# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2011 data_global _journal_name_full Chem.Commun. _journal_coden_Cambridge 0182 _journal_volume ? _journal_page_first ? _journal_year ? _publ_contact_author_name 'Guoping Yong' _publ_contact_author_email gpyong@ustc.edu.cn _publ_section_title ; From zwitterionic radical to neutral radical with unusual magnetic properties: First K-promoted air oxidative ring opening reaction of aromatic N-heterocycle ; loop_ _publ_author_name 'Guoping Yong.' 'Yimen Zhang' 'Chongfu Li.' 'Yingzhou Li.' 'Yongshou Li' 'Wenlong She' # Attachment '- Compd2.cif' data_1 _database_code_depnum_ccdc_archive 'CCDC 764965' #TrackingRef '- Compd2.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C14 H10 N4 O2' _chemical_formula_weight 266.26 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 '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 0.0311 0.0180 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0492 0.0322 '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 c a 21' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z+1/2' '-x+1/2, y, z+1/2' 'x+1/2, -y, z' _cell_length_a 27.0027(16) _cell_length_b 3.8705(2) _cell_length_c 11.6121(7) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1213.63(12) _cell_formula_units_Z 4 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used 1873 _cell_measurement_theta_min 3.2699 _cell_measurement_theta_max 62.6935 _exptl_crystal_description block _exptl_crystal_colour yellow _exptl_crystal_size_max 0.34 _exptl_crystal_size_mid 0.30 _exptl_crystal_size_min 0.26 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.457 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 552 _exptl_absorpt_coefficient_mu 0.845 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.788 _exptl_absorpt_correction_T_max 0.803 _exptl_absorpt_process_details ; CrysAlisPro, Oxford Diffraction Ltd., Version 1.171.33.46 (release 27-08-2009 CrysAlis171 .NET) (compiled Aug 27 2009,17:19:36) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. ; _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_wavelength 1.54184 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'Enhance Ultra (Cu) X-ray Source' _diffrn_radiation_monochromator mirror _diffrn_measurement_device_type 'Xcalibur, Sapphire3, Gemini ultra' _diffrn_measurement_method '\w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 2353 _diffrn_reflns_av_R_equivalents 0.0317 _diffrn_reflns_av_sigmaI/netI 0.0249 _diffrn_reflns_limit_h_min -31 _diffrn_reflns_limit_h_max 30 _diffrn_reflns_limit_k_min -4 _diffrn_reflns_limit_k_max 2 _diffrn_reflns_limit_l_min -13 _diffrn_reflns_limit_l_max 12 _diffrn_reflns_theta_min 3.27 _diffrn_reflns_theta_max 62.81 _reflns_number_total 1359 _reflns_number_gt 1249 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrysAlisPro (Oxford Diffraction Ltd.)' _computing_cell_refinement 'CrysAlisPro (Oxford Diffraction Ltd.)' _computing_data_reduction 'CrysAlisPro (Oxford Diffraction Ltd.)