# 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 _journal_year ? _journal_volume ? _journal_page_first ? _publ_contact_author_name 'Yih-Chern Horng' _publ_contact_author_email ychorng@cc.ncue.edu.tw loop_ _publ_author_name 'Pin-Shen Huang' 'Chih-Hong Kuo' 'Chang-Chih Hsieh' 'Yih-Chern Horng' data_1-I2 _database_code_depnum_ccdc_archive 'CCDC 848479' #TrackingRef 'web_deposit_cif_file_0_Yih-ChernHorng_1326272386.1-I2.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ? _chemical_name_common ? _chemical_formula_moiety 'C66 H72 N6 S6, I2' _chemical_formula_sum 'C66 H72 I2 N6 S6' _chemical_melting_point ? _exptl_crystal_description ? _exptl_crystal_colour ? _diffrn_ambient_temperature 200(2) _chemical_formula_weight 1395.46 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' S S 0.1246 0.1234 '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 trigonal _symmetry_space_group_name_H-M 'R -3 c' _symmetry_int_tables_number 167 _chemical_absolute_configuration ? loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x-y, z' '-x+y, -x, z' 'y, x, -z+1/2' 'x-y, -y, -z+1/2' '-x, -x+y, -z+1/2' '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' 'y+2/3, x+1/3, -z+5/6' 'x-y+2/3, -y+1/3, -z+5/6' '-x+2/3, -x+y+1/3, -z+5/6' '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' 'y+1/3, x+2/3, -z+7/6' 'x-y+1/3, -y+2/3, -z+7/6' '-x+1/3, -x+y+2/3, -z+7/6' '-x, -y, -z' 'y, -x+y, -z' 'x-y, x, -z' '-y, -x, z-1/2' '-x+y, y, z-1/2' 'x, x-y, z-1/2' '-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' '-y+2/3, -x+1/3, z-1/6' '-x+y+2/3, y+1/3, z-1/6' 'x+2/3, x-y+1/3, z-1/6' '-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' '-y+1/3, -x+2/3, z+1/6' '-x+y+1/3, y+2/3, z+1/6' 'x+1/3, x-y+2/3, z+1/6' _cell_length_a 17.583(3) _cell_length_b 17.583(3) _cell_length_c 48.345(10) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 120.00 _cell_volume 12943(4) _cell_formula_units_Z 6 _cell_measurement_temperature 200(2) _cell_measurement_reflns_used 2293 _cell_measurement_theta_min 3.92 _cell_measurement_theta_max 18.26 _exptl_crystal_size_max 0.44 _exptl_crystal_size_mid 0.32 _exptl_crystal_size_min 0.21 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.074 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 4272 _exptl_absorpt_coefficient_mu 0.907 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.6909 _exptl_absorpt_correction_T_max 0.8323 _exptl_absorpt_process_details 'SADABS (Sheldrick, 2003)' _exptl_special_details ; The R(int) is relatively high due to the relatively poor quality of the crystal resulting in the weak intensities of some high-angle reflections. An appropiate structural model could only be obtained the current space