# Electronic Supplementary Material (ESI) for CrystEngComm # This journal is © The Royal Society of Chemistry 2011 data_General _journal_name_full CrystEngComm _journal_coden_cambridge 1350 #TrackingRef '- JPLangCIF.CIF' _audit_creation_date 2010-3-20 _audit_creation_method 'by CrystalStructure 3.6.0' _audit_update_record ? #============================================================================== # PROCESSING SUMMARY (IUCr Office Use Only) _journal_date_recd_electronic ? _journal_date_from_coeditor ? _journal_date_accepted ? _journal_coeditor_code ? #============================================================================== # SUBMISSION DETAILS _publ_contact_author_name 'Jian-Ping Lang' _publ_contact_author_address ; College of Chemistry, Chemical Engineering and Materials Science Soochow University Suzhou 215123, Jiangsu P.R.China ; _publ_contact_author_email jplang@suda.edu.cn _publ_contact_author_fax 86-512-65880089 _publ_contact_author_phone 86-512-65882865 _publ_contact_letter ; ENTER TEXT OF LETTER ; _publ_requested_category FM _publ_requested_coeditor_name ? #============================================================================== # TITLE AND AUTHOR LIST _publ_section_title ; ENTER SECTION TITLE ; _publ_section_title_footnote ; ENTER FOOTNOTE TO TITLE OF PAPER ; loop_ _publ_author_name _publ_author_footnote _publ_author_address 'Henry Chan' ; FIRST AUTHORS FOOTNOTES ; ; FIRST AUTHORS ADDRESS ; 'Yang Chen' '' '' 'Ming Dai' '' '' 'Hui-Fang Wang' '' '' 'Zhi-Gang Ren' '' '' 'Zheng-Jun Huang' '' '' 'Chun-Yan Ni' '' '' 'Jian-Ping Lang' '' '' _publ_section_synopsis ; ENTER SYNOPSIS ; #============================================================================== # TEXT _publ_section_abstract ; ENTER ABSTRACT ; _publ_section_comment ; ENTER TEXT ; _publ_section_references ; ENTER OTHER REFERENCES Rigaku/MSC and Rigaku Corporation. (2004). CrystalStructure 3.6.0. Single Crystal Structure Analysis Software. Rigaku/MSC, 9009 New Trails Drive, The Woodlands, TX, USA 77381-5209. Rigaku, 3-9-12 Akishima, Tokyo 196-8666, Japan. Watkin, D.J., Prout, C.K. Carruthers, J.R. & Betteridge, P.W. (1996) CRYSTALS Issue 10, Chemical Crystallography Laboratory, Oxford, UK. ; _publ_section_figure_captions ; ENTER FIGURE CAPTIONS ; _publ_section_exptl_prep ; ENTER COMPOUND PREPARATION DETAILS ; _publ_section_exptl_refinement ; ENTER SPECIAL DETAILS OF THE REFINEMENT ; #========================================================================== data_1 _database_code_depnum_ccdc_archive 'CCDC 830727' #TrackingRef '- JPLangCIF.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'Cu4 I6, 2(C7 H7 N2)' _chemical_formula_sum 'C14 H14 Cu4 I6 N4' _chemical_formula_weight 1253.89 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' Cu Cu 0.3201 1.2651 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Orthorhombic _symmetry_space_group_name_H-M 'P 21 21 21' _symmetry_space_group_name_Hall 'P 2ac 2ab' 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 10.507(2) _cell_length_b 10.643(2) _cell_length_c 23.510(5) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 2629.0(9) _cell_formula_units_Z 4 _cell_measurement_temperature 223(2) _cell_measurement_reflns_used 10568 _cell_measurement_theta_min 3.2280 _cell_measurement_theta_max 27.6217 _exptl_crystal_description Block _exptl_crystal_colour Black _exptl_crystal_size_max 0.24 _exptl_crystal_size_mid 0.23 _exptl_crystal_size_min 0.22 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 3.168 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2240 _exptl_absorpt_coefficient_mu 10.247 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.107 _exptl_absorpt_correction_T_max 0.115 _exptl_absorpt_process_details 'Jacobson, R. (1998) Private communication to Rigaku Company, Tokyo, Japan.' _exptl_special_details ; ? ; _diffrn_ambient_temperature 223(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 MercuryCCD area detector' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 13142 _diffrn_reflns_av_R_equivalents 0.0640 _diffrn_reflns_av_sigmaI/netI 0.0896 _diffrn_reflns_limit_h_min -13 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -11 _diffrn_reflns_limit_k_max 13 _diffrn_reflns_limit_l_min -24 _diffrn_reflns_limit_l_max 30 _diffrn_reflns_theta_min 3.23 _diffrn_reflns_theta_max 27.49 _reflns_number_total 5733 _reflns_number_gt 4762 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_cell_refinement 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_data_reduction 'CrystalStructure, Ver. 3.60 (Rigaku/MSC, 2004)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'ORTEPII (Johnson, 1976)' _computing_publication_material SHELXL97 _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^)+(0.0633P)^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 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 -0.16(10) _refine_ls_number_reflns 5733 _refine_ls_number_parameters 232 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0618 _refine_ls_R_factor_gt 0.0523 _refine_ls_wR_factor_ref 0.1349 _refine_ls_wR_factor_gt 0.1217 _refine_ls_goodness_of_fit_ref 1.003 _refine_ls_restrained_S_all 1.003 _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 Cu1 Cu 0.4099(3) 0.8031(3) 0.57702(10) 0.0520(6) Uani 1 1 d . . . Cu2 Cu 0.5957(2) 0.8172(3) 0.67927(10) 0.0518(6) Uani 1 1 d . . . Cu3 Cu 0.4407(2) 0.5959(3) 0.66944(10) 0.0508(6) Uani 1 1 d . . . Cu4 Cu 0.6328(3) 0.6515(2) 0.57611(10) 0.0501(6) Uani 1 1 d . . . I1 I 0.64993(12) 0.89822(12) 0.57430(5) 0.0405(3) Uani 1 1 d . . . I2 I 0.34394(11) 0.82916(12) 