# 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 #TrackingRef '9490_web_deposit_cif_file_0_ToruOkawara_1328787363.865212.cif' _audit_creation_method 'APEX2 v2010.1-2' _publ_contact_author_name 'Toru Okawara' _publ_contact_author_address ; ; _publ_contact_author_email t-okawara@ms.hisaeda.cstm.kyushu-u.ac.jp _publ_contact_author_fax ? _publ_contact_author_phone ? _publ_section_title ; ; _publ_section_abstract ; ; _publ_section_references ; ; _publ_section_comment ; ; loop_ _publ_author_name 'Toru Okawara' 'Koichi Hashimoto' 'Masaaki Abe' 'Hisashi Shimakoshi' 'Yoshio Hisaeda' data_I _database_code_depnum_ccdc_archive 'CCDC 865212' #TrackingRef '9490_web_deposit_cif_file_0_ToruOkawara_1328787363.865212.cif' _audit_creation_method 'APEX2 v2010.1-2' _chemical_name_systematic ? _chemical_name_common ? _chemical_formula_moiety ? _chemical_formula_sum 'C32 H22 N4' _chemical_formula_iupac ? _chemical_formula_weight 462.54 _chemical_melting_point ? _space_group_crystal_system triclinic _space_group_name_H-M_alt 'P -1' _space_group_name_Hall '-P 1' loop_ _space_group_symop_operation_xyz 'x, y, z' '-x, -y, -z' _cell_length_a 6.799(2) _cell_length_b 8.080(3) _cell_length_c 12.822(4) _cell_angle_alpha 104.488(4) _cell_angle_beta 92.528(5) _cell_angle_gamma 96.782(5) _cell_volume 675.2(4) _cell_formula_units_Z 1 _cell_measurement_reflns_used 3110 _cell_measurement_theta_min 2.6271 _cell_measurement_theta_max 29.9946 _cell_measurement_temperature 17 _exptl_crystal_description prism _exptl_crystal_colour violet _exptl_crystal_size_max 0.68 _exptl_crystal_size_mid 0.16 _exptl_crystal_size_min 0.09 _exptl_crystal_density_diffrn 1.138 _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 242 _exptl_absorpt_coefficient_mu 0.068 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_process_details 'SADABS V2008/1 (Bruker AXS)' _exptl_absorpt_correction_T_min 0.69 _exptl_absorpt_correction_T_max 0.99 _exptl_special_details ; ; _diffrn_ambient_temperature 173 _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker SMART APEX CCD' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean 8.3333 _diffrn_reflns_number 8859 _diffrn_reflns_av_R_equivalents 0.0445 _diffrn_reflns_av_sigmaI/netI 0.0490 _diffrn_reflns_theta_min 1.65 _diffrn_reflns_theta_max 28.28 _diffrn_reflns_theta_full 28.28 _diffrn_measured_fraction_theta_max 0.996 _diffrn_measured_fraction_theta_full 0.996 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 9 _diffrn_reflns_limit_k_min -10 _diffrn_reflns_limit_k_max 10 _diffrn_reflns_limit_l_min -17 _diffrn_reflns_limit_l_max 17 _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. ; _reflns_number_total 3330 _reflns_number_gt 2176 _reflns_threshold_expression >2sigma(I) _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_R_factor_all 0.1268 _refine_ls_R_factor_gt 0.0908 _refine_ls_wR_factor_gt 0.1919 _refine_ls_wR_factor_ref 0.2093 _refine_ls_goodness_of_fit_ref 1.070 _refine_ls_restrained_S_all 1.073 _refine_ls_number_reflns 3330 _refine_ls_number_parameters 210 _refine_ls_number_restraints 12 _refine_ls_hydrogen_treatment constr _refine_ls_weighting_scheme calc _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.0100P)^2^+1.1000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_hydrogens geom _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _refine_ls_shift/su_max 0.000 _refine_ls_shift/su_mean 0.000 _refine_diff_density_max 0.395 _refine_diff_density_min -0.252 _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef 0.141(8) 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' _computing_data_collection ? _computing_cell_refinement 'SAINT V7.68A (Bruker AXS, 2009)' _computing_data_reduction 'SAINT V7.68A (Bruker AXS, 2009)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics ? _computing_publication_material ? loop_ _atom_site_type_symbol _atom_site_label _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_U_iso_or_equiv _atom_site_adp_type _atom_site_calc_flag _atom_site_refinement_flags _atom_site_occupancy _atom_site_disorder_assembly _atom_site_disorder_group C C2B 1.119(4) 0.792(3) 0.3307(17) 0.100(7) Uani d PU 0.5 A 1 C C3B 0.906(4) 0.678(3) 0.3156(19) 0.076(7) Uani d P 0.5 A 1 C C11B 1.2675(13) 0.7382(15) 0.4011(7) 0.087(3) Uani d P 0.5 A 1 C C12B 1.2148(14) 0.8024(15) 0.5184(6) 0.082(3) Uani d P 0.5 A 1 C C13B 1.3534(19) 0.6982(19) 0.5784(9) 0.119(4) Uani d P 0.5 A 1 C C2A 1.1250(18) 0.7925(13) 0.3257(8) 0.036(3) Uani d PU 0.5 A 2 C C3A 0.925(3) 0.707(3) 0.3072(12) 0.037(3) Uani d P 0.5 A 2 C C11A 1.2135(10) 0.8900(9) 0.4368(5) 0.0583(19) Uani d P 0.5 A 2 C C12A 1.3522(18) 0.7782(16) 0.4892(8) 0.099(3) Uani d P 0.5 A 2 C C13A 1.264(2) 0.6190(17) 0.5085(9) 0.105(4) Uani d P 0.5 A 2 C C1 1.2000(5) 0.7570(4) 0.2198(3) 0.0538(9) Uani d . 1 . . C C4 0.9031(5) 0.6046(4) 0.1955(3) 0.0499(8) Uani d . 1 . . C C5 0.7400(5) 0.4839(4) 0.1393(3) 0.0487(8) Uani d . 1 A . C C6 0.5607(5) 0.4256(4) 0.1762(3) 0.0529(8) Uani d . 1 . . H H6 0.5216 0.4624 0.2476 0.063 Uiso calc R 1 A . C C7 0.4513(5) 0.3070(4) 0.0927(3) 0.0495(8) Uani d . 1 A . C C8 0.5676(5) 0.2917(4) -0.0002(3) 0.0499(8) Uani d . 1 . . C C9 0.5162(5) 0.1880(4) -0.1041(3) 0.0536(9) Uani d . 