# Supplementary Material (ESI) for Journal of Materials Chemistry # This journal is (C) The Royal Society of Chemistry 2007 data_global _journal_name_full J.Mater.Chem. _journal_coden_Cambridge 1145 _publ_contact_author_name 'Yu-Peng Tian' _publ_contact_author_address ; Department of Chemistry Anhui University Longhe Road Hefei 230039 CHINA ; _publ_contact_author_email YPTIAN@AHU.EDU.CN _publ_section_title ; Investigations and facile synthesis of a series of novel multi-functional two-photon materials ; loop_ _publ_author_name 'Yu-Peng Tian' 'Ya-Hui Guo' 'Wen-Hao Huang' 'Min-Hua Jiang' 'Lin Li' ; Ping-Ping Sun ; 'Xutang Tao' 'Li-Min Tao' 'Chuan-Kui Wang' 'Jie-Ying Wu' 'Hui Xing' ; Jia-Xiang Yang ; 'Ju-Zhou Zhang' 'Hongping zhou' data_tian245 _database_code_depnum_ccdc_archive 'CCDC 648000' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C27 H18 N4' _chemical_formula_weight 398.45 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 Rhombohedral _symmetry_space_group_name_H-M 'R-3 ' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x-y, z' '-x+y, -x, z' 'x+2/3, y+1/3, z+1/3' '-y+2/3, x-y+1/3, z+1/3' '-x+y+2/3, -x+1/3, z+1/3' 'x+1/3, y+2/3, z+2/3' '-y+1/3, x-y+2/3, z+2/3' '-x+y+1/3, -x+2/3, z+2/3' '-x, -y, -z' 'y, -x+y, -z' 'x-y, x, -z' '-x+2/3, -y+1/3, -z+1/3' 'y+2/3, -x+y+1/3, -z+1/3' 'x-y+2/3, x+1/3, -z+1/3' '-x+1/3, -y+2/3, -z+2/3' 'y+1/3, -x+y+2/3, -z+2/3' 'x-y+1/3, x+2/3, -z+2/3' _cell_length_a 15.244(5) _cell_length_b 15.244(5) _cell_length_c 16.059(5) _cell_angle_alpha 90.000(5) _cell_angle_beta 90.000(5) _cell_angle_gamma 120.000(5) _cell_volume 3231.8(18) _cell_formula_units_Z 6 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description ? _exptl_crystal_colour ? _exptl_crystal_size_max 0.45 _exptl_crystal_size_mid 0.37 _exptl_crystal_size_min 0.23 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.228 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1248 _exptl_absorpt_coefficient_mu 0.074 _exptl_absorpt_correction_type ? _exptl_absorpt_correction_T_min 0.9673 _exptl_absorpt_correction_T_max 0.9831 _exptl_absorpt_process_details ? _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_wavelength 0.71069 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type ? _diffrn_measurement_method ? _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 7129 _diffrn_reflns_av_R_equivalents 0.0629 _diffrn_reflns_av_sigmaI/netI 0.0709 _diffrn_reflns_limit_h_min -19 _diffrn_reflns_limit_h_max 20 _diffrn_reflns_limit_k_min -18 _diffrn_reflns_limit_k_max 20 _diffrn_reflns_limit_l_min -21 _diffrn_reflns_limit_l_max 20 _diffrn_reflns_theta_min 2.00 _diffrn_reflns_theta_max 28.57 _reflns_number_total 1806 _reflns_number_gt 701 _reflns_threshold_expression >2sigma(I) _computing_data_collection ? _computing_cell_refinement ? _computing_data_reduction ? _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics ? _computing_publication_material ? _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^)+(0.0673P)^2^+10.6538P] 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 1806 _refine_ls_number_parameters 94 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.1803 _refine_ls_R_factor_gt 0.0757 _refine_ls_wR_factor_ref 0.2335 _refine_ls_wR_factor_gt 0.1830 _refine_ls_goodness_of_fit_ref 0.939 _refine_ls_restrained_S_all 0.939 _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 