0.68649(5) 0.0412(3) Uani 1 1 d . . . I3 I 0.39641(12) 0.55709(13) 0.55817(5) 0.0420(3) Uani 1 1 d . . . I4 I 0.69190(11) 0.57961(12) 0.68282(5) 0.0413(3) Uani 1 1 d . . . I5 I 0.27822(12) 0.94162(13) 0.50486(5) 0.0452(3) Uani 1 1 d . . . I6 I 0.69401(12) 0.95046(13) 0.76294(5) 0.0444(3) Uani 1 1 d . . . N2 N 0.484(3) 0.368(3) 0.3143(9) 0.098(9) Uani 1 1 d . . . N4 N 0.921(3) 1.250(3) 0.5672(10) 0.093(8) Uani 1 1 d . . . N1 N 0.5273(13) 0.8477(13) 0.3774(6) 0.082(8) Uani 1 1 d G . . C1 C 0.5153(13) 0.8176(15) 0.3201(5) 0.061(7) Uani 1 1 d G . . H1 H 0.5178 0.8815 0.2925 0.073 Uiso 1 1 calc R . . C2 C 0.4997(14) 0.6931(16) 0.3036(4) 0.075(8) Uani 1 1 d G . . H2 H 0.4916 0.6728 0.2649 0.090 Uiso 1 1 calc R . . C3 C 0.4960(14) 0.5987(13) 0.3445(6) 0.060(6) Uani 1 1 d G . . C4 C 0.5080(14) 0.6288(14) 0.4017(5) 0.075(8) Uani 1 1 d G . . H4 H 0.5055 0.5650 0.4294 0.090 Uiso 1 1 calc R . . C5 C 0.5236(14) 0.7533(16) 0.4182(4) 0.063(7) Uani 1 1 d G . . H5 H 0.5317 0.7737 0.4569 0.075 Uiso 1 1 calc R . . C6 C 0.489(3) 0.469(3) 0.3278(11) 0.069(8) Uani 1 1 d . . . C7 C 0.547(3) 0.980(3) 0.3914(11) 0.088(10) Uani 1 1 d . . . H7A H 0.5345 1.0306 0.3576 0.132 Uiso 1 1 calc R . . H7B H 0.6322 0.9917 0.4058 0.132 Uiso 1 1 calc R . . H7C H 0.4856 1.0050 0.4203 0.132 Uiso 1 1 calc R . . N3 N 0.4252(12) 1.1976(13) 0.6248(5) 0.073(7) Uani 1 1 d G . . C8 C 0.5179(15) 1.1933(13) 0.6670(4) 0.065(7) Uani 1 1 d G . . H8 H 0.4948 1.1759 0.7048 0.078 Uiso 1 1 calc R . . C9 C 0.6447(14) 1.2147(14) 0.6532(5) 0.063(6) Uani 1 1 d G . . H9 H 0.7074 1.2118 0.6817 0.075 Uiso 1 1 calc R . . C10 C 0.6788(12) 1.2404(14) 0.5973(6) 0.064(6) Uani 1 1 d G . . C11 C 0.5861(15) 1.2447(13) 0.5551(4) 0.056(6) Uani 1 1 d G . . H11 H 0.6092 1.2621 0.5173 0.067 Uiso 1 1 calc R . . C12 C 0.4593(14) 1.2233(13) 0.5689(5) 0.073(8) Uani 1 1 d G . . H12 H 0.3967 1.2262 0.5404 0.088 Uiso 1 1 calc R . . C13 C 0.820(3) 1.250(3) 0.5806(12) 0.083(9) Uani 1 1 d . . . C14 C 0.299(2) 1.175(3) 0.6383(9) 0.069(7) Uani 1 1 d . . . H14A H 0.2948 1.1211 0.6715 0.104 Uiso 1 1 calc R . . H14B H 0.2574 1.1348 0.6065 0.104 Uiso 1 1 calc R . . H14C H 0.2572 1.2544 0.6466 0.104 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 0.0584(15) 0.0549(16) 0.0426(13) -0.0012(12) -0.0009(12) 0.0009(13) Cu2 0.0519(14) 0.0602(17) 0.0431(13) -0.0027(12) 0.0015(12) -0.0005(13) Cu3 0.0506(14) 0.0595(17) 0.0423(13) 0.0006(11) -0.0016(11) -0.0034(13) Cu4 0.0586(15) 0.0480(14) 0.0437(13) -0.0025(11) 0.0030(11) 0.0031(12) I1 0.0471(7) 0.0399(6) 0.0343(5) -0.0006(5) 0.0043(5) -0.0021(5) I2 0.0433(6) 0.0473(7) 0.0331(5) -0.0015(5) 0.0017(5) 0.0036(6) I3 0.0490(6) 0.0459(7) 0.0312(5) -0.0018(5) -0.0017(5) -0.0039(6) I4 0.0426(6) 0.0472(7) 0.0340(5) 0.0028(5) 0.0005(5) 0.0029(5) I5 0.0524(7) 0.0455(7) 0.0378(6) -0.0019(6) -0.0079(5) -0.0020(6) I6 0.0470(7) 0.0478(7) 0.0383(6) -0.0057(6) 0.0000(5) 0.0016(6) N2 0.14(2) 0.11(2) 0.047(12) -0.006(14) 0.003(14) 0.02(2) N4 0.13(2) 0.09(2) 0.060(14) 0.011(13) -0.005(16) -0.007(19) N1 0.038(10) 0.15(3) 0.054(12) 0.010(14) 0.009(9) 0.008(13) C1 0.029(9) 0.12(2) 0.035(10) -0.001(12) -0.007(9) 0.006(12) C2 0.070(16) 0.13(3) 0.029(11) -0.003(14) 0.001(10) 0.002(17) C3 0.045(11) 0.084(19) 0.052(12) -0.002(13) -0.007(10) 0.003(12) C4 0.057(14) 0.12(2) 0.046(12) -0.003(14) 0.013(11) 0.036(16) C5 0.066(14) 0.085(19) 0.037(11) 0.000(12) 0.001(10) 0.022(14) C6 0.079(17) 0.073(19) 0.055(14) 0.034(13) -0.028(13) -0.008(15) C7 0.067(17) 0.12(3) 0.076(17) -0.040(18) 0.004(14) -0.020(18) N3 0.14(2) 0.043(11) 0.034(9) -0.012(8) 0.004(11) 0.012(12) C8 0.12(2) 0.056(14) 0.024(9) -0.006(9) -0.008(11) 0.021(14) C9 0.077(16) 0.058(14) 0.053(12) 0.011(11) -0.005(12) 0.024(13) C10 0.090(18) 0.041(12) 0.059(14) 0.015(10) -0.001(13) -0.014(13) C11 0.063(14) 0.035(11) 0.070(15) 0.011(10) 0.005(12) -0.009(10) C12 0.13(2) 0.055(14) 0.039(12) -0.008(11) -0.019(13) 0.008(16) C13 0.10(2) 0.09(2) 0.058(16) 0.015(14) 0.009(16) 0.01(2) C14 0.085(18) 0.073(17) 0.049(13) -0.008(12) 0.014(12) 0.002(15) _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 I5 2.639(3) . ? Cu1 I3 2.659(3) . ? Cu1 I2 2.679(3) . ? Cu1 I1 2.719(3) . ? Cu1 Cu4 2.845(4) . ? Cu2 I6 2.636(3) . ? Cu2 I2 2.654(3) . ? Cu2 I1 2.675(3) . ? Cu2 I4 2.725(3) . ? Cu2 Cu3 2.873(4) . ? Cu2 Cu4 3.024(4) . ? Cu3 I6 2.632(3) 3_646 ? Cu3 I4 2.664(3) . ? Cu3 I3 2.689(3) . ? Cu3 I2 2.712(3) . ? Cu3 Cu4 3.040(4) . ? Cu4 I1 2.633(3) . ? Cu4 I5 2.634(3) 4_566 ? Cu4 I4 2.695(3) . ? Cu4 I3 2.712(3) . ? I5 Cu4 2.634(3) 4_466 ? I6 Cu3 2.632(3) 3_656 ? N2 C6 1.12(3) . ? N4 C13 1.11(4) . ? N1 C1 1.3900 . ? N1 C5 1.3900 . ? N1 C7 1.46(3) . ? C1 C2 1.3900 . ? C1 H1 0.9400 . ? C2 C3 1.3900 . ? C2 H2 0.9400 . ? C3 C4 1.3900 . ? C3 C6 1.43(3) . ? C4 C5 1.3900 . ? C4 H4 0.9400 . ? C5 H5 0.9400 . ? C7 H7A 0.9700 . ? C7 H7B 0.9700 . ? C7 H7C 0.9700 . ? N3 C14 1.38(3) . ? N3 C8 1.3900 . ? N3 C12 1.3900 . ? C8 C9 1.3900 . ? C8 H8 0.9400 . ? C9 C10 1.3900 . ? C9 H9 0.9400 . ? C10 C11 1.3900 . ? C10 C13 1.54(4) . ? C11 C12 1.3900 . ? C11 H11 0.9400 . ? C12 H12 0.9400 . ? C14 H14A 0.9700 . ? C14 H14B 0.9700 . ? C14 H14C 0.9700 . ? 