group. ; _diffrn_radiation_probe x-ray _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker SMART APEXII' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 2548 _diffrn_reflns_av_R_equivalents 0.1459 _diffrn_reflns_av_sigmaI/netI 0.0724 _diffrn_reflns_limit_h_min -18 _diffrn_reflns_limit_h_max 0 _diffrn_reflns_limit_k_min 0 _diffrn_reflns_limit_k_max 20 _diffrn_reflns_limit_l_min 0 _diffrn_reflns_limit_l_max 57 _diffrn_reflns_theta_min 1.58 _diffrn_reflns_theta_max 25.08 _reflns_number_total 2548 _reflns_number_gt 1182 _reflns_threshold_expression I>2\s _computing_data_collection 'APEX2 (Bruker, 2007)' _computing_cell_refinement 'SAINT (Bruker, 2007)' _computing_data_reduction 'SAINT (Bruker, 2007)' _computing_structure_solution 'SHELXTL (Sheldrick, 2008)' _computing_structure_refinement 'SHELXTL (Sheldrick, 2008)' _computing_molecular_graphics 'SHELXTL (Sheldrick, 2008)' _computing_publication_material 'DIAMOND (Brandenburg, 2006)' _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. Two of the carbon atoms in the pheny ring are disorded. SADI and EADP restraints were applied to C2, C2', C3 and C3'. ; _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^)+(0.1990P)^2^+0.0000P] 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 2548 _refine_ls_number_parameters 126 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.1417 _refine_ls_R_factor_gt 0.0924 _refine_ls_wR_factor_ref 0.3261 _refine_ls_wR_factor_gt 0.2989 _refine_ls_goodness_of_fit_ref 1.015 _refine_ls_restrained_S_all 1.015 _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 0.6758(5) 0.9299(6) 0.2157(2) 0.102(3) Uani 1 1 d . . . C2 C 0.5999(11) 0.9287(17) 0.2212(5) 0.125(8) Uani 0.60 1 d PD A 1 H2 H 0.5822 0.9255 0.2399 0.150 Uiso 0.60 1 calc PR A 1 C3 C 0.5424(11) 0.9322(9) 0.1989(5) 0.099(3) Uani 0.60 1 d PD A 1 H3 H 0.4936 0.9400 0.2025 0.119 Uiso 0.60 1 calc PR A 1 C2' C 0.5740(19) 0.885(3) 0.2240(7) 0.125(8) Uani 0.40 1 d PD A 2 H2' H 0.5499 0.8629 0.2418 0.150 Uiso 0.40 1 calc PR A 2 C3' C 0.5237(19) 0.8838(15) 0.1989(7) 0.099(3) Uani 0.40 1 d PD A 2 H3' H 0.4615 0.8563 0.1998 0.119 Uiso 0.40 1 calc PR A 2 C4 C 0.5670(7) 0.9231(7) 0.1736(2) 0.106(3) Uani 1 1 d . . . H4 H 0.5265 0.9082 0.1588 0.127 Uiso 1 1 calc R A 1 C5 C 0.6464(5) 0.9342(5) 0.16844(18) 0.087(2) Uani 1 1 d . A . H5 H 0.6644 0.9388 0.1497 0.104 Uiso 1 1 calc R . . C6 C 0.7050(5) 0.9394(5) 0.18917(18) 0.079(2) Uani 1 1 d . A . C7 C 0.8186(5) 0.9610(5) 0.15680(16) 0.084(2) Uani 1 1 d . A . H7A H 0.8137 1.0077 0.1469 0.101 Uiso 1 1 calc R . . H7B H 0.7827 0.9052 0.1467 0.101 Uiso 1 1 calc R . . C8 C 0.9131(5) 0.9830(5) 0.15680(14) 0.0730(19) Uani 1 1 d . . . C9 C 0.9328(5) 0.9112(5) 0.15583(16) 