2 C3 1.356(5) . ? N3 C4 1.334(4) . ? N3 C5 1.349(5) . ? N4 C1 1.416(5) . ? C2 C3 1.365(6) . ? C2 H2A 0.9300 . ? C3 H3A 0.9300 . ? N5 O3 1.235(3) 14_465 ? N5 C4 1.420(7) . ? C4 N3 1.334(4) 14_465 ? C5 C5 1.370(10) 14_465 ? C5 H5A 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 N1 Cd1 N1 97.49(6) 4_656 2_665 ? N1 Cd1 N1 137.68(17) 4_656 3_566 ? N1 Cd1 N1 97.49(6) 2_665 3_566 ? N1 Cd1 N1 97.49(6) 4_656 . ? N1 Cd1 N1 137.68(17) 2_665 . ? N1 Cd1 N1 97.49(6) 3_566 . ? N3 Cd2 N3 106.3(2) 5_556 . ? N3 Cd2 N2 135.54(12) 5_556 . ? N3 Cd2 N2 92.86(13) . . ? N3 Cd2 N2 92.86(13) 5_556 5_556 ? N3 Cd2 N2 135.54(12) . 5_556 ? N2 Cd2 N2 100.88(18) . 5_556 ? C1 N1 C2 102.7(3) . . ? C1 N1 Cd1 126.5(3) . . ? C2 N1 Cd1 130.6(3) . . ? C1 N2 C3 102.8(3) . . ? C1 N2 Cd2 123.7(3) . . ? C3 N2 Cd2 130.3(3) . . ? C4 N3 C5 102.4(4) . . ? C4 N3 Cd2 125.2(3) . . ? C5 N3 Cd2 132.3(3) . . ? O2 N4 O1 123.5(4) . . ? O2 N4 C1 118.5(4) . . ? O1 N4 C1 118.0(3) . . ? N1 C1 N2 116.1(4) . . ? N1 C1 N4 122.3(4) . . ? N2 C1 N4 121.5(3) . . ? N1 C2 C3 109.5(4) . . ? N1 C2 H2A 125.2 . . ? C3 C2 H2A 125.2 . . ? N2 C3 C2 108.9(4) . . ? N2 C3 H3A 125.6 . . ? C2 C3 H3A 125.6 . . ? O3 N5 O3 122.9(4) . 14_465 ? O3 N5 C4 118.5(2) . . ? O3 N5 C4 118.5(2) 14_465 . ? N3 C4 N3 116.4(5) 14_465 . ? N3 C4 N5 121.8(2) 14_465 . ? N3 C4 N5 121.8(2) . . ? N3 C5 C5 109.4(3) . 14_465 ? N3 C5 H5A 125.3 . . ? C5 C5 H5A 125.3 14_465 . ? _diffrn_measured_fraction_theta_max 0.958 _diffrn_reflns_theta_full 29.17 _diffrn_measured_fraction_theta_full 0.958 _refine_diff_density_max 0.292 _refine_diff_density_min -0.268 _refine_diff_density_rms 0.062