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 I5 Cu1 I3 114.52(10) . . ? I5 Cu1 I2 115.10(11) . . ? I3 Cu1 I2 104.37(10) . . ? I5 Cu1 I1 105.26(10) . . ? I3 Cu1 I1 114.32(11) . . ? I2 Cu1 I1 102.94(9) . . ? I5 Cu1 Cu4 138.04(11) . . ? I3 Cu1 Cu4 58.93(9) . . ? I2 Cu1 Cu4 106.19(10) . . ? I1 Cu1 Cu4 56.43(8) . . ? I6 Cu2 I2 108.49(10) . . ? I6 Cu2 I1 115.56(11) . . ? I2 Cu2 I1 104.83(9) . . ? I6 Cu2 I4 109.33(9) . . ? I2 Cu2 I4 114.36(11) . . ? I1 Cu2 I4 104.38(9) . . ? I6 Cu2 Cu3 136.33(11) . . ? I2 Cu2 Cu3 58.63(9) . . ? I1 Cu2 Cu3 108.10(10) . . ? I4 Cu2 Cu3 56.76(8) . . ? I6 Cu2 Cu4 149.51(12) . . ? I2 Cu2 Cu4 102.00(10) . . ? I1 Cu2 Cu4 54.60(7) . . ? I4 Cu2 Cu4 55.62(7) . . ? Cu3 Cu2 Cu4 61.99(9) . . ? I6 Cu3 I4 115.04(10) 3_646 . ? I6 Cu3 I3 113.85(10) 3_646 . ? I4 Cu3 I3 106.04(10) . . ? I6 Cu3 I2 104.33(10) 3_646 . ? I4 Cu3 I2 114.42(11) . . ? I3 Cu3 I2 102.68(9) . . ? I6 Cu3 Cu2 137.60(11) 3_646 . ? I4 Cu3 Cu2 58.81(8) . . ? I3 Cu3 Cu2 107.59(10) . . ? I2 Cu3 Cu2 56.64(8) . . ? I6 Cu3 Cu4 155.18(13) 3_646 . ? I4 Cu3 Cu4 55.93(7) . . ? I3 Cu3 Cu4 56.12(7) . . ? I2 Cu3 Cu4 100.22(10) . . ? Cu2 Cu3 Cu4 61.45(9) . . ? I1 Cu4 I5 108.90(10) . 4_566 ? I1 Cu4 I4 106.40(9) . . ? I5 Cu4 I4 115.62(10) 4_566 . ? I1 Cu4 I3 115.43(11) . . ? I5 Cu4 I3 106.23(9) 4_566 . ? I4 Cu4 I3 104.51(9) . . ? I1 Cu4 Cu1 59.36(8) . . ? I5 Cu4 Cu1 134.14(11) 4_566 . ? I4 Cu4 Cu1 110.10(10) . . ? I3 Cu4 Cu1 57.12(8) . . ? I1 Cu4 Cu2 55.94(8) . . ? I5 Cu4 Cu2 150.89(12) 4_566 . ? I4 Cu4 Cu2 56.54(7) . . ? I3 Cu4 Cu2 102.85(10) . . ? Cu1 Cu4 Cu2 63.69(9) . . ? I1 Cu4 Cu3 104.54(10) . . ? I5 Cu4 Cu3 146.47(12) 4_566 . ? I4 Cu4 Cu3 54.96(7) . . ? I3 Cu4 Cu3 55.38(7) . . ? Cu1 Cu4 Cu3 63.77(9) . . ? Cu2 Cu4 Cu3 56.56(8) . . ? Cu4 I1 Cu2 69.46(8) . . ? Cu4 I1 Cu1 64.21(9) . . ? Cu2 I1 Cu1 70.17(8) . . ? Cu2 I2 Cu1 71.10(8) . . ? Cu2 I2 Cu3 64.73(9) . . ? Cu1 I2 Cu3 70.52(8) . . ? Cu1 I3 Cu3 71.19(9) . . ? Cu1 I3 Cu4 63.95(9) . . ? Cu3 I3 Cu4 68.50(8) . . ? Cu3 I4 Cu4 69.11(8) . . ? Cu3 I4 Cu2 64.43(9) . . ? Cu4 I4 Cu2 67.83(8) . . ? Cu4 I5 Cu1 123.95(10) 4_466 . ? Cu3 I6 Cu2 123.81(9) 3_656 . ? C1 N1 C5 120.0 . . ? C1 N1 C7 117.0(15) . . ? C5 N1 C7 123.0(15) . . ? N1 C1 C2 120.0 . . ? N1 C1 H1 120.0 . . ? C2 C1 H1 120.0 . . ? C3 C2 C1 120.0 . . ? C3 C2 H2 120.0 . . ? C1 C2 H2 120.0 . . ? C2 C3 C4 120.0 . . ? C2 C3 C6 120.4(13) . . ? C4 C3 C6 119.4(13) . . ? C5 C4 C3 120.0 . . ? C5 C4 H4 120.0 . . ? C3 C4 H4 120.0 . . ? C4 C5 N1 120.0 . . ? C4 C5 H5 120.0 . . ? N1 C5 H5 120.0 . . ? N2 C6 C3 179(4) . . ? N1 C7 H7A 109.5 . . ? N1 C7 H7B 109.5 . . ? H7A C7 H7B 109.5 . . ? N1 C7 H7C 109.5 . . ? H7A C7 H7C 109.5 . . ? H7B C7 H7C 109.5 . . ? C14 N3 C8 120.1(14) . . ? C14 N3 C12 119.9(14) . . ? C8 N3 C12 120.0 . . ? N3 C8 C9 120.0 . . ? N3 C8 H8 120.0 . . ? C9 C8 H8 120.0 . . ? C10 C9 C8 120.0 . . ? C10 C9 H9 120.0 . . ? C8 C9 H9 120.0 . . ? C9 C10 C11 120.0 . . ? C9 C10 C13 120.2(14) . . ? C11 C10 C13 119.5(14) . . ? C12 C11 C10 120.0 . . ? C12 C11 H11 120.0 . . ? C10 C11 H11 120.0 . . ? C11 C12 N3 120.0 . . ? C11 C12 H12 120.0 . . ? N3 C12 H12 120.0 . . ? N4 C13 C10 176(4) . . ? N3 C14 H14A 109.5 . . ? N3 C14 H14B 109.5 . . ? H14A C14 H14B 109.5 . . ? N3 C14 H14C 109.5 . . ? H14A C14 H14C 109.5 . . ? H14B C14 H14C 109.5 . . ? _diffrn_measured_fraction_theta_max 0.982 _diffrn_reflns_theta_full 27.49 _diffrn_measured_fraction_theta_full 0.982 _refine_diff_density_max 1.264 _refine_diff_density_min -1.493 _refine_diff_density_rms 0.248 #===END data_2 _database_code_depnum_ccdc_archive 'CCDC 830728' #TrackingRef '- JPLangCIF.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C9 H11 N2, Cu I2' _chemical_formula_sum 'C9 H11 Cu I2 N2' _chemical_formula_weight 464.55 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' I I -0.4742 1.8119 '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 Tetragonal _symmetry_space_group_name_H-M 'P 42' _symmetry_space_group_name_Hall 'P 4c' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x, z+1/2' '-x, -y, z' 'y, -x, z+1/2' _cell_length_a 14.015(3) _cell_length_b 14.015(3) _cell_length_c 6.6579(13) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1307.8(5) _cell_formula_units_Z 4 _cell_measurement_temperature 223(2) _cell_measurement_reflns_used 5990 _cell_measurement_theta_min 3.0597 _cell_measurement_theta_max 27.4778 _exptl_crystal_description Needle _exptl_crystal_colour Black _exptl_crystal_size_max 0.25 _exptl_crystal_size_mid 0.11 _exptl_crystal_size_min 0.09 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.359 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 856 _exptl_absorpt_coefficient_mu 6.359 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.446 _exptl_absorpt_correction_T_max 0.564 _exptl_absorpt_process_details 'Jacobson, R. (1998) Private communication to Rigaku Company, Tokyo, Japan.' _exptl_special_details ; ? ; _diffrn_ambient_temperature 223(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 MercuryCCD area detector' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 7522 _diffrn_reflns_av_R_equivalents 0.0286 _diffrn_reflns_av_sigmaI/netI 0.0369 _diffrn_reflns_limit_h_min -18 _diffrn_reflns_limit_h_max 14 _diffrn_reflns_limit_k_min -18 _diffrn_reflns_limit_k_max 13 _diffrn_reflns_limit_l_min -8 _diffrn_reflns_limit_l_max 8 _diffrn_reflns_theta_min 3.25 _diffrn_reflns_theta_max 27.47 _reflns_number_total 2921 _reflns_number_gt 2586 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_cell_refinement 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_data_reduction 'CrystalStructure, Ver. 3.60 (Rigaku/MSC, 2004)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'ORTEPII (Johnson, 1976)' _computing_publication_material SHELXL97 _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^)+(0.0224P)^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 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 0.07(4) _refine_ls_number_reflns 2921 _refine_ls_number_parameters 129 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.0366 _refine_ls_R_factor_gt 0.0293 _refine_ls_wR_factor_ref 0.0526 _refine_ls_wR_factor_gt 0.0496 _refine_ls_goodness_of_fit_ref 0.991 _refine_ls_restrained_S_all 0.991 _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 Cu1 Cu 0.0000 1.0000 0.9652(2) 0.0450(2) Uani 1 2 d S . . Cu2 Cu 0.5000 0.5000 0.9920(3) 0.0509(2) Uani 1 2 d S . . I1 I -0.09739(2) 0.887817(19) 0.71538(5) 0.03591(9) Uani 1 1 d . . . I2 I 0.37009(2) 0.57373(2) 1.24158(5) 0.04425(10) Uani 1 1 d . . . N1 N 0.2489(3) 0.7961(3) 0.7484(8) 0.0459(10) Uani 1 1 d . . . N2 N 0.1117(5) 0.4467(5) 0.6425(10) 0.095(2) Uani 1 1 d . . . C1 C 0.1566(3) 0.7834(4) 0.7058(12) 0.0494(13) Uani 1 1 d . . . H1 H 0.1160 0.8366 0.6963 0.059 Uiso 1 1 calc R . . C2 C 0.1204(4) 0.6932(4) 0.6756(9) 0.0548(16) Uani 1 1 d . . . H2 H 0.0554 0.6844 0.6461 0.066 Uiso 1 1 calc R . . C3 C 0.1810(4) 0.6160(4) 0.6894(9) 0.0547(16) Uani 1 1 d . . . C4 C 0.2766(4) 0.6306(4) 0.7368(10) 0.0559(13) Uani 1 1 d . . . H4 H 0.3184 0.5784 0.7480 0.067 Uiso 1 1 calc R . . C5 C 0.3090(4) 0.7205(4) 0.7668(9) 0.0550(17) Uani 1 1 d . . . H5 H 0.3733 0.7307 0.8005 0.066 Uiso 1 1 calc R . . C6 C 0.1438(5) 0.5206(6) 0.6602(10) 0.072(2) Uani 1 1 d . . . C7 C 0.2856(4) 0.8951(4) 0.7783(10) 0.0599(19) Uani 1 1 d . . . H7A H 0.3215 0.8979 0.9044 0.072 Uiso 1 1 calc R . . H7B H 0.2315 0.9391 0.7895 0.072 Uiso 1 1 calc R . . C8 C 0.3489(5) 0.9267(6) 0.6090(9) 0.073(2) Uani 1 1 d . . . H8A H 0.3141 0.9231 0.4815 0.088 Uiso 1 1 calc R . . H8B H 0.4048 0.8849 0.6001 0.088 Uiso 1 1 calc R . . C9 C 0.3806(4) 1.0300(5) 0.6486(10) 0.077(2) Uani 1 1 d . . . H9A H 0.3249 1.0709 0.6564 0.115 Uiso 1 1 calc R . . H9B H 0.4215 1.0513 0.5400 0.115 Uiso 1 1 calc R . . H9C H 0.4154 1.0329 0.7744 0.115 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 0.0462(10) 0.0424(9) 0.0463(6) 0.000 0.000 -0.0022(9) Cu2 0.0496(10) 0.0538(10) 0.0493(6) 0.000 0.000 0.0034(9) I1 0.03586(15) 0.03917(16) 0.03268(18) -0.0026(2) 0.0020(2) -0.00280(11) I2 0.04517(18) 0.05146(19) 0.0361(2) 0.0020(2) 0.0013(2) 0.00603(13) N1 0.042(2) 0.064(3) 0.032(3) -0.001(3) 0.004(2) 0.0107(18) N2 0.132(6) 0.076(4) 0.077(4) -0.006(4) -0.008(4) -0.008(4) C1 0.041(3) 0.064(3) 0.044(3) 0.008(4) -0.001(3) 0.016(2) C2 0.047(3) 0.075(4) 0.042(4) 0.002(3) 0.001(3) 0.018(3) C3 0.068(4) 0.067(4) 0.030(4) -0.002(3) 0.000(3) 0.017(3) C4 0.061(3) 0.071(4) 0.035(3) 0.002(4) 0.002(4) 0.030(3) C5 0.042(3) 0.080(4) 0.044(4) 0.001(3) 0.000(3) 0.026(3) C6 0.075(5) 0.082(5) 0.058(5) -0.003(4) 0.005(3) 0.012(4) C7 0.055(4) 0.073(4) 0.052(5) 0.006(3) 0.003(3) 0.016(3) C8 0.048(4) 0.124(7) 0.048(4) 0.005(4) 0.003(3) -0.019(4) C9 0.050(4) 0.107(6) 0.072(5) 0.031(4) 0.002(3) -0.009(4) _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 I1 2.6663(12) 4_465 ? Cu1 I1 2.6663(12) 2_665 ? Cu1 I1 2.6649(12) . ? Cu1 I1 2.6649(12) 3_575 ? Cu1 Cu1 3.329(2) 2_665 ? Cu1 Cu1 3.329(2) 2_664 ? Cu2 I2 2.6730(12) 3_665 ? Cu2 I2 2.6730(12) . ? Cu2 I2 2.6761(12) 2_654 ? Cu2 I2 2.6761(12) 4_564 ? Cu2 Cu2 3.329(3) 2_655 ? Cu2 Cu2 3.329(3) 2_654 ? I1 Cu1 2.6663(12) 2_664 ? I2 Cu2 2.6761(12) 2_655 ? N1 C1 1.335(6) . ? N1 C5 1.359(6) . ? N1 C7 1.493(7) . ? N2 C6 1.135(8) . ? C1 C2 1.377(7) . ? C1 H1 0.9400 . ? C2 C3 1.379(7) . ? C2 H2 0.9400 . ? C3 C4 1.391(7) . ? C3 C6 1.448(9) . ? C4 C5 1.354(7) . ? C4 H4 0.9400 . ? C5 H5 0.9400 . ? C7 C8 1.501(7) . ? C7 H7A 0.9800 . ? C7 H7B 0.9800 . ? C8 C9 1.538(9) . ? C8 H8A 0.9800 . ? C8 H8B 0.9800 . ? C9 H9A 0.9700 . ? C9 H9B 0.9700 . ? C9 H9C 0.9700 . ? 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 I1 Cu1 I1 102.68(6) 4_465 2_665 ? I1 Cu1 I1 112.949(9) 4_465 . ? I1 Cu1 I1 112.949(9) 2_665 . ? I1 Cu1 I1 112.949(9) 4_465 3_575 ? I1 Cu1 I1 112.949(9) 2_665 3_575 ? I1 Cu1 I1 102.76(6) . 3_575 ? I1 Cu1 Cu1 51.34(3) 4_465 2_665 ? I1 Cu1 Cu1 51.34(3) 2_665 2_665 ? I1 Cu1 Cu1 128.62(3) . 2_665 ? I1 Cu1 Cu1 128.62(3) 3_575 2_665 ? I1 Cu1 Cu1 128.66(3) 4_465 2_664 ? I1 Cu1 Cu1 128.66(3) 2_665 2_664 ? I1 Cu1 Cu1 51.38(3) . 2_664 ? I1 Cu1 Cu1 51.38(3) 3_575 2_664 ? Cu1 Cu1 Cu1 180.000(1) 2_665 2_664 ? I2 Cu2 I2 103.11(6) 3_665 . ? I2 Cu2 I2 112.787(9) 3_665 2_654 ? I2 Cu2 I2 112.787(9) . 2_654 ? I2 Cu2 I2 112.787(9) 3_665 4_564 ? I2 Cu2 I2 112.787(9) . 4_564 ? I2 Cu2 I2 102.94(6) 2_654 4_564 ? I2 Cu2 Cu2 51.56(3) 3_665 2_655 ? I2 Cu2 Cu2 51.56(3) . 2_655 ? I2 Cu2 Cu2 128.53(3) 2_654 2_655 ? I2 Cu2 Cu2 128.53(3) 4_564 2_655 ? I2 Cu2 Cu2 128.44(3) 3_665 2_654 ? I2 Cu2 Cu2 128.44(3) . 2_654 ? I2 Cu2 Cu2 51.47(3) 2_654 2_654 ? I2 Cu2 Cu2 51.47(3) 4_564 2_654 ? Cu2 Cu2 Cu2 180.000(1) 2_655 2_654 ? Cu1 I1 Cu1 77.280(17) 2_664 . ? Cu2 I2 Cu2 76.974(18) . 2_655 ? C1 N1 C5 121.0(5) . . ? C1 N1 C7 119.1(4) . . ? C5 N1 C7 119.9(4) . . ? N1 C1 C2 120.7(4) . . ? N1 C1 H1 119.7 . . ? C2 C1 H1 119.7 . . ? C1 C2 C3 118.9(5) . . ? C1 C2 H2 120.6 . . ? C3 C2 H2 120.6 . . ? C4 C3 C2 119.5(6) . . ? C4 C3 C6 120.9(5) . . ? C2 C3 C6 119.6(6) . . ? C5 C4 C3 119.6(5) . . ? C5 C4 H4 120.2 . . ? C3 C4 H4 120.2 . . ? C4 C5 N1 120.3(5) . . ? C4 C5 H5 119.9 . . ? N1 C5 H5 119.9 . . ? N2 C6 C3 177.2(8) . . ? N1 C7 C8 112.2(5) . . ? N1 C7 H7A 109.2 . . ? C8 C7 H7A 109.2 . . ? N1 C7 H7B 109.2 . . ? C8 C7 H7B 109.2 . . ? H7A C7 H7B 107.9 . . ? C7 C8 C9 108.7(6) . . ? C7 C8 H8A 110.0 . . ? C9 C8 H8A 110.0 . . ? C7 C8 H8B 110.0 . . ? C9 C8 H8B 110.0 . . ? H8A C8 H8B 108.3 . . ? C8 C9 H9A 109.5 . . ? C8 C9 H9B 109.5 . . ? H9A C9 H9B 109.5 . . ? C8 C9 H9C 109.5 . . ? H9A C9 H9C 109.5 . . ? H9B C9 H9C 109.5 . . ? _diffrn_measured_fraction_theta_max 0.996 _diffrn_reflns_theta_full 27.47 _diffrn_measured_fraction_theta_full 0.996 _refine_diff_density_max 0.734 _refine_diff_density_min -0.594 _refine_diff_density_rms 0.090 #===END data_3 _database_code_depnum_ccdc_archive 'CCDC 830729' #TrackingRef '- JPLangCIF.