# Supplementary Material (ESI) for Chemical Communications # This journal is (c) The Royal Society of Chemistry 2010 data_global _journal_coden_Cambridge 182 _journal_volume ? _journal_page_first ? _journal_year ? loop_ _publ_author_name 'Beverina, Luca ' _publ_contact_author_name 'Beverina, Luca ' _publ_contact_author_email luca.beverina@mater.unimib.it _publ_section_title ; UV Absorbing Zwitterionic Pyridinium-Tetrazolate. Exceptional Transparency/Optical Nonlinearity Tradeoff ; # Attachment '- LBZW01.cif' data_LBZW01 _database_code_depnum_ccdc_archive 'CCDC 779200' #TrackingRef '- LBZW01.cif' _audit_creation_date 2009-11-04 _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point 547 _chemical_formula_moiety 'C7 H7 N5' _chemical_formula_sum 'C7 H7 N5' _chemical_formula_weight 161.18 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' _symmetry_cell_setting Monoclinic _symmetry_space_group_name_H-M c_2/c _symmetry_space_group_name_Hall -C2yc loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, y, -z+1/2' 'x+1/2, y+1/2, z' '-x+1/2, y+1/2, -z+1/2' '-x, -y, -z' 'x, -y, z-1/2' '-x+1/2, -y+1/2, -z' 'x+1/2, -y+1/2, z-1/2' _cell_length_a 10.5257(10) _cell_length_b 10.8919(11) _cell_length_c 7.0298(7) _cell_angle_alpha 90.00 _cell_angle_beta 108.360(2) _cell_angle_gamma 90.00 _cell_volume 764.91(13) _cell_formula_units_Z 4 _cell_measurement_temperature 298(2) _cell_measurement_reflns_used 1012 _cell_measurement_theta_min 2.766 _cell_measurement_theta_max 24.566 _exptl_crystal_description prism _exptl_crystal_colour 'dark orange' _exptl_crystal_size_max 0.25 _exptl_crystal_size_mid 0.15 _exptl_crystal_size_min 0.15 _exptl_crystal_density_diffrn 1.400 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 336 _exptl_absorpt_coefficient_mu 0.096 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.9063 _exptl_absorpt_correction_T_max 1.0000 _exptl_absorpt_process_details SADABS-2007/4 _exptl_special_details ; ? ; _diffrn_ambient_temperature 298(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_measurement_device_type 'Bruker AXS Smart' _diffrn_measurement_method '\w scans' _diffrn_reflns_number 4877 _diffrn_reflns_av_R_equivalents 0.0258 _diffrn_reflns_av_sigmaI/netI 0.0161 _diffrn_reflns_limit_h_min -13 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min -14 _diffrn_reflns_limit_k_max 14 _diffrn_reflns_limit_l_min -9 _diffrn_reflns_limit_l_max 9 _diffrn_reflns_theta_min 2.77 _diffrn_reflns_theta_max 27.51 _reflns_number_total 878 _reflns_number_gt 623 _reflns_threshold_expression >2sigma(I) _computing_structure_refinement '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^)+(0.0382P)^2^+0.1800P] 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_number_reflns 878 _refine_ls_number_parameters 77 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0596 _refine_ls_R_factor_gt 0.0364 _refine_ls_wR_factor_ref 0.0950 _refine_ls_wR_factor_gt 0.0831 _refine_ls_goodness_of_fit_ref 1.076 _refine_ls_restrained_S_all 1.076 _refine_ls_shift/su_max 0.012 _refine_ls_shift/su_mean 0.001 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 0.5000 0.12982(16) 0.2500 0.0448(5) Uani 1 2 d S . . C2 C 0.5000 -0.00380(16) 0.2500 