# Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics # This journal is © The Owner Societies 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_1 _database_code_depnum_ccdc_archive 'CCDC 908910' #TrackingRef 'TIE.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C2 I4' _chemical_formula_weight 531.62 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' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Monoclinic _symmetry_space_group_name_H-M P2(1)/c loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, y+1/2, -z+1/2' '-x, -y, -z' 'x, -y-1/2, z-1/2' _cell_length_a 14.979(3) _cell_length_b 4.3028(8) _cell_length_c 12.748(2) _cell_angle_alpha 90.00 _cell_angle_beta 108.508(3) _cell_angle_gamma 90.00 _cell_volume 779.1(3) _cell_formula_units_Z 4 _cell_measurement_temperature 110(2) _cell_measurement_reflns_used 2517 _cell_measurement_theta_min 2.87 _cell_measurement_theta_max 27.49 _exptl_crystal_description ? _exptl_crystal_colour ? _exptl_crystal_size_max 0.28 _exptl_crystal_size_mid 0.20 _exptl_crystal_size_min 0.13 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 4.532 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 896 _exptl_absorpt_coefficient_mu 15.886 _exptl_absorpt_correction_type Multi-scan _exptl_absorpt_correction_T_min 0.0950 _exptl_absorpt_correction_T_max 0.2319 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 110(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'CCD area detector' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 3335 _diffrn_reflns_av_R_equivalents 0.0315 _diffrn_reflns_av_sigmaI/netI 0.0398 _diffrn_reflns_limit_h_min -14 _diffrn_reflns_limit_h_max 17 _diffrn_reflns_limit_k_min -5 _diffrn_reflns_limit_k_max 4 _diffrn_reflns_limit_l_min -15 _diffrn_reflns_limit_l_max 13 _diffrn_reflns_theta_min 2.87 _diffrn_reflns_theta_max 25.25 _reflns_number_total 1393 _reflns_number_gt 1344 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker SMART' _computing_cell_refinement 'Bruker SMART' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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^)+(0.0151P)^2^+20.3839P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 1393 _refine_ls_number_parameters 58 _refine_ls_number_restraints 18 _refine_ls_R_factor_all 0.0413 _refine_ls_R_factor_gt 0.0397 _refine_ls_wR_factor_ref 0.0893 _refine_ls_wR_factor_gt 0.0886 _refine_ls_goodness_of_fit_ref 1.251 _refine_ls_restrained_S_all 1.243 _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 C1A C 0.4548(15) 0.525(5) 0.4960(18) 0.010(3) Uani 0.50 1 d PU . . C1B C 0.4873(16) 0.447(5) 0.4564(18) 0.010(3) Uani 0.50 1 d PU . . C2 C 0.0451(8) 0.980(3) 0.5293(9) 0.012(2) Uani 1 1 d U . . I1 I 0.34409(5) 0.40431(19) 0.35217(6) 0.0182(2) Uani 1 1 d . . . I2 I 0.41212(5) 0.73326(18) 0.62035(6) 0.0161(2) Uani 1 1 d . . . I3 I 0.09242(5) 0.76950(17) 0.68480(6) 0.0150(2) Uani 1 1 d . . . I4 I 0.15478(5) 1.13422(18) 0.47011(6) 0.0154(2) 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 C1A 0.007(4) 0.011(4) 0.011(4) 0.000(3) 0.003(3) 0.002(3) C1B 0.007(4) 0.011(4) 0.011(4) 0.000(3) 0.003(3) 0.002(3) C2 0.015(4) 0.012(4) 0.012(4) -0.001(3) 0.006(3) -0.004(3) I1 0.0081(4) 0.0327(5) 0.0134(4) -0.0020(3) 0.0027(3) -0.0040(3) I2 0.0152(4) 0.0216(4) 0.0146(4) 0.0000(3) 0.0091(3) 0.0060(3) I3 0.0143(4) 0.0208(4) 0.0108(4) 0.0017(3) 0.0053(3) 0.0019(3) I4 0.0109(4) 0.0216(4) 0.0170(4) -0.0011(3) 0.0092(3) -0.0026(3) _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 C1A C1B 0.87(3) . ? C1A C1B 0.90(3) 3_666 ? C1A C1A 1.34(4) 3_666 ? C1A I2 2.09(2) . ? C1A I1 2.11(2) . ? C1B C1A 0.90(3) 3_666 ? C1B C1B 1.15(4) 3_666 ? C1B I1 2.14(2) . ? C1B I2 2.18(2) 3_666 ? C2 C2 1.33(2) 3_576 ? C2 I3 2.088(11) . ? C2 I4 2.121(11) . ? I2 C1B 2.18(2) 3_666 ? 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 C1B C1A C1B 81(3) . 3_666 ? C1B C1A C1A 41(2) . 3_666 ? C1B C1A C1A 40.0(19) 3_666 3_666 ? C1B C1A I2 165(3) . . ? C1B C1A I2 84(2) 3_666 . ? C1A C1A I2 124(2) 3_666 . ? C1B C1A I1 80(2) . . ? C1B C1A I1 162(3) 3_666 . ? C1A C1A I1 122(2) 3_666 . ? I2 C1A I1 114.8(10) . . ? C1A C1B C1A 99(3) . 3_666 ? C1A C1B C1B 50(2) . 3_666 ? C1A C1B C1B 49(2) 3_666 3_666 ? C1A C1B I1 76(2) . . ? C1A C1B I1 175(3) 3_666 . ? C1B C1B I1 126(3) 3_666 . ? C1A C1B I2 171(3) . 3_666 ? C1A C1B I2 72(2) 3_666 3_666 ? C1B C1B I2 121(3) 3_666 3_666 ? I1 C1B I2 113.0(10) . 3_666 ? C2 C2 I3 124.6(11) 3_576 . ? C2 C2 I4 121.5(11) 3_576 . ? I3 C2 I4 113.9(5) . . ? C1A I1 C1B 23.7(7) . . ? C1A I2 C1B 24.1(7) . 3_666 ? _diffrn_measured_fraction_theta_max 0.989 _diffrn_reflns_theta_full 25.25 _diffrn_measured_fraction_theta_full 0.989 _refine_diff_density_max 2.205 _refine_diff_density_min -2.121 _refine_diff_density_rms 0.324