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1997)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'Ortep-3 (L. J. Farrugia, 2001)' _computing_publication_material SHELXL-97 _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^)+(0.0331P)^2^+0.9850P] 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 0.2(6) _refine_ls_number_reflns 1359 _refine_ls_number_parameters 185 _refine_ls_number_restraints 2 _refine_ls_R_factor_all 0.0478 _refine_ls_R_factor_gt 0.0448 _refine_ls_wR_factor_ref 0.1061 _refine_ls_wR_factor_gt 0.1049 _refine_ls_goodness_of_fit_ref 1.024 _refine_ls_restrained_S_all 1.023 _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 O2 O 0.85630(10) 0.7766(10) 0.1347(2) 0.0706(9) Uani 1 1 d . . . N1 N 0.72535(10) 0.3685(8) 0.3347(2) 0.0447(8) Uani 1 1 d . . . N2 N 0.76365(11) 0.4581(9) 0.1658(3) 0.0538(8) Uani 1 1 d . . . N3 N 0.91219(12) 1.0348(10) 0.2974(3) 0.0537(8) Uani 1 1 d D . . O1 O 0.86073(10) 0.8039(9) 0.4337(3) 0.0662(8) Uani 1 1 d . . . C14 C 0.68842(13) 0.2527(11) 0.4068(3) 0.0536(10) Uani 1 1 d . . . H14 H 0.6906 0.2829 0.4861 0.064 Uiso 1 1 calc R . . C11 C 0.68159(14) 0.1627(12) 0.1683(4) 0.0587(11) Uani 1 1 d . . . H11 H 0.6788 0.1308 0.0892 0.070 Uiso 1 1 calc R . . C8 C 0.79187(12) 0.5824(10) 0.2551(3) 0.0451(9) Uani 1 1 d . . . C10 C 0.72363(14) 0.3300(11) 0.2153(3) 0.0481(10) Uani 1 1 d . . . C2 C 1.03376(17) 1.4070(13) 0.4706(4) 0.0691(13) Uani 1 1 d . . . H2 H 1.0625 1.4905 0.5049 0.083 Uiso 1 1 calc R . . C5 C 0.95241(13) 1.1602(10) 0.3631(4) 0.0507(10) Uani 1 1 d . . . C9 C 0.76889(12) 0.5319(10) 0.3594(4) 0.0480(9) Uani 1 1 d . . . H9 H 0.7806 0.5957 0.4317 0.058 Uiso 1 1 calc R . . C4 C 0.95406(16) 1.1559(13) 0.4823(4) 0.0641(12) Uani 1 1 d . . . H4 H 0.9275 1.0723 0.5250 0.077 Uiso 1 1 calc R . . N4 N 0.98848(11) 1.2886(9) 0.2979(3) 0.0609(9) Uani 1 1 d . . . C7 C 0.83960(13) 0.7413(11) 0.2312(3) 0.0501(9) Uani 1 1 d . . . C13 C 0.64914(13) 0.0949(12) 0.3593(4) 0.0548(10) Uani 1 1 d . . . H13 H 0.6239 0.0139 0.4065 0.066 Uiso 1 1 calc R . . C6 C 0.87164(13) 0.8658(10) 0.3333(3) 0.0501(9) Uani 1 1 d . . . C3 C 0.99569(18) 1.2778(14) 0.5358(4) 0.0723(14) Uani 1 1 d . . . H3 H 0.9981 1.2730 0.6156 0.087 Uiso 1 1 calc R . . C12 C 0.64555(15) 0.0501(12) 0.2395(4) 0.0591(11) Uani 1 1 d . . . H12 H 0.6179 -0.0591 0.2088 0.071 Uiso 1 1 calc R . . C1 C 1.02817(15) 1.4091(13) 0.3541(5) 0.0663(12) Uani 1 1 d . . . H1 H 1.0538 1.5012 0.3104 0.080 Uiso 1 1 calc R . . H5 H 0.9182(17) 1.040(13) 0.2212(18) 0.079(16) Uiso 1 1 d D . . 