0.0427(4) Uani 1 2 d S . . C3 C 0.61306(14) -0.07005(13) 0.2516(2) 0.0508(4) Uani 1 1 d . . . C4 C 0.61061(15) -0.19554(14) 0.2507(2) 0.0551(4) Uani 1 1 d . . . C5 C 0.5000 -0.3921(2) 0.2500 0.0754(8) Uani 1 2 d S . . N1 N 0.5000 -0.25650(14) 0.2500 0.0531(5) Uani 1 2 d S . . N2 N 0.39713(12) 0.19817(11) 0.25869(18) 0.0566(4) Uani 1 1 d . . . N3 N 0.43879(13) 0.31422(11) 0.2553(2) 0.0661(4) Uani 1 1 d . . . H3 H 0.6960(16) -0.0286(12) 0.254(2) 0.060(4) Uiso 1 1 d . . . H4 H 0.6885(16) -0.2474(14) 0.250(2) 0.073(5) Uiso 1 1 d . . . H5A H 0.582(4) -0.421(3) 0.206(8) 0.078(11) Uiso 0.50 1 d P . . H5B H 0.411(4) -0.419(3) 0.141(7) 0.071(10) Uiso 0.50 1 d P . . H5C H 0.507(6) -0.417(3) 0.388(6) 0.077(11) Uiso 0.50 1 d P . . 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 0.0507(10) 0.0391(10) 0.0472(11) 0.000 0.0193(8) 0.000 C2 0.0492(10) 0.0374(10) 0.0445(10) 0.000 0.0190(8) 0.000 C3 0.0488(8) 0.0448(8) 0.0635(9) 0.0035(6) 0.0246(7) 0.0006(6) C4 0.0595(9) 0.0457(8) 0.0653(10) 0.0051(6) 0.0270(7) 0.0101(7) C5 0.117(3) 0.0346(11) 0.079(2) 0.000 0.037(2) 0.000 N1 0.0679(11) 0.0357(8) 0.0600(11) 0.000 0.0263(9) 0.000 N2 0.0627(8) 0.0387(6) 0.0743(9) 0.0000(5) 0.0299(6) 0.0055(5) N3 0.0816(9) 0.0395(7) 0.0831(9) 0.0005(6) 0.0346(8) 0.0068(6) _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 N2 1.3312(14) . ? C1 N2 1.3312(14) 2_655 ? C1 C2 1.455(2) . ? C2 C3 1.3887(17) 2_655 ? C2 C3 1.3887(17) . ? C3 C4 1.367(2) . ? C3 H3 0.978(15) . ? C4 N1 1.3390(17) . ? C4 H4 0.997(17) . ? C5 N1 1.477(3) . ? C5 H5A 1.05(4) . ? C5 H5B 1.04(4) . ? C5 H5C 0.98(4) . ? N1 C4 1.3390(17) 2_655 ? N2 N3 1.3406(17) . ? N3 N3 1.314(3) 2_655 ? 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 N2 C1 N2 111.99(16) . 2_655 ? N2 C1 C2 124.01(8) . . ? N2 C1 C2 124.01(8) 2_655 . ? C3 C2 C3 117.39(18) 2_655 . ? C3 C2 C1 121.30(9) 2_655 . ? C3 C2 C1 121.30(9) . . ? C4 C3 C2 120.31(14) . . ? C4 C3 H3 118.5(8) . . ? C2 C3 H3 121.2(8) . . ? N1 C4 C3 120.73(14) . . ? N1 C4 H4 115.8(9) . . ? C3 C4 H4 123.5(9) . . ? N1 C5 H5A 107.4(19) . . ? N1 C5 H5B 106.0(18) . . ? H5A C5 H5B 109(2) . . ? N1 C5 H5C 106(2) . . ? H5A C5 H5C 113(2) . . ? H5B C5 H5C 115(2) . . ? C4 N1 C4 120.54(17) . 2_655 ? C4 N1 C5 119.73(9) . . ? C4 N1 C5 119.73(9) 2_655 . ? C1 N2 N3 104.55(12) . . ? N3 N3 N2 109.46(7) 2_655 . ? loop_ _geom_torsion_atom_site_label_1 _geom_torsion_atom_site_label_2 _geom_torsion_atom_site_label_3 _geom_torsion_atom_site_label_4 _geom_torsion _geom_torsion_site_symmetry_1 _geom_torsion_site_symmetry_2 _geom_torsion_site_symmetry_3 _geom_torsion_site_symmetry_4 _geom_torsion_publ_flag N2 C1 C2 C3 3.52(9) . . . 2_655 ? N2 C1 C2 C3 -176.48(9) 2_655 . . 2_655 ? N2 C1 C2 C3 -176.48(9) . . . . ? N2 C1 C2 C3 3.52(9) 2_655 . . . ? C3 C2 C3 C4 0.28(10) 2_655 . . . ? C1 C2 C3 C4 -179.72(10) . . . . ? C2 C3 C4 N1 -0.6(2) . . . . ? C3 C4 N1 C4 0.29(10) . . . 2_655 ? C3 C4 N1 C5 -179.71(10) . . . . ? N2 C1 N2 N3 -0.04(7) 2_655 . . . ? C2 C1 N2 N3 179.96(7) . . . . ? C1 N2 N3 N3 0.10(18) . . . 2_655 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 27.51 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.153 _refine_diff_density_min -0.165 _refine_diff_density_rms 0.030