1 . . H H9 0.3915 0.1173 -0.1123 0.064 Uiso calc R 1 . . C C10 1.3841(5) 0.8309(4) 0.1993(3) 0.0531(9) Uani d . 1 . . H H10 1.456 0.9086 0.2609 0.064 Uiso calc R 1 . . C C14 0.2475(5) 0.2091(4) 0.0910(3) 0.0562(9) Uani d . 1 . . H H14A 0.2533 0.0851 0.0587 0.067 Uiso calc R 1 A . H H14B 0.1546 0.2481 0.0433 0.067 Uiso calc R 1 . . C C15 0.1649(5) 0.2287(4) 0.1990(3) 0.0608(9) Uani d . 1 A . H H15A 0.1523 0.3517 0.2304 0.073 Uiso calc R 1 . . H H15B 0.2589 0.1934 0.2479 0.073 Uiso calc R 1 . . C C16 -0.0365(5) 0.1217(5) 0.1924(3) 0.0638(10) Uani d . 1 . . H H16A -0.1325 0.1615 0.1481 0.096 Uiso calc R 1 A . H H16B -0.0815 0.1343 0.2652 0.096 Uiso calc R 1 . . H H16C -0.0256 0.0001 0.1596 0.096 Uiso calc R 1 . . N N1 1.0673(3) 0.6446(3) 0.14590(19) 0.0413(6) Uani d . 1 A . H H1 1.0848 0.6043 0.077 0.05 Uiso calc PR 0.5 . . N N2 0.7428(4) 0.4028(3) 0.0341(2) 0.0454(7) Uani d . 1 A . H H2 0.8407 0.4179 -0.0066 0.054 Uiso calc PR 0.5 . . loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_12 _atom_site_aniso_U_13 _atom_site_aniso_U_23 C2B 0.102(10) 0.112(10) 0.100(9) 0.044(8) 0.020(7) 0.038(7) C3B 0.067(12) 0.051(8) 0.098(13) 0.009(7) -0.025(8) 0.000(7) C11B 0.072(6) 0.134(9) 0.059(5) 0.007(5) -0.007(4) 0.034(5) C12B 0.063(5) 0.146(10) 0.029(4) -0.003(6) -0.004(4) 0.014(4) C13B 0.127(10) 0.164(12) 0.076(7) 0.051(9) -0.012(7) 0.038(8) C2A 0.042(4) 0.034(4) 0.020(3) 0.007(3) -0.020(3) -0.012(3) C3A 0.033(5) 0.046(7) 0.025(4) -0.006(4) 0.006(3) 0.001(4) C11A 0.050(4) 0.059(4) 0.043(4) 0.007(3) -0.011(3) -0.028(3) C12A 0.097(8) 0.124(9) 0.054(6) -0.010(7) -0.029(5) -0.001(5) C13A 0.130(10) 0.124(9) 0.065(6) 0.030(8) -0.013(6) 0.029(6) C1 0.0532(19) 0.0405(16) 0.060(2) 0.0120(14) -0.0183(16) 0.0007(14) C4 0.0485(18) 0.0402(15) 0.057(2) 0.0102(13) -0.0149(15) 0.0070(14) C5 0.0486(18) 0.0389(15) 0.057(2) 0.0113(13) -0.0144(14) 0.0108(14) C6 0.0534(19) 0.0419(16) 0.062(2) 0.0096(14) -0.0131(15) 0.0116(14) C7 0.0443(17) 0.0402(15) 0.065(2) 0.0075(13) -0.0110(15) 0.0165(14) C8 0.0557(19) 0.0351(14) 0.0570(19) 0.0131(13) -0.0192(15) 0.0091(13) C9 0.0421(17) 0.0423(16) 0.070(2) 0.0025(13) -0.0166(16) 0.0073(15) C10 0.0433(17) 0.0401(16) 0.065(2) 0.0039(13) -0.0192(15) -0.0012(14) C14 0.055(2) 0.0447(17) 0.068(2) 0.0074(15) -0.0129(16) 0.0142(15) C15 0.061(2) 0.0475(18) 0.074(2) 0.0108(16) -0.0079(18) 0.0168(17) C16 0.055(2) 0.058(2) 0.080(3) 0.0059(16) -0.0017(18) 0.0224(18) N1 0.0420(14) 0.0350(12) 0.0430(13) 0.0056(10) -0.0115(11) 0.0051(10) N2 0.0414(13) 0.0352(12) 0.0573(16) 0.0046(10) -0.0150(11) 0.0111(11) _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_site_symmetry_2 _geom_bond_distance _geom_bond_publ_flag C2B C11B . 