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 O2 0.0667(17) 0.103(3) 0.0423(17) -0.0023(18) 0.0052(15) -0.0162(17) N1 0.0450(15) 0.0513(17) 0.0377(17) 0.0002(15) -0.0015(14) 0.0031(14) N2 0.0552(17) 0.065(2) 0.0415(16) -0.0083(19) -0.0006(16) -0.0031(15) N3 0.0534(17) 0.064(2) 0.0435(19) 0.0013(19) 0.0022(15) -0.0061(15) O1 0.0635(15) 0.092(2) 0.0433(16) -0.0045(18) 0.0047(14) -0.0144(16) C14 0.060(2) 0.061(2) 0.039(2) 0.001(2) 0.0028(18) 0.001(2) C11 0.062(2) 0.069(3) 0.045(2) -0.010(2) -0.010(2) -0.008(2) C8 0.0466(17) 0.051(2) 0.038(2) -0.0019(18) 0.0000(16) 0.0038(16) C10 0.053(2) 0.056(3) 0.035(2) -0.0006(19) -0.0004(17) 0.0034(19) C2 0.059(2) 0.068(3) 0.081(4) -0.009(3) -0.013(2) -0.001(2) C5 0.047(2) 0.053(2) 0.052(2) -0.002(2) 0.0005(19) 0.0026(17) C9 0.0475(17) 0.056(2) 0.0404(19) -0.005(2) -0.0028(17) 0.0017(16) C4 0.060(2) 0.080(3) 0.052(3) -0.001(3) 0.002(2) -0.010(2) N4 0.0546(18) 0.068(2) 0.060(2) 0.000(2) 0.0049(18) -0.0087(17) C7 0.0488(19) 0.059(2) 0.042(2) -0.0011(19) 0.0042(18) 0.0068(18) C13 0.0478(19) 0.060(2) 0.057(2) 0.001(2) 0.003(2) -0.0053(18) C6 0.0481(19) 0.055(2) 0.047(2) 0.002(2) 0.0059(17) 0.0058(18) C3 0.074(3) 0.085(4) 0.058(3) -0.010(3) -0.009(2) 0.000(3) C12 0.056(2) 0.062(3) 0.060(3) -0.001(2) -0.010(2) -0.007(2) C1 0.054(2) 0.065(3) 0.080(3) 0.006(3) 0.005(2) -0.009(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 O2 C7 1.216(5) . ? N1 C9 1.366(5) . ? N1 C14 1.377(5) . ? N1 C10 1.395(4) . ? N2 C10 1.320(5) . ? N2 C8 1.373(5) . ? N3 C6 1.342(5) . ? N3 C5 1.413(5) . ? O1 C6 1.226(5) . ? C14 C13 1.342(5) . ? C11 C12 1.349(6) . ? C11 C10 1.416(5) . ? C8 C9 1.376(5) . ? C8 C7 1.455(5) . ? C2 C1 1.361(7) . ? C2 C3 1.371(7) . ? C5 N4 1.330(5) . ? C5 C4 1.385(6) . ? C4 C3 1.368(7) . ? N4 C1 1.339(6) . ? C7 C6 1.545(5) . ? C13 C12 1.405(6) . ? 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 C9 N1 C14 130.2(3) . . ? C9 N1 C10 106.7(3) . . ? C14 N1 C10 123.1(3) . . ? C10 N2 C8 104.9(3) . . ? C6 N3 C5 128.9(4) . . ? C13 C14 N1 118.0(4) . . ? C12 C11 C10 119.3(4) . . ? N2 C8 C9 111.4(3) . . ? N2 C8 C7 119.7(3) . . ? C9 C8 C7 128.9(4) . . ? N2 C10 N1 111.4(4) . . ? N2 C10 C11 131.3(4) . . ? N1 C10 C11 117.3(4) . . ? C1 C2 C3 117.9(4) . . ? N4 C5 C4 123.4(4) . . ? N4 C5 N3 112.6(4) . . ? C4 C5 N3 124.0(4) . . ? N1 C9 C8 105.6(4) . . ? C3 C4 C5 118.4(4) . . ? C5 N4 C1 116.0(4) . . ? O2 C7 C8 123.5(4) . . ? O2 C7 C6 117.7(3) . . ? C8 C7 C6 118.8(3) . . ? C14 C13 C12 121.2(4) . . ? O1 C6 N3 125.9(4) . . ? O1 C6 C7 122.3(3) . . ? N3 C6 C7 111.8(3) . . ? C4 C3 C2 119.4(5) . . ? C11 C12 C13 121.1(4) . . ? N4 C1 C2 124.9(5) . . ? _diffrn_measured_fraction_theta_max 0.987 _diffrn_reflns_theta_full 62.81 _diffrn_measured_fraction_theta_full 0.986 _refine_diff_density_max 0.234 _refine_diff_density_min -0.180 _refine_diff_density_rms 0.048