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C9 H11 N2, Cu I2' _chemical_formula_sum 'C9 H11 Cu I2 N2' _chemical_formula_weight 464.55 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 0.0000 '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 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Cu Cu 0.3201 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' I I -0.4742 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Tetragonal _symmetry_space_group_name_H-M 'P -4 21 c' _symmetry_space_group_name_Hall 'P -4 2n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' 'y, -x, -z' '-y, x, -z' '-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' _cell_length_a 20.190(3) _cell_length_b 20.190(3) _cell_length_c 6.4628(13) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 2634.5(8) _cell_formula_units_Z 8 _cell_measurement_temperature 223(2) _cell_measurement_reflns_used 11006 _cell_measurement_theta_min 3.0268 _cell_measurement_theta_max 27.4739 _exptl_crystal_description Needle _exptl_crystal_colour Black _exptl_crystal_size_max 0.29 _exptl_crystal_size_mid 0.20 _exptl_crystal_size_min 0.10 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.342 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1712 _exptl_absorpt_coefficient_mu 6.313 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.250 _exptl_absorpt_correction_T_max 0.532 _exptl_absorpt_process_details 'Jacobson, R. (1998) Private communication to Rigaku Company, Tokyo, Japan.' _exptl_special_details ; ? ; _diffrn_ambient_temperature 223(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 MercuryCCD area detector' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 12792 _diffrn_reflns_av_R_equivalents 0.0435 _diffrn_reflns_av_sigmaI/netI 0.0191 _diffrn_reflns_limit_h_min -18 _diffrn_reflns_limit_h_max 24 _diffrn_reflns_limit_k_min -24 _diffrn_reflns_limit_k_max 21 _diffrn_reflns_limit_l_min -6 _diffrn_reflns_limit_l_max 7 _diffrn_reflns_theta_min 3.19 _diffrn_reflns_theta_max 25.00 _reflns_number_total 1329 _reflns_number_gt 1296 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_cell_refinement 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_data_reduction 'CrystalStructure, Ver. 3.60 (Rigaku/MSC, 2004)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'ORTEPII (Johnson, 1976)' _computing_publication_material SHELXL97 _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^)+(0.0636P)^2^+13.5755P] 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(10) _refine_ls_number_reflns 1329 _refine_ls_number_parameters 130 _refine_ls_number_restraints 115 _refine_ls_R_factor_all 0.0529 _refine_ls_R_factor_gt 0.0509 _refine_ls_wR_factor_ref 0.1208 _refine_ls_wR_factor_gt 0.1193 _refine_ls_goodness_of_fit_ref 1.036 _refine_ls_restrained_S_all 1.017 _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 Cu1 Cu 0.0000 0.5000 0.9677(4) 0.0590(6) Uani 1 2 d S . . Cu2 Cu 0.0000 1.0000 1.0000 0.0532(9) Uani 1 4 d S . . Cu3 Cu 0.0000 1.0000 0.5000 0.0552(9) Uani 1 4 d S . . I1 I 0.10490(4) 0.49055(5) 0.71673(15) 0.0539(3) Uani 1 1 d . . . I2 I 0.10440(4) 1.00848(4) 0.75014(12) 0.0524(3) Uani 1 1 d . . . N1 N -0.0184(5) 0.7612(4) 0.7251(16) 0.048(2) Uani 1 1 d U . . N2 N 0.2316(7) 0.6864(9) 0.785(3) 0.110(5) Uani 1 1 d U . . C1 C -0.0023(6) 0.6969(6) 0.715(2) 0.055(3) Uani 1 1 d U . . H1 H -0.0349 0.6642 0.6970 0.066 Uiso 1 1 calc R . . C2 C 0.0644(6) 0.6800(6) 0.733(2) 0.057(3) Uani 1 1 d U . . H2 H 0.0771 0.6352 0.7304 0.068 Uiso 1 1 calc R . . C3 C 0.1096(7) 0.7264(7) 0.752(2) 0.059(3) Uani 1 1 d U . . C4 C 0.0922(7) 0.7916(7) 0.764(3) 0.067(3) Uani 1 1 d U . . H4 H 0.1248 0.8243 0.7829 0.080 Uiso 1 1 calc R . . C5 C 0.0263(7) 0.8090(6) 0.747(2) 0.059(3) Uani 1 1 d U . . H5 H 0.0133 0.8537 0.7500 0.071 Uiso 1 1 calc R . . C6 C 0.1785(8) 0.7069(9) 0.776(3) 0.082(4) Uani 1 1 d U . . C7 C -0.1225(8) 0.7631(9) 0.918(3) 0.085(5) Uani 1 1 d U . . H7A H -0.1221 0.7154 0.9352 0.127 Uiso 1 1 calc R . . H7B H -0.1678 0.7790 0.9219 0.127 Uiso 1 1 calc R . . H7C H -0.0974 0.7834 1.0297 0.127 Uiso 1 1 calc R . . C8 C -0.0914(7) 0.7810(7) 0.714(3) 0.065(3) Uani 1 1 d U . . H8 H -0.0936 0.8297 0.6983 0.078 Uiso 1 1 calc R . . C9 C -0.1226(9) 0.7506(10) 0.525(3) 0.090(5) Uani 1 1 d U . . H9A H -0.1229 0.7028 0.5389 0.135 Uiso 1 1 calc R . . H9B H -0.0973 0.7629 0.4031 0.135 Uiso 1 1 calc R . . H9C H -0.1676 0.7666 0.5107 0.135 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 0.0502(15) 0.0522(16) 0.0745(15) 0.000 0.000 0.0026(8) Cu2 0.0495(14) 0.0495(14) 0.0607(18) 0.000 0.000 0.000 Cu3 0.0530(14) 0.0530(14) 0.0594(18) 0.000 0.000 0.000 I1 0.0422(5) 0.0627(5) 0.0568(5) 0.0011(4) 0.0001(4) 0.0077(4) I2 0.0409(5) 0.0730(6) 0.0432(4) 0.0002(5) 0.0004(4) -0.0002(3) N1 0.060(5) 0.040(5) 0.043(5) -0.004(5) 0.005(5) -0.002(4) N2 0.079(6) 0.142(9) 0.108(9) 0.011(8) -0.001(7) 0.004(6) C1 0.046(5) 0.046(5) 0.073(7) 0.000(7) 0.004(7) -0.004(4) C2 0.053(5) 0.054(6) 0.063(8) 0.001(7) 0.010(7) 0.000(4) C3 0.055(5) 0.087(7) 0.037(7) 0.010(7) -0.005(7) -0.015(5) C4 0.074(6) 0.073(6) 0.053(8) -0.003(8) -0.002(8) -0.037(5) C5 0.088(6) 0.045(5) 0.044(6) 0.002(6) 0.006(7) -0.016(5) C6 0.066(5) 0.111(8) 0.070(8) 0.010(7) 0.005(7) -0.007(6) C7 0.069(7) 0.106(9) 0.079(7) 0.000(7) 0.011(6) 0.013(7) C8 0.069(6) 0.055(7) 0.070(8) -0.004(7) 0.004(7) 0.018(6) C9 0.080(8) 0.107(9) 0.083(7) -0.008(7) -0.016(6) 0.014(8) _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 I1 2.6667(18) 8_455 ? Cu1 I1 2.6668(18) 7 ? Cu1 I1 2.6746(18) . ? Cu1 I1 2.6746(18) 2_565 ? Cu2 I2 2.6608(8) 4_667 ? Cu2 I2 2.6608(9) 2_575 ? Cu2 I2 2.6608(9) . ? Cu2 I2 2.6608(8) 3_467 ? Cu3 I2 2.6619(8) . ? Cu3 I2 2.6619(8) 4_666 ? Cu3 I2 2.6619(8) 3_466 ? Cu3 I2 2.6619(8) 2_575 ? I1 Cu1 2.6668(18) 7_554 ? N1 C5 1.328(14) . ? N1 C1 1.340(14) . ? N1 C8 1.530(16) . ? N2 C6 1.151(18) . ? C1 C2 1.393(16) . ? C1 H1 0.9400 . ? C2 C3 1.313(18) . ? C2 H2 0.9400 . ? C3 C4 1.36(2) . ? C3 C6 1.45(2) . ? C4 C5 1.381(19) . ? C4 H4 0.9400 . ? C5 H5 0.9400 . ? C7 C8 1.51(2) . ? C7 H7A 0.9700 . ? C7 H7B 0.9700 . ? C7 H7C 0.9700 . ? C8 C9 1.50(2) . ? C8 H8 0.9900 . ? C9 H9A 0.9700 . ? C9 H9B 0.9700 . ? C9 H9C 0.9700 . ? 