0.080(2) Uani 1 1 d . . . C10 C 0.8577(5) 0.8193(5) 0.15820(18) 0.091(2) Uani 1 1 d . . . H10A H 0.8762 0.7845 0.1695 0.110 Uiso 1 1 calc R . . H10B H 0.8087 0.8202 0.1680 0.110 Uiso 1 1 calc R . . C11 C 0.8270(8) 0.7772(9) 0.1322(3) 0.164(5) Uani 1 1 d . . . H11A H 0.7760 0.7186 0.1350 0.246 Uiso 1 1 calc R . . H11B H 0.8738 0.7717 0.1230 0.246 Uiso 1 1 calc R . . H11C H 0.8102 0.8121 0.1206 0.246 Uiso 1 1 calc R . . N1 N 0.7852(4) 0.9526(4) 0.18383(13) 0.0835(18) Uani 1 1 d . . . H1 H 0.8188 0.9562 0.1978 0.100 Uiso 1 1 calc R A . S2 S 0.74430(18) 0.9360(2) 0.24422(5) 0.1215(10) Uani 1 1 d . . . I1 I 0.0000 0.0000 0.22287(2) 0.1141(7) Uani 1 3 d S . . 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 0.083(6) 0.129(7) 0.118(8) 0.007(6) -0.022(5) 0.071(5) C2 0.079(12) 0.18(3) 0.115(9) 0.094(13) 0.062(9) 0.063(14) C3 0.066(8) 0.075 0.152(10) -0.005(13) -0.016(8) 0.032(9) C2' 0.079(12) 0.18(3) 0.115(9) 0.094(13) 0.062(9) 0.063(14) C3' 0.066(8) 0.075 0.152(10) -0.005(13) -0.016(8) 0.032(9) C4 0.104(7) 0.132(8) 0.091(7) -0.002(5) 0.003(5) 0.066(6) C5 0.069(5) 0.097(6) 0.101(6) 0.001(5) -0.011(4) 0.048(4) C6 0.072(5) 0.071(4) 0.090(6) 0.000(4) 0.008(4) 0.032(4) C7 0.083(5) 0.094(5) 0.082(6) -0.020(4) -0.023(4) 0.048(4) C8 0.080(5) 0.079(5) 0.057(4) 0.000(3) 0.006(3) 0.037(4) C9 0.080(5) 0.072(5) 0.088(5) -0.001(4) 0.014(4) 0.039(4) C10 0.089(6) 0.080(5) 0.100(6) -0.015(5) 0.007(5) 0.039(5) C11 0.138(10) 0.139(9) 0.144(11) -0.009(8) 0.017(8) 0.016(8) N1 0.072(4) 0.109(5) 0.076(4) -0.004(3) -0.013(3) 0.050(4) S2 0.125(2) 0.186(3) 0.0992(18) 0.0260(17) 0.0140(15) 0.1123(19) I1 0.1297(9) 0.1297(9) 0.0829(9) 0.000 0.000 0.0649(4) _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 1.35(2) . ? C1 C6 1.360(12) . ? C1 C2' 1.60(3) . ? C1 S2 1.798(8) . ? C2 C3 1.498(16) . ? C2 H2 0.9500 . ? C3 C4 1.33(2) . ? C3 H3 0.9500 . ? C2' C3' 1.499(16) . ? C2' H2' 0.9500 . ? C3' C4 1.42(3) . ? C3' H3' 0.9500 . ? C4 C5 1.334(11) . ? C4 H4 0.9500 . ? C5 C6 1.407(11) . ? C5 H5 0.9500 . ? C6 N1 1.334(9) . ? C7 N1 1.410(10) . ? C7 C8 1.507(10) . ? C7 H7A 0.9900 . ? C7 H7B 0.9900 . ? C8 C9 1.345(10) 3_675 ? C8 C9 1.467(10) . ? C9 C8 1.346(10) 2_765 ? C9 C10 1.495(10) . ? C10 C11 1.421(14) . ? C10 H10A 0.9900 . ? C10 H10B 0.9900 . ? C11 H11A 0.9800 . ? C11 H11B 0.9800 . ? C11 H11C 0.9800 . ? N1 H1 0.8800 . ? S2 S2 2.027(7) 5_675 ? I1 I1 2.623(2) 4 ? 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 119.7(11) . . ? C6 C1 C2' 123.8(14) . . ? C2 C1 S2 118.5(12) . . ? C6 C1 S2 121.0(6) . . ? C2' C1 S2 112.7(12) . . ? C1 C2 C3 122.7(18) . . ? C1 C2 H2 118.6 . . ? C3 C2 H2 118.6 . . ? C4 C3 C2 112.8(17) . . ? C4 C3 H3 123.6 . . ? C2 C3 H3 123.6 . . ? C3' C2' C1 108(2