1.50(2) ? C2B C3B . 1.60(3) ? C2B C1 . 1.52(2) ? C3B C4 . 1.50(2) ? C11B C12B . 1.536(12) ? C12B C13B . 1.624(15) ? C2A C1 . 1.445(14) ? C2A C3A . 1.43(2) ? C2A C11A . 1.504(9) ? C3A C4 . 1.455(16) ? C11A C12A . 1.614(14) ? C12A C13A . 1.437(16) ? C1 N1 . 1.355(4) ? C1 C10 . 1.387(5) ? C4 N1 . 1.354(4) ? C4 C5 . 1.422(4) ? C5 N2 . 1.346(4) ? C5 C6 . 1.399(5) ? C6 C7 . 1.366(4) ? C6 H6 . 0.95 ? C7 C8 . 1.446(5) ? C7 C14 . 1.508(4) ? C8 C9 . 1.389(4) ? C8 N2 . 1.386(4) ? C9 C10 2_765 1.406(5) ? C9 H9 . 0.95 ? C10 C9 2_765 1.406(5) ? C10 H10 . 0.95 ? C14 C15 . 1.497(5) ? C14 H14A . 0.99 ? C14 H14B . 0.99 ? C15 C16 . 1.518(5) ? C15 H15A . 0.99 ? C15 H15B . 0.99 ? C16 H16A . 0.98 ? C16 H16B . 0.98 ? C16 H16C . 0.98 ? N1 H1 . 0.88 ? N2 H2 . 0.88 ? loop_ _geom_angle_atom_site_label_1 _geom_angle_atom_site_label_2 _geom_angle_atom_site_label_3 _geom_angle_site_symmetry_1 _geom_angle_site_symmetry_3 _geom_angle _geom_angle_publ_flag C11B C2B C3B . . 113.2(19) ? C11B C2B C1 . . 104.9(15) ? C3B C2B C1 . . 106.2(14) ? C4 C3B C2B . . 96.9(15) ? C2B C11B C12B . . 107.2(12) ? C11B C12B C13B . . 100.5(9) ? C1 C2A C3A . . 104.1(7) ? C1 C2A C11A . . 133.9(10) ? C3A C2A C11A . . 122.0(12) ? C2A C3A C4 . . 106.3(10) ? C2A C11A C12A . . 111.8(7) ? C13A C12A C11A . . 118.9(10) ? N1 C1 C2A . . 111.0(5) ? N1 C1 C10 . . 125.9(3) ? C2A C1 C10 . . 123.1(5) ? N1 C1 C2B . . 110.2(9) ? C2A C1 C2B . . 0.8(12) ? C10 C1 C2B . . 123.9(9) ? N1 C4 C5 . . 121.9(3) ? N1 C4 C3B . . 117.8(10) ? C5 C4 C3B . . 120.0(10) ? N1 C4 C3A . . 109.0(7) ? C5 C4 C3A . . 129.1(8) ? C3B C4 C3A . . 11.5(16) ? N2 C5 C6 . . 108.6(3) ? N2 C5 C4 . . 121.3(3) ? C6 C5 C4 . . 130.1(3) ? C7 C6 C5 . . 108.8(3) ? C7 C6 H6 . . 125.6 ? C5 C6 H6 . . 125.6 ? C6 C7 C8 . . 106.6(3) ? C6 C7 C14 . . 129.2(3) ? C8 C7 C14 . . 124.2(3) ? C9 C8 N2 . . 126.0(3) ? C9 C8 C7 . . 127.5(3) ? N2 C8 C7 . . 106.5(3) ? C8 C9 C10 . 2_765 131.4(3) ? C8 C9 H9 . . 114.3 ? C10 C9 H9 2_765 . 114.3 ? C1 C10 C9 . 2_765 131.8(3) ? C1 C10 H10 . . 114.1 ? C9 C10 H10 2_765 . 114.1 ? C7 C14 C15 . . 115.0(3) ? C7 C14 H14A . . 108.5 ? C15 C14 H14A . . 108.5 ? C7 C14 H14B . . 108.5 ? C15 C14 H14B . . 108.5 ? H14A C14 H14B . . 107.5 ? C14 C15 C16 . . 112.4(3) ? C14 C15 H15A . . 109.1 ? C16 C15 H15A . . 109.1 ? C14 C15 H15B . . 109.1 ? C16 C15 H15B . . 109.1 ? H15A C15 H15B . . 107.8 ? C15 C16 H16A . . 109.5 ? C15 C16 H16B . . 109.5 ? H16A C16 H16B . . 109.5 ? C15 C16 H16C . . 109.5 ? H16A C16 H16C . . 109.5 ? H16B C16 H16C . . 109.5 ? C4 N1 C1 . . 108.8(3) ? C4 N1 H1 . . 125.6 ? C1 N1 H1 . . 125.6 ? C5 N2 C8 . . 109.5(3) ? C5 N2 H2 . . 125.2 ? C8 N2 H2 . . 125.2 ?