# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2013 ####################################################################### # # Cambridge Crystallographic Data Centre # CCDC # ####################################################################### # # This CIF contains data from an original supplementary publication # deposited with the CCDC, and may include chemical, crystal, # experimental, refinement, atomic coordinates, # anisotropic displacement parameters and molecular geometry data, # as required by the journal to which it was submitted. # # This CIF is provided on the understanding that it is used for bona # fide research purposes only. It may contain copyright material # of the CCDC or of third parties, and may not be copied or further # disseminated in any form, whether machine-readable or not, # except for the purpose of generating routine backup copies # on your local computer system. # # For further information on the CCDC, data deposition and # data retrieval see: # www.ccdc.cam.ac.uk # # Bona fide researchers may freely download Mercury and enCIFer # from this site to visualise CIF-encoded structures and # to carry out CIF format checking respectively. # ####################################################################### data_ab47-iiip _database_code_depnum_ccdc_archive 'CCDC 924716' #TrackingRef '17817_web_deposit_cif_file_0_ChristophJaniak_1361026650.ab47-iiip_final.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; tetra(4-cyanophenyl)ethylene ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C30 H16 N4' _chemical_formula_sum 'C30 H16 N4' _chemical_formula_weight 432.27 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 Tetragonal _symmetry_space_group_name_H-M 'I 41/a c d' _symmetry_space_group_name_Hall '-I 4bd 2c' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-y+1/4, x+3/4, z+1/4' 'y+1/4, -x+1/4, z+3/4' '-x+1/2, y, -z' 'x, -y, -z+1/2' 'y+1/4, x+3/4, -z+3/4' '-y+1/4, -x+1/4, -z+1/4' 'x+1/2, y+1/2, z+1/2' '-x+1, -y+1/2, z+1' '-y+3/4, x+5/4, z+3/4' 'y+3/4, -x+3/4, z+5/4' '-x+1, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z+1' 'y+3/4, x+5/4, -z+5/4' '-y+3/4, -x+3/4, -z+3/4' '-x, -y, -z' 'x-1/2, y, -z-1/2' 'y-1/4, -x-3/4, -z-1/4' '-y-1/4, x-1/4, -z-3/4' 'x-1/2, -y, z' '-x, y, z-1/2' '-y-1/4, -x-3/4, z-3/4' 'y-1/4, x-1/4, z-1/4' '-x+1/2, -y+1/2, -z+1/2' 'x, y+1/2, -z' 'y+1/4, -x-1/4, -z+1/4' '-y+1/4, x+1/4, -z-1/4' 'x, -y+1/2, z+1/2' '-x+1/2, y+1/2, z' '-y+1/4, -x-1/4, z-1/4' 'y+1/4, x+1/4, z+1/4' _cell_length_a 22.0767(8) _cell_length_b 22.0767(8) _cell_length_c 21.1707(10) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 10318.2(7) _cell_formula_units_Z 16 _cell_measurement_temperature 173(2) _cell_measurement_reflns_used 4210 _cell_measurement_theta_min 4.005 _cell_measurement_theta_max 39.53 _exptl_crystal_description block _exptl_crystal_colour colorless _exptl_crystal_size_max 0.3 _exptl_crystal_size_mid 0.3 _exptl_crystal_size_min 0.2 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.134 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 3656 _exptl_absorpt_coefficient_mu 0.543 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.5672 _exptl_absorpt_correction_T_max 0.7478 _exptl_absorpt_process_details '(SADABS; Sheldrick, 1996)' _exptl_special_details ; Several