N1 N 1.0000 1.0000 0.3515(3) 0.0541(12) Uani 1 3 d S . . C1 C 0.9201(2) 0.8981(2) 0.3601(2) 0.0508(8) Uani 1 1 d . . . C6 C 0.9301(3) 0.8298(2) 0.4100(2) 0.0566(9) Uani 1 1 d . . . H6 H 0.9914 0.8488 0.4363 0.068 Uiso 1 1 calc R . . C5 C 0.8483(3) 0.7326(3) 0.4208(2) 0.0634(10) Uani 1 1 d . . . H5 H 0.8559 0.6870 0.4541 0.076 Uiso 1 1 calc R . . C3 C 0.7483(3) 0.7700(3) 0.3328(3) 0.0725(11) Uani 1 1 d . . . H3 H 0.6870 0.7508 0.3064 0.087 Uiso 1 1 calc R . . C2 C 0.8284(3) 0.8657(3) 0.3198(2) 0.0655(10) Uani 1 1 d . . . H2 H 0.8211 0.9093 0.2836 0.079 Uiso 1 1 calc R . . C4 C 0.7558(3) 0.7022(3) 0.3833(2) 0.0651(10) Uani 1 1 d . . . C7 C 0.6636(3) 0.6016(3) 0.3988(3) 0.0848(13) Uani 1 1 d . . . H7 H 0.6026 0.5924 0.3782 0.102 Uiso 1 1 calc R . . C8 C 0.6606(4) 0.5292(3) 0.4367(3) 0.0922(14) Uani 1 1 d . . . H8 H 0.7216 0.5348 0.4535 0.111 Uiso 1 1 calc R . . C9 C 0.5674(4) 0.4358(4) 0.4565(3) 0.0972(15) Uani 1 1 d . . . N2 N 0.4961(3) 0.3616(3) 0.4757(3) 0.1148(15) Uani 1 1 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 N1 0.0462(16) 0.0462(16) 0.070(3) 0.000 0.000 0.0231(8) C1 0.0482(19) 0.0459(18) 0.0567(19) -0.0051(15) 0.0008(15) 0.0223(15) C6 0.061(2) 0.054(2) 0.059(2) -0.0034(16) -0.0038(16) 0.0317(18) C5 0.081(3) 0.049(2) 0.064(2) 0.0015(17) 0.002(2) 0.036(2) C3 0.057(2) 0.061(2) 0.085(3) -0.003(2) -0.012(2) 0.0183(19) C2 0.058(2) 0.057(2) 0.075(2) 0.0018(18) -0.0099(18) 0.0236(18) C4 0.060(2) 0.049(2) 0.072(2) -0.0101(18) -0.0022(19) 0.0165(18) C7 0.089(3) 0.069(3) 0.090(3) -0.008(2) -0.014(2) 0.034(2) C8 0.099(3) 0.071(3) 0.099(3) 0.002(3) 0.003(3) 0.036(3) C9 0.103(4) 0.063(3) 0.103(4) 0.000(3) 0.003(3) 0.024(3) N2 0.102(3) 0.066(2) 0.143(4) 0.010(3) -0.003(3) 0.018(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 N1 C1 1.423(3) 2_765 ? N1 C1 1.423(3) . ? N1 C1 1.423(3) 3_675 ? C1 C6 1.381(4) . ? C1 C2 1.389(4) . ? C6 C5 1.390(5) . ? C5 C4 1.383(5) . ? C3 C4 1.362(5) . ? C3 C2 1.372(5) . ? C4 C7 1.494(5) . ? C7 C8 1.241(5) . ? C8 C9 1.458(6) . ? C9 N2 1.151(5) . ? 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 C1 N1 C1 119.07(8) 2_765 . ? C1 N1 C1 119.07(8) 2_765 3_675 ? C1 N1 C1 119.07(8) . 3_675 ? C6 C1 C2 118.3(3) . . ? C6 C1 N1 121.5(3) . . ? C2 C1 N1 120.2(3) . . ? C5 C6 C1 119.8(3) . . ? C6 C5 C4 121.6(3) . . ? C4 C3 C2 122.1(4) . . ? C3 C2 C1 120.6(3) . . ? C3 C4 C5 117.6(3) . . ? C3 C4 C7 119.1(4) . . ? C5 C4 C7 123.3(4) . . ? C8 C7 C4 126.3(5) . . ? C7 C8 C9 124.0(5) . . ? N2 C9 C8 176.5(6) . . ? 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 C1 N1 C1 C6 29.0(6) 2_765 . . . ? C1 N1 C1 C6 -131.9(3) 3_675 . . . ? C1 N1 C1 C2 -152.8(3) 2_765 . . . ? C1 N1 C1 C2 46.4(6) 3_675 . . . ? C2 C1 C6 C5 -2.1(5) . . . . ? N1 C1 C6 C5 176.1(3) . . . . ? C1 C6 C5 C4 -0.6(5) . . . . ? C4 C3 C2 C1 -2.0(6) . . . . ? C6 C1 C2 C3 3.4(5) . . . . ? N1 C1 C2 C3 -174.9(3) . . . . ? C2 C3 C4 C5 -0.8(6) . . . . ? C2 C3 C4 C7 176.1(4) . . . . ? C6 C5 C4 C3 2.0(5) . . . . ? C6 C5 C4 C7 -174.7(3) . . . . ? C3 C4 C7 C8 172.9(5) . . . . ? C5 C4 C7 C8 -10.4(7) . . . . ? C4 C7 C8 C9 174.4(4) . . . . ? C7 C8 C9 N2 -149(9) . . . . ? _diffrn_measured_fraction_theta_max 0.980 _diffrn_reflns_theta_full 28.57 _diffrn_measured_fraction_theta_full 0.980 _refine_diff_density_max 0.449 _refine_diff_density_min -0.177 _refine_diff_density_rms 0.050