# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2012 data_global _journal_name_full Chem.Commun. _journal_coden_cambridge 0182 _journal_year ? _journal_volume ? _journal_page_first ? loop_ _publ_author_name 'William Gee' 'Stuart Batten' _publ_contact_author_email stuart.batten@sci.monash.edu.au _publ_contact_author_name 'Stuart Batten' data_c:\CuGel _database_code_depnum_ccdc_archive 'CCDC 862495' #TrackingRef '- 1.CIF' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C16 H14 Cl2 Cu N6' _chemical_formula_sum 'C16 H14 Cl2 Cu N6' _chemical_formula_weight 424.77 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' Cl Cl 0.1484 0.1585 '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' _symmetry_cell_setting Orthorhombic _symmetry_space_group_name_H-M 'P n n m' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' 'x+1/2, -y+1/2, -z+1/2' '-x+1/2, y+1/2, -z+1/2' '-x, -y, -z' 'x, y, -z' '-x-1/2, y-1/2, z-1/2' 'x-1/2, -y-1/2, z-1/2' _cell_length_a 3.7720(8) _cell_length_b 10.381(2) _cell_length_c 20.876(4) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 817.4(3) _cell_formula_units_Z 2 _cell_measurement_temperature 123(2) _cell_measurement_reflns_used 13606 _cell_measurement_theta_min 2.82 _cell_measurement_theta_max 29.78 _exptl_crystal_description needle _exptl_crystal_colour green _exptl_crystal_size_max 0.03 _exptl_crystal_size_mid 0.01 _exptl_crystal_size_min 0.01 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.726 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 430 _exptl_absorpt_coefficient_mu 1.675 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.9834 _exptl_absorpt_correction_T_max 0.9834 _exptl_absorpt_process_details 'SADABS (Sheldrick, 1997)' _exptl_special_details ; ? ; _diffrn_ambient_temperature 123(2) _diffrn_radiation_wavelength 0.710698 _diffrn_radiation_type synchrotron _diffrn_radiation_source 'Australian synchrotron MX1' _diffrn_radiation_monochromator silicon _diffrn_measurement_device_type 'ADSC Quantum 210r' _diffrn_measurement_method 'scans in phi' _diffrn_detector_area_resol_mean none _diffrn_standards_number 0 _diffrn_standards_interval_count none _diffrn_standards_interval_time none _diffrn_standards_decay_% none _diffrn_reflns_number 13606 _diffrn_reflns_av_R_equivalents 0.0727 _diffrn_reflns_av_sigmaI/netI 0.0290 _diffrn_reflns_limit_h_min -5 _diffrn_reflns_limit_h_max 5 _diffrn_reflns_limit_k_min -14 _diffrn_reflns_limit_k_max 14 _diffrn_reflns_limit_l_min -28 _diffrn_reflns_limit_l_max 28 _diffrn_reflns_theta_min 3.90 _diffrn_reflns_theta_max 29.38 _reflns_number_total 1136 _reflns_number_gt 1071 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Blu-Ice (McPhillips et al, 2002)' _computing_cell_refinement 'XDS (Kabsch, 1993)' _computing_data_reduction 'XDS (Kabsch, 1993)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics X-SEED _computing_publication_material 'XCIF V6.12 (BrukerAXS, 2001).' _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^)+(0.0978P)^2^+3.2279P] 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_number_reflns 1136 _refine_ls_number_parameters 56 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0674 _refine_ls_R_factor_gt 0.0635 _refine_ls_wR_factor_ref 0.1852 _refine_ls_wR_factor_gt 0.1766 _refine_ls_goodness_of_fit_ref 1.108 _refine_ls_restrained_S_all 1.108 _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 0.0000 0.0000 0.0000 0.0269(3) Uani 1 4 d S . . Cl1 Cl -0.3718(4) -0.17715(11) 0.0000 0.0254(4) Uani 1 2 d S . . C2 C 0.1038(10) -0.1083(3) 0.19535(17) 0.0235(7) Uani 1 1 d . . . H2 H 0.1786 -0.1842 0.2170 0.028 Uiso 1 1 calc R . . C3 C 0.0000 0.0000 0.2304(2) 0.0222(9) Uani 1 2 d S . . N1 N 0.0000 0.0000 0.0960(2) 0.0249(9) Uani 1 2 d S . . C1 C 0.0973(11) -0.1048(3) 0.12921(17) 0.0250(7) Uani 1 1 d . . . H1 H 0.1647 -0.1799 0.1062 0.030 Uiso 1 1 calc R . . C4 C 0.0000 0.0000 0.3001(2) 0.0280(11) Uani 1 2 d S . . C5 C 0.0946(14) -0.1049(6) 0.3365(2) 0.0560(11) Uani 0.50 1 d P A 1 H5 H 0.1698 -0.1872 0.3220 0.067 Uiso 0.50 1 calc PR A 1 C6 C 0.0567(14) -0.0645(6) 0.3972(2) 0.0560(11) Uani 0.50 1 d P . 1 H6 H 0.0997 -0.1151 0.4343 0.067 Uiso 0.50 1 calc PR . 1 N2 N 0.0946(14) -0.1049(6) 0.3365(2) 0.0560(11) Uani 0.50 1 d P A 2 N3 N 0.0567(14) -0.0645(6) 0.3972(2) 0.0560(11) Uani 0.50 1 d P . 2 H3 H 0.0965 -0.1114 0.4316 0.067 Uiso 0.50 1 calc PR . 2 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 0.0426(6) 0.0241(5) 0.0141(5) 0.000 0.000 -0.0108(4) Cl1 0.0345(7) 0.0242(6) 0.0174(5) 0.000 0.000 -0.0050(4) C2 0.0307(17) 0.0206(14) 0.0192(15) 0.0014(11) 0.0000(13) -0.0002(13) C3 0.024(2) 0.024(2) 0.019(2) 0.000 0.000 -0.0031(16) N1 0.036(2) 0.0216(19) 0.0169(18) 0.000 0.000 -0.0042(16) C1 0.0341(18) 0.0219(15) 0.0190(15) -0.0018(11) 0.0014(14) -0.0003(14) C4 0.033(3) 0.032(3) 0.018(2) 0.000 0.000 -0.003(2) C5 0.0462(19) 0.084(3) 0.0374(17) 0.0332(18) -0.0041(14) -0.0058(18) C6 0.0462(19) 0.084(3) 0.0374(17) 0.0332(18) -0.0041(14) -0.0058(18) N2 0.0462(19) 0.084(3) 0.0374(17) 0.0332(18) -0.0041(14) -0.0058(18) N3 0.0462(19) 0.084(3) 0.0374(17) 0.0332(18) -0.0041(14) -0.0058(18) _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 N1 2.004(4) . ? Cu1 N1 2.004(4) 5 ? Cu1 Cl1 2.3126(12) . ? Cu1 Cl1 2.3126(12) 5 ? C2 C1 1.382(5) . ? C2 C3 1.398(4) . ? C2 H2 0.9500 . ? C3 C2 1.398(4) 2 ? C3 C4 1.455(7) . ? N1 C1 1.341(4) . ? N1 C1 1.341(4) 2 ? C1 H1 0.9500 . ? C4 C5 1.375(6) . ? C4 N2 1.375(6) 2 ? C4 C5 1.375(6) 2 ? C5 C6 1.343(8) . ? C5 H5 0.9500 . ? C6 C6 1.405(13) 2 ? C6 H6 0.9500 . ? 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 Cu1 N1 180.0 . 5 ? N1 Cu1 Cl1 90.0 . . ? N1 Cu1 Cl1 90.0 5 . ? N1 Cu1 Cl1 90.0 . 5 ? N1 Cu1 Cl1 90.0 5 5 ? Cl1 Cu1 Cl1 180.00(3) . 5 ? C1 C2 C3 119.8(3) . . ? C1 C2 H2 120.1 . . ? C3 C2 H2 120.1 . . ? C2 C3 C2 116.9(4) . 2 ? C2 C3 C4 121.6(2) . . ? C2 C3 C4 121.6(2) 2 . ? C1 N1 C1 117.8(4) . 2 ? C1 N1 Cu1 121.1(2) . . ? C1 N1 Cu1 121.1(2) 2 . ? N1 C1 C2 122.9(3) . . ? N1 C1 H1 118.6 . . ? C2 C1 H1 118.6 . . ? C5 C4 N2 112.9(6) . 2 ? C5 C4 C5 112.9(6) . 2 ? C5 C4 C3 123.5(3) . . ? N2 C4 C3 123.5(3) 2 . ? C5 C4 C3 123.5(3) 2 . ? C6 C5 C4 104.3(6) . . ? C6 C5 H5 127.9 . . ? C4 C5 H5 127.9 . . ? C5 C6 C6 109.3(3) . 2 ? C5 C6 H6 125.4 . . ? C6 C6 H6 125.4 2 . ? loop_ _geom_hbond_atom_site_label_D _geom_hbond_atom_site_label_H _geom_hbond_atom_site_label_A _geom_hbond_distance_DH _geom_hbond_distance_HA _geom_hbond_distance_DA _geom_hbond_angle_DHA _geom_hbond_site_symmetry_A N3 H3 Cl1 0.88 2.62 3.446(5) 156.2 3_545 _diffrn_measured_fraction_theta_max 0.975 _diffrn_reflns_theta_full 29.38 _diffrn_measured_fraction_theta_full 0.975 _refine_diff_density_max 1.474 _refine_diff_density_min -1.501 _refine_diff_density_rms 0.144