crystals of the compound were measured both at room and low temperature. Because of the high symmetry not only small crystals but also larger crystals of the size up to 0.3 x 0.3 x 0.2 did not diffract above a 2Theta angle of 77 deg. For this reason it was decided to limit the 2Theta angle to 79 deg for the given measurement, which causes the Alerts level A: "ratio of reflections to parameters < 6", "value of sine(theta_max)/wavelength is less than 0.550" and "poor data / parameter ratio". ; _diffrn_ambient_temperature 173(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker Kappa APEX II CCD area detector' _diffrn_measurement_method '\f and \w scans' _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 10906 _diffrn_reflns_av_R_equivalents 0.0295 _diffrn_reflns_av_sigmaI/netI 0.0139 _diffrn_reflns_limit_h_min -17 _diffrn_reflns_limit_h_max 16 _diffrn_reflns_limit_k_min -18 _diffrn_reflns_limit_k_max 17 _diffrn_reflns_limit_l_min -17 _diffrn_reflns_limit_l_max 17 _diffrn_reflns_theta_min 4.00 _diffrn_reflns_theta_max 39.53 _reflns_number_total 753 _reflns_number_gt 665 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'APEX2 (Bruker, 2006)' _computing_cell_refinement 'SAINT (Bruker, 2006)' _computing_data_reduction SAINT _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008), PLATON (Spek, 2009)' _computing_molecular_graphics 'DIAMOND (Crystal Impact, 2009)' _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. ; loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 0.000 0.250 -0.004 437 101 ' ' 2 0.000 0.750 -0.017 437 101 ' ' 3 0.500 0.250 -0.021 437 101 ' ' 4 0.500 0.750 -0.008 437 101 ' ' _platon_squeeze_details ; The unit cell contains 4 ethanol molecules which have been treated as a diffuse contribution to the overall scattering without specific atom positions by SQUEEZE/PLATON ; _iucr_refine_instructions_details ; TITL AB47-II in I4(1)/acd CELL 1.54178 22.0767 22.0767 21.1707 90.000 90.000 90.000 ZERR 16.00 0.0008 0.0008 0.0010 0.000 0.000 0.000 LATT 2 SYMM 1/2 - X, - Y, 1/2 + Z SYMM 1/4 - Y, 3/4 + X, 1/4 + Z SYMM 1/4 + Y, 1/4 - X, 3/4 + Z SYMM 1/2 - X, Y, - Z SYMM X, - Y, 1/2 - Z SYMM 1/4 + Y, 3/4 + X, 3/4 - Z SYMM 1/4 - Y, 1/4 - X, 1/4 - Z SFAC C H N O UNIT 488 280 64 4 TEMP -100.00 MERG 2 FMAP 2 PLAN 1 ACTA BOND $H L.S. 40 WGHT 0.086300 29.228500 EXTI 0.000025 FVAR 0.36125 C1 1 0.105125 0.067417 0.920077 11.00000 0.07836 0.07405 = 0.05675 -0.00762 -0.00613 -0.00289 C2 1 0.132108 0.109036 0.882918 11.00000 0.09273 0.07164 = 0.06612 -0.01099 -0.02640 0.03844 AFIX 43 H2 2 0.108724 0.141167 0.865703 11.00000 -1.20000 AFIX 0 C3 1 0.192660 0.105684 0.869637 11.00000 0.09271 0.04713 = 0.06940 0.00370 -0.01264 0.00413 C4 1 0.226629 0.057477 0.893961 11.00000 0.03186 0.06584 = 0.07396 -0.00065 -0.00078 -0.02071 C5 1 0.200339 0.014615 0.930812 11.00000 0.03295 0.05477 = 0.06766 -0.00887 0.00872 -0.00380 C6 1 0.138719 0.019138 0.943951 11.00000 0.09349 0.04382 = 0.04488 0.00195 0.00197 -0.02237 C7 1 0.040468 0.071744 0.933815 11.00000 0.06405 0.14945 = 0.09055 -0.05139 -0.00457 0.01584 C8 1 0.293723 0.043723 0.875000 10.50000 0.12315 0.12315 = 0.06248 0.05187 -0.05187 -0.08426 C9 1 0.333157 0.083157 0.875000 10.50000 0.11790 0.11790 = 0.06485 0.02733 -0.02733 -0.00870 C10 1 0.324161 0.149498 0.899027 11.00000 