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 I1 Cu1 I1 105.77(10) 8_455 7 ? I1 Cu1 I1 118.64(4) 8_455 . ? I1 Cu1 I1 104.64(3) 7 . ? I1 Cu1 I1 104.64(3) 8_455 2_565 ? I1 Cu1 I1 118.64(4) 7 2_565 ? I1 Cu1 I1 105.32(10) . 2_565 ? I2 Cu2 I2 111.612(19) 4_667 2_575 ? I2 Cu2 I2 111.612(19) 4_667 . ? I2 Cu2 I2 105.27(4) 2_575 . ? I2 Cu2 I2 105.27(4) 4_667 3_467 ? I2 Cu2 I2 111.612(19) 2_575 3_467 ? I2 Cu2 I2 111.612(19) . 3_467 ? I2 Cu3 I2 111.644(19) . 4_666 ? I2 Cu3 I2 111.644(19) . 3_466 ? I2 Cu3 I2 105.21(4) 4_666 3_466 ? I2 Cu3 I2 105.21(4) . 2_575 ? I2 Cu3 I2 111.64(2) 4_666 2_575 ? I2 Cu3 I2 111.644(19) 3_466 2_575 ? Cu1 I1 Cu1 74.45(2) 7_554 . ? Cu2 I2 Cu3 74.76(2) . . ? C5 N1 C1 123.0(11) . . ? C5 N1 C8 118.0(10) . . ? C1 N1 C8 119.0(10) . . ? N1 C1 C2 117.9(11) . . ? N1 C1 H1 121.1 . . ? C2 C1 H1 121.1 . . ? C3 C2 C1 120.3(13) . . ? C3 C2 H2 119.8 . . ? C1 C2 H2 119.8 . . ? C2 C3 C4 121.0(13) . . ? C2 C3 C6 118.8(15) . . ? C4 C3 C6 120.1(14) . . ? C3 C4 C5 119.2(11) . . ? C3 C4 H4 120.4 . . ? C5 C4 H4 120.4 . . ? N1 C5 C4 118.6(12) . . ? N1 C5 H5 120.7 . . ? C4 C5 H5 120.7 . . ? N2 C6 C3 174(2) . . ? C8 C7 H7A 109.5 . . ? C8 C7 H7B 109.5 . . ? H7A C7 H7B 109.5 . . ? C8 C7 H7C 109.5 . . ? H7A C7 H7C 109.5 . . ? H7B C7 H7C 109.5 . . ? C9 C8 C7 116.1(14) . . ? C9 C8 N1 109.7(12) . . ? C7 C8 N1 107.2(13) . . ? C9 C8 H8 107.9 . . ? C7 C8 H8 107.9 . . ? N1 C8 H8 107.9 . . ? C8 C9 H9A 109.5 . . ? C8 C9 H9B 109.5 . . ? H9A C9 H9B 109.5 . . ? C8 C9 H9C 109.5 . . ? H9A C9 H9C 109.5 . . ? H9B C9 H9C 109.5 . . ? _diffrn_measured_fraction_theta_max 0.991 _diffrn_reflns_theta_full 25.00 _diffrn_measured_fraction_theta_full 0.991 _refine_diff_density_max 1.052 _refine_diff_density_min -0.741 _refine_diff_density_rms 0.189 #===END data_4 _database_code_depnum_ccdc_archive 'CCDC 830730' #TrackingRef '- JPLangCIF.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C7 H9 N, Cu I2' _chemical_formula_sum 'C7 H9 Cu I2 N' _chemical_formula_weight 424.50 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' Cu Cu 0.3201 1.2651 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Tetragonal _symmetry_space_group_name_H-M 'P 42/m n m' _symmetry_space_group_name_Hall '-P 4n 2n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' '-y+1/2, x+1/2, z+1/2' 'y+1/2, -x+1/2, z+1/2' '-x+1/2, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z+1/2' 'y, x, -z' '-y, -x, -z' '-x, -y, -z' 'x, y, -z' 'y-1/2, -x-1/2, -z-1/2' '-y-1/2, x-1/2, -z-1/2' 'x-1/2, -y-1/2, z-1/2' '-x-1/2, y-1/2, z-1/2' '-y, -x, z' 'y, x, z' _cell_length_a 12.4720(18) _cell_length_b 12.4720(18) _cell_length_c 6.7927(14) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1056.6(3) _cell_formula_units_Z 4 _cell_measurement_temperature 223(2) _cell_measurement_reflns_used 3438 _cell_measurement_theta_min 3.2646 _cell_measurement_theta_max 25.3491 _exptl_crystal_description Block _exptl_crystal_colour black _exptl_crystal_size_max 0.34 _exptl_crystal_size_mid 0.19 _exptl_crystal_size_min 0.19 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.669 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 772 _exptl_absorpt_coefficient_mu 7.854 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.175 _exptl_absorpt_correction_T_max 0.317 _exptl_absorpt_process_details 'Jacobson, R. (1998) Private communication.' _exptl_special_details ; ? ; _diffrn_ambient_temperature 223(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 Mercury' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 9669 _diffrn_reflns_av_R_equivalents 0.0462 _diffrn_reflns_av_sigmaI/netI 0.0186 _diffrn_reflns_limit_h_min -15 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -15 _diffrn_reflns_limit_k_max 15 _diffrn_reflns_limit_l_min -8 _diffrn_reflns_limit_l_max 7 _diffrn_reflns_theta_min 3.27 _diffrn_reflns_theta_max 25.35 _reflns_number_total 563 _reflns_number_gt 546 _reflns_threshold_expression >2sigma(I) _computing_data_collection CrystalClear _computing_cell_refinement CrystalClear _computing_data_reduction CrystalStructure _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'SHELXL-97 (Sheldrick, 1997)' _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^)+(0.0425P)^2^+1.8635P] 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 SHELXL _refine_ls_extinction_coef 0.0034(6) _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 563 _refine_ls_number_parameters 42 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0316 _refine_ls_R_factor_gt 0.0299 _refine_ls_wR_factor_ref 0.0765 _refine_ls_wR_factor_gt 0.0756 _refine_ls_goodness_of_fit_ref 1.172 _refine_ls_restrained_S_all 1.172 _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 0.5000 0.0000 -0.7500 0.0447(4) Uani 1 4 d S . . I1 I 0.57383(4) 0.14773(4) -0.5000 0.0343(3) Uani 1 2 d S . . C1 C 0.7720(6) -0.0964(7) -0.5000 0.0447(19) Uani 1 2 d S . . H1 H 0.6990 -0.0780 -0.5000 0.054 Uiso 1 2 calc SR . . C2 C 0.8497(6) -0.0161(7) -0.5000 0.0420(18) Uani 1 2 d S . . H2 H 0.8281 0.0561 -0.5000 0.050 Uiso 1 2 calc SR . . C3 C 0.9593(7) -0.0407(7) -0.5000 0.038(2) Uani 1 4 d S . . C4 C 0.7163(10) -0.2837(10) -0.571(2) 0.038(4) Uani 0.50 2 d SP . . H4A H 0.6989 -0.2114 -0.6179 0.046 Uiso 0.25 1 calc PR . . H4B H 0.7886 -0.3011 -0.6179 0.046 Uiso 0.25 1 calc PR . . C5 C 0.6729(12) -0.3271(12) -0.379(3) 0.050(5) Uani 0.50 2 d SP . . H5A H 0.6369 -0.3664 -0.4829 0.075 Uiso 0.50 2 calc SPR . . H5B H 0.6203 -0.2883 -0.3016 0.075 Uiso 0.25 1 calc PR . . H5C H 0.7112 -0.3769 -0.2948 0.075 Uiso 0.25 1 calc PR . . N1 N 0.8008(6) -0.1992(6) -0.5000 0.059(3) Uani 1 4 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 Cu1 0.0429(5) 0.0429(5) 0.0484(8) 0.000 0.000 0.000 I1 0.0330(3) 0.0324(4) 0.0373(4) 0.000 0.000 -0.00020(17) C1 0.034(4) 0.042(5) 0.058(5) 0.000 0.000 0.015(3) C2 0.041(4) 0.038(5) 0.047(4) 0.000 0.000 0.017(3) C3 0.039(3) 0.039(3) 0.036(5) 0.000 0.000 0.014(4) C4 0.041(5) 0.041(5) 0.033(9) -0.001(5) -0.001(5) 0.010(7) C5 0.060(7) 0.060(7) 0.030(9) 0.013(6) 0.013(6) 0.009(9) N1 0.034(3) 0.034(3) 0.110(10) 0.000 0.000 0.001(4) _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 I1 2.6696(5) . ? Cu1 I1 2.6696(5) 3_544 ? Cu1 I1 2.6696(5) 11_664 ? Cu1 I1 2.6696(5) 9_654 ? I1 Cu1 2.6696(5) 9_654 ? C1 N1 1.331(9) . ? C1 C2 1.394(12) . ? C1 H1 0.9400 . ? C2 C3 1.401(9) . ? C2 H2 0.9400 . ? C3 C3 1.44(2) 9_754 ? C3 C2 1.401(9) 7_644 ? C4 C5 0.84(2) 10_554 ? C4 C4 0.97(3) 10_554 ? C4 N1 1.567(19) . ? C4 C5 1.51(2) . ? C4 H4A 0.9800 . ? C4 H4B 0.9800 . ? C5 C4 0.84(2) 10_554 ? C5 C5 1.64(3) 10_554 ? C5 H5A 0.9700 . ? C5 H5B 0.9700 . ? C5 H5C 0.9700 . ? N1 C1 1.331(9) 7_644 ? N1 C4 1.567(19) 10_554 ? 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 I1 Cu1 I1 113.869(10) . 3_544 ? I1 Cu1 I1 113.869(10) . 11_664 ? I1 Cu1 I1 100.993(19) 3_544 11_664 ? I1 Cu1 I1 100.993(19) . 9_654 ? I1 Cu1 I1 113.869(10) 3_544 9_654 ? I1 Cu1 I1 113.869(10) 11_664 9_654 ? Cu1 I1 Cu1 79.007(19) . 9_654 ? N1 C1 C2 120.4(7) . . ? N1 C1 H1 119.8 . . ? C2 C1 H1 119.8 . . ? C1 C2 C3 121.4(8) . . ? C1 C2 H2 119.3 . . ? C3 C2 H2 119.3 . . ? C3 C3 C2 122.3(5) 9_754 . ? C3 C3 C2 122.3(5) 9_754 7_644 ? C2 C3 C2 115.3(10) . 7_644 ? C5 C4 C4 113.8(19) 10_554 10_554 ? C5 C4 N1 174(2) 10_554 . ? C4 C4 N1 72.0(6) 10_554 . ? C5 C4 C5 83(3) 10_554 . ? C4 C4 C5 30.4(9) 10_554 . ? N1 C4 C5 102.3(10) . . ? C5 C4 H4A 108.8 10_554 . ? C4 C4 H4A 108.8 10_554 . ? N1 C4 H4A 68.3 . . ? C5 C4 H4A 121.9 . . ? C5 C4 H4B 108.8 10_554 . ? C4 C4 H4B 108.8 10_554 . ? N1 C4 H4B 68.3 . . ? C5 C4 H4B 121.9 . . ? H4A C4 H4B 107.7 . . ? C4 C5 C4 35.9(16) 10_554 . ? C4 C5 C5 66.2(19) 10_554 10_554 ? C4 C5 C5 30.4(9) . 10_554 ? C4 C5 H5A 109.5 10_554 . ? C4 C5 H5A 73.6 . . ? C5 C5 H5A 43.3 10_554 . ? C4 C5 H5B 109.5 10_554 . ? C4 C5 H5B 122.1 . . ? C5 C5 H5B 122.8 10_554 . ? H5A C5 H5B 109.5 . . ? C4 C5 H5C 109.5 10_554 . ? C4 C5 H5C 124.2 . . ? C5 C5 H5C 126.1 10_554 . ? H5A C5 H5C 109.5 . . ? H5B C5 H5C 109.5 . . ? C1 N1 C1 121.3(10) . 7_644 ? C1 N1 C4 117.8(5) . 10_554 ? C1 N1 C4 117.8(5) 7_644 10_554 ? C1 N1 C4 117.8(5) . . ? C1 N1 C4 117.8(5) 7_644 . ? C4 N1 C4 36.1(12) 10_554 . ? _diffrn_measured_fraction_theta_max 0.995 _diffrn_reflns_theta_full 25.35 _diffrn_measured_fraction_theta_full 0.995 _refine_diff_density_max 1.151 _refine_diff_density_min -0.540 _refine_diff_density_rms 0.143 #===END data_5 _database_code_depnum_ccdc_archive 'CCDC 830731' #TrackingRef '- JPLangCIF.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C8 H11 N, Cu I2' _chemical_formula_sum 'C8 H11 Cu I2 N' _chemical_formula_weight 438.52 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' Cu Cu 0.3201 1.2651 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Tetragonal _symmetry_space_group_name_H-M 'P 42/n' _symmetry_space_group_name_Hall '-P 4bc' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y+1/2, z' '-y, x+1/2, z+1/2' 'y+1/2, -x, z+1/2' '-x, -y, -z' 'x-1/2, y-1/2, -z' 'y, -x-1/2, -z-1/2' '-y-1/2, x, -z-1/2' _cell_length_a 17.911(3) _cell_length_b 17.911(3) _cell_length_c 6.8270(14) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 2190.2(6) _cell_formula_units_Z 8 _cell_measurement_temperature 223(2) _cell_measurement_reflns_used 7186 _cell_measurement_theta_min 3.1929 _cell_measurement_theta_max 25.3491 _exptl_crystal_description Block _exptl_crystal_colour black _exptl_crystal_size_max 0.41 _exptl_crystal_size_mid 0.10 _exptl_crystal_size_min 0.06 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 2.660 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1608 _exptl_absorpt_coefficient_mu 7.582 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.1471 _exptl_absorpt_correction_T_max 0.6590 _exptl_absorpt_process_details 'Jacobson, R. (1998) Private communication to Rigaku Company, Tokyo, Japan.' _exptl_special_details ; ? ; _diffrn_ambient_temperature 223(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 MercuryCCD area detector' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0 _diffrn_reflns_number 21498 _diffrn_reflns_av_R_equivalents 0.0584 _diffrn_reflns_av_sigmaI/netI 0.0286 _diffrn_reflns_limit_h_min -21 _diffrn_reflns_limit_h_max 21 _diffrn_reflns_limit_k_min -21 _diffrn_reflns_limit_k_max 21 _diffrn_reflns_limit_l_min -8 _diffrn_reflns_limit_l_max 7 _diffrn_reflns_theta_min 3.19 _diffrn_reflns_theta_max 25.35 _reflns_number_total 2003 _reflns_number_gt 1915 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_cell_refinement 'CrystalClear, Ver. 1.30 (Rigaku/MSC, 2001)' _computing_data_reduction 'CrystalStructure, Ver. 3.60 (Rigaku/MSC, 2004)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'ORTEPII (Johnson, 1976)' _computing_publication_material SHELXL97 _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^)+(0.0314P)^2^+12.2207P] 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 SHELXL _refine_ls_extinction_coef 0.00141(11) _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 2003 _refine_ls_number_parameters 52 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0435 _refine_ls_R_factor_gt 0.0407 _refine_ls_wR_factor_ref 0.0902 _refine_ls_wR_factor_gt 0.0890 _refine_ls_goodness_of_fit_ref 1.174 _refine_ls_restrained_S_all 1.174 _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 0.7500 -0.2500 -0.2500 0.0404(8) Uani 1 4 d S . . Cu2 Cu 0.7500 -0.2500 0.2500 0.0446(8) Uani 1 4 d S . . Cu3 Cu 0.7500 0.2500 0.7100(3) 0.0438(6) Uani 1 2 d S . . I1 I 0.78170(5) -0.13983(5) -0.00276(8) 0.0334(2) Uani 1 1 d . . . I2 I 0.78367(5) 0.14027(5) 0.96074(9) 0.0337(2) Uani 1 1 d . . . C1 C 1.0658(4) 0.3414(4) 0.9733(9) 0.0373(7) Uani 1 1 d G . . H1 H 1.1110 0.3148 0.9715 0.045 Uiso 1 1 calc R . . C2 C 1.0663(5) 0.4185(4) 0.9958(9) 0.0373(7) Uani 1 1 d G . . H2 H 1.1118 0.4441 1.0093 0.045 Uiso 1 1 calc R . . C3 C 0.9994(6) 0.45786(19) 0.9985(10) 0.0373(7) Uani 1 1 d G . . C4 C 0.9320(5) 0.4201(4) 0.9786(10) 0.0373(7) Uani 1 1 d G . . H4 H 0.8868 0.4467 0.9804 0.045 Uiso 1 1 calc R . . C5 C 0.9315(4) 0.3429(4) 0.9560(9) 0.0373(7) Uani 1 1 d G . . H5 H 0.8860 0.3174 0.9426 0.045 Uiso 1 1 calc R . . C6 C 0.9956(6) 0.2235(5) 0.9007(14) 0.0373(7) Uani 1 1 d . . . H6A H 1.0367 0.2120 0.8108 0.045 Uiso 1 1 calc R . . H6B H 0.9486 0.2129 0.8329 0.045 Uiso 1 1 calc R . . C7 C 1.0016(7) 0.1752(5) 1.0772(14) 0.0373(7) Uani 1 1 d . . . H7A H 0.9577 0.1818 1.1611 0.045 Uiso 1 1 calc R . . H7B H 1.0462 0.1883 1.1529 0.045 Uiso 1 1 calc R . . C8 C 1.0066(8) 0.0931(5) 1.0044(16) 0.0373(7) Uani 1 1 d . . . H8A H 1.0573 0.0824 0.9633 0.056 Uiso 1 1 calc R . . H8B H 0.9730 0.0861 0.8946 0.056 Uiso 1 1 calc R . . H8C H 0.9927 0.0596 1.1098 0.056 Uiso 1 1 calc R . . N1 N 0.9984(5) 0.30361(19) 0.9534(8) 0.0373(7) Uani 1 1 d G . . 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 0.0404(12) 0.0404(12) 0.0403(15) 0.000 0.000 0.000 Cu2 0.0416(12) 0.0416(12) 0.0506(17) 0.000 0.000 0.000 Cu3 0.0414(13) 0.0465(13) 0.0435(11) 0.000 0.000 -0.0009(8) I1 0.0331(5) 0.0343(5) 0.0329(3) -0.0018(2) 0.0002(3) -0.0026(4) I2 0.0339(6) 0.0327(5) 0.0344(3) 0.0004(3) -0.0016(3) 0.0009(4) C1 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C2 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C3 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C4 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C5 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C6 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C7 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) C8 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(2) N1 0.0330(14) 0.0365(14) 0.0425(17) 0.0002(14) 0.0017(15) -0.003(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 Cu1 I1 2.6580(8) . ? Cu1 I1 2.6580(8) 2_645 ? Cu1 I1 2.6580(8) 8_645 ? Cu1 I1 2.6580(8) 7_665 ? Cu2 I1 2.6822(8) 2_645 ? Cu2 I1 2.6822(8) 7_666 ? Cu2 I1 2.6822(8) 8_646 ? Cu2 I1 2.6822(8) . ? Cu3 I2 2.6686(15) 4_564 ? Cu3 I2 2.6686(15) 3_644 ? Cu3 I2 2.6755(15) 2_655 ? Cu3 I2 2.6755(15) . ? I2 Cu3 2.6686(15) 3_645 ? C1 C2 1.3900 . ? C1 N1 1.3900 . ? C1 H1 0.9400 . ? C2 C3 1.3900 . ? C2 H2 0.9400 . ? C3 C4 1.3900 . ? C3 C3 1.510(7) 5_767 ? C4 C5 1.3900 . ? C4 H4 0.9400 . ? C5 N1 1.3900 . ? C5 H5 0.9400 . ? C6 N1 1.480(9) . ? C6 C7 1.487(12) . ? C6 H6A 0.9800 . ? C6 H6B 0.9800 . ? C7 C8 1.555(12) . ? C7 H7A 0.9800 . ? C7 H7B 0.9800 . ? C8 H8A 0.9700 . ? C8 H8B 0.9700 . ? C8 H8C 0.9700 . ? 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 I1 Cu1 I1 101.16(3) . 2_645 ? I1 Cu1 I1 113.781(18) . 8_645 ? I1 Cu1 I1 113.781(18) 2_645 8_645 ? I1 Cu1 I1 113.781(18) . 7_665 ? I1 Cu1 I1 113.781(18) 2_645 7_665 ? I1 Cu1 I1 101.16(3) 8_645 7_665 ? I1 Cu2 I1 114.452(18) 2_645 7_666 ? I1 Cu2 I1 114.451(18) 2_645 8_646 ? I1 Cu2 I1 99.91(3) 7_666 8_646 ? I1 Cu2 I1 99.91(3) 2_645 . ? I1 Cu2 I1 114.451(18) 7_666 . ? I1 Cu2 I1 114.452(18) 8_646 . ? I2 Cu3 I2 100.78(7) 4_564 3_644 ? I2 Cu3 I2 114.079(14) 4_564 2_655 ? I2 Cu3 I2 114.079(15) 3_644 2_655 ? I2 Cu3 I2 114.079(14) 4_564 . ? I2 Cu3 I2 114.079(14) 3_644 . ? I2 Cu3 I2 100.42(7) 2_655 . ? Cu1 I1 Cu2 79.46(3) . . ? Cu3 I2 Cu3 79.40(3) 3_645 . ? C2 C1 N1 120.0 . . ? C2 C1 H1 120.0 . . ? N1 C1 H1 120.0 . . ? C3 C2 C1 120.0 . . ? C3 C2 H2 120.0 . . ? C1 C2 H2 120.0 . . ? C4 C3 C2 120.0 . . ? C4 C3 C3 120.1(14) . 5_767 ? C2 C3 C3 119.6(14) . 5_767 ? C3 C4 C5 120.0 . . ? C3 C4 H4 120.0 . . ? C5 C4 H4 120.0 . . ? C4 C5 N1 120.0 . . ? C4 C5 H5 120.0 . . ? N1 C5 H5 120.0 . . ? N1 C6 C7 111.4(7) . . ? N1 C6 H6A 109.4 . . ? C7 C6 H6A 109.4 . . ? N1 C6 H6B 109.4 . . ? C7 C6 H6B 109.4 . . ? H6A C6 H6B 108.0 . . ? C6 C7 C8 107.2(8) . . ? C6 C7 H7A 110.3 . . ? C8 C7 H7A 110.3 . . ? C6 C7 H7B 110.3 . . ? C8 C7 H7B 110.3 . . ? H7A C7 H7B 108.5 . . ? C7 C8 H8A 109.5 . . ? C7 C8 H8B 109.5 . . ? H8A C8 H8B 109.5 . . ? C7 C8 H8C 109.5 . . ? H8A C8 H8C 109.5 . . ? H8B C8 H8C 109.5 . . ? C5 N1 C1 120.0 . . ? C5 N1 C6 117.7(7) . . ? C1 N1 C6 121.7(7) . . ? _diffrn_measured_fraction_theta_max 0.999 _diffrn_reflns_theta_full 25.35 _diffrn_measured_fraction_theta_full 0.999 _refine_diff_density_max 1.275 _refine_diff_density_min -0.742 _refine_diff_density_rms 0.177 #===END