0.08883 0.06357 = 0.06362 0.00104 -0.01550 0.00557 C11 1 0.330127 0.196647 0.855899 11.00000 0.12247 0.09151 = 0.06478 0.02598 -0.01206 -0.00560 AFIX 43 H11 2 0.333772 0.188317 0.812039 11.00000 -1.20000 AFIX 0 C12 1 0.330689 0.254236 0.876916 11.00000 0.11815 0.06382 = 0.11042 0.02661 -0.04128 -0.02506 AFIX 43 H12A 2 0.333552 0.286866 0.847814 11.00000 -1.20000 AFIX 0 C13 1 0.327176 0.265355 0.939310 11.00000 0.16772 0.03623 = 0.10562 -0.00438 -0.06402 -0.01972 C14 1 0.321027 0.219120 0.982371 11.00000 0.15569 0.05746 = 0.08561 0.01320 -0.03703 0.00451 AFIX 43 H14A 2 0.317903 0.227717 1.026219 11.00000 -1.20000 AFIX 0 C15 1 0.319466 0.160418 0.961166 11.00000 0.09568 0.04826 = 0.07304 0.01269 -0.01589 -0.00307 C16 1 0.331723 0.325621 0.958411 11.00000 0.34304 0.07451 = 0.14996 0.01566 -0.13517 -0.00837 N1 3 -0.008762 0.077001 0.945833 11.00000 0.05803 0.25704 = 0.14642 -0.08191 -0.02067 0.03880 N2 3 0.331115 0.376017 0.976665 11.00000 0.66205 0.07920 = 0.21653 0.00337 -0.25616 -0.01788 H3 2 0.220734 0.131820 0.839572 11.00000 0.08212 H5 2 0.227958 -0.028340 0.947218 11.00000 0.08982 H6 2 0.121694 -0.007839 0.970382 11.00000 0.01044 H15 2 0.313720 0.126842 0.990629 11.00000 0.06880 HKLF 4 REM AB47-II in I4(1)/acd REM R1 = 0.0592 for 665 Fo > 4sig(Fo) and 0.0660 for all 753 data REM 172 parameters refined using 0 restraints END ; _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^)+(0.0863P)^2^+29.2285P] 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 SHELXL _refine_ls_extinction_coef 0.000025(19) _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 753 _refine_ls_number_parameters 172 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0660 _refine_ls_R_factor_gt 0.0592 _refine_ls_wR_factor_ref 0.1693 _refine_ls_wR_factor_gt 0.1643 _refine_ls_goodness_of_fit_ref 1.105 _refine_ls_restrained_S_all 1.105 _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 C1 C 0.1051(4) 0.0674(6) 0.9201(5) 0.070(2) Uani 1 1 d . . . C2 C 0.1321(6) 0.1090(4) 0.8829(5) 0.077(2) Uani 1 1 d . . . H2 H 0.1087 0.1412 0.8657 0.092 Uiso 1 1 calc R . . C3 C 0.1927(6) 0.1057(4) 0.8696(3) 0.070(2) Uani 1 1 d . . . C4 C 0.2266(3) 0.0575(5) 0.8940(4) 0.057(2) Uani 1 1 d . . . C5 C 0.2003(5) 0.0146(4) 0.9308(4) 0.0518(19) Uani 1 1 d . . . C6 C 0.1387(6) 0.0191(4) 0.9440(4) 0.061(2) Uani 1 1 d . . . C7 C 0.0405(5) 0.0717(3) 0.9338(3) 0.101(3) Uani 1 1 d . . . C8 C 0.2937(6) 0.0437(6) 0.8750 0.103(6) Uani 1 2 d S . . C9 C 0.3332(7) 0.0832(7) 0.8750 0.100(4) Uani 1 2 d S . . C10 C 0.3242(3) 0.1495(4) 0.8990(6) 0.072(2) Uani 1 1 d . . . C11 C 0.3301(3) 0.1966(7) 0.8559(4) 0.093(2) Uani 1 1 d . . . H11 H 0.3338 0.1883 0.8120 0.112 Uiso 1 1 calc R . . C12 C 0.3307(3) 0.2542(6) 0.8769(7) 0.097(3) Uani 1 1 d . . . H12A H 0.3336 0.2869 0.8478 0.117 Uiso 1 1 calc R . . C13 C 0.3272(4) 0.2654(4) 0.9393(7) 0.103(3) Uani 1 1 d . . . C14 C 0.3210(3) 0.2191(7) 0.9824(4) 0.100(3) Uani 1 1 d . . . H14A H 0.3179 0.2277 1.0262 0.120 Uiso 1 1 calc R . . C15 C 0.3195(3) 0.1604(5) 0.9612(6) 0.072(2) Uani 1 1 d . . . C16 C 0.3317(6) 0.3256(7) 0.9584(5) 0.189(5) Uani 1 1 d . . . N1 N -0.0088(3) 0.0770(4) 0.9458(4) 0.154(4) Uani 1 1 d . . . N2 N 0.3311(7) 0.3760(4) 0.9767(5) 0.319(9) Uani 1 1 d . . . H3 H 0.221(3) 0.132(3) 0.840(3) 0.08(2) Uiso 1 1 d . . . H5 H 0.228(3) -0.028(3) 0.947(2) 0.090(19) Uiso 1 1 d . . . H6 H 0.1217(17) -0.0078(18) 0.9704(18) 0.010(16) Uiso 1 1 d . . . H15 H 0.314(2) 0.127(3) 0.991(3) 0.07(2) Uiso 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 C1 0.078(8) 0.074(6) 0.057(5) -0.008(5) -0.006(6) -0.003(8) C2 0.093(9) 0.072(7) 0.066(6) -0.011(6) -0.026(5) 0.038(6) C3 0.093(9) 0.047(6) 0.069(5) 0.004(4) -0.013(6) 0.004(6) C4 0.032(6) 0.066(6) 0.074(5) -0.001(5) -0.001(5) -0.021(7) C5 0.033(7) 0.055(7) 0.068(5) -0.009(5) 0.009(4) -0.004(5) C6 0.093(10) 0.044(7) 0.045(5) 0.002(5) 0.002(6) -0.022(6) C7 0.064(7) 0.149(7) 0.091(6) -0.051(5) -0.005(5) 0.016(6) C8 0.123(8) 0.123(8) 0.062(7) 0.052(7) -0.052(7) -0.084(14) C9 0.118(6) 0.118(6) 0.065(8) 0.027(6) -0.027(6) -0.009(11) C10 0.089(5) 0.064(9) 0.064(8) 0.001(8) -0.016(4) 0.006(4) C11 0.122(6) 0.092(7) 0.065(6) 0.026(9) -0.012(4) -0.006(5) C12 0.118(6) 0.064(9) 0.110(11) 0.027(7) -0.041(5) -0.025(5) C13 0.168(8) 0.036(9) 0.106(9) -0.004(9) -0.064(6) -0.020(4) C14 0.156(7) 0.057(7) 0.086(7) 0.013(9) -0.037(5) 0.005(4) C15 0.096(5) 0.048(9) 0.073(9) 0.013(7) -0.016(4) -0.003(4) C16 0.343(16) 0.075(9) 0.150(10) 0.016(8) -0.135(9) -0.008(8) N1 0.058(5) 0.257(9) 0.146(6) -0.082(6) -0.021(5) 0.039(5) N2 0.66(2) 0.079(7) 0.217(11) 0.003(7) -0.256(13) -0.018(10) _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 C2 1.348(9) . ? C1 C6 1.393(9) . ? C1 C7 1.460(11) . ? C2 C3 1.368(9) . ? C2 H2 0.9500 . ? C3 C4 1.400(9) . ? C3 H3 1.06(6) . ? C4 C5 1.357(8) . ? C4 C8 1.564(8) . ? C5 C6 1.392(8) . ? C5 H5 1.18(6) . ? C6 H6 0.90(4) . ? C7 N1 1.122(9) . ? C8 C9 1.231(13) . ? C8 C4 1.564(8) 7_546 ? C9 C10 1.563(10) 7_546 ? C9 C10 1.563(10) . ? C10 C15 1.341(8) . ? C10 C11 1.391(9) . ? C11 C12 1.347(9) . ? C11 H11 0.9500 . ? C12 C13 1.346(10) . ? C12 H12A 0.9500 . ? C13 C14 1.375(10) . ? C13 C16 1.394(13) . ? C14 C15 1.372(9) . ? C14 H14A 0.9500 . ? C15 H15 0.98(6) . ? C16 N2 1.178(13) . ? 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 C2 C1 C6 119.9(7) . . ? C2 C1 C7 120.2(12) . . ? C6 C1 C7 119.9(11) . . ? C1 C2 C3 121.0(6) . . ? C1 C2 H2 119.5 . . ? C3 C2 H2 119.5 . . ? C2 C3 C4 119.3(7) . . ? C2 C3 H3 132(3) . . ? C4 C3 H3 109(3) . . ? C5 C4 C3 120.8(7) . . ? C5 C4 C8 114.7(9) . . ? C3 C4 C8 124.1(9) . . ? C4 C5 C6 118.9(6) . . ? C4 C5 H5 121(3) . . ? C6 C5 H5 120(3) . . ? C5 C6 C1 120.2(7) . . ? C5 C6 H6 119(2) . . ? C1 C6 H6 121(3) . . ? N1 C7 C1 177.3(8) . . ? C9 C8 C4 122.2(5) . 7_546 ? C9 C8 C4 122.2(5) . . ? C4 C8 C4 115.7(10) 7_546 . ? C8 C9 C10 124.9(7) . 7_546 ? C8 C9 C10 124.9(7) . . ? C10 C9 C10 110.1(14) 7_546 . ? C15 C10 C11 121.1(8) . . ? C15 C10 C9 119.8(9) . . ? C11 C10 C9 118.4(11) . . ? C12 C11 C10 119.4(7) . . ? C12 C11 H11 120.3 . . ? C10 C11 H11 120.3 . . ? C13 C12 C11 119.7(8) . . ? C13 C12 H12A 120.1 . . ? C11 C12 H12A 120.1 . . ? C12 C13 C14 121.4(8) . . ? C12 C13 C16 117.0(13) . . ? C14 C13 C16 121.5(13) . . ? C15 C14 C13 119.1(8) . . ? C15 C14 H14A 120.4 . . ? C13 C14 H14A 120.4 . . ? C10 C15 C14 119.3(8) . . ? C10 C15 H15 120(3) . . ? C14 C15 H15 121(3) . . ? N2 C16 C13 174.7(16) . . ? _diffrn_measured_fraction_theta_max 0.980 _diffrn_reflns_theta_full 39.53 _diffrn_measured_fraction_theta_full 0.980 _refine_diff_density_max 0.134 _refine_diff_density_min -0.121 _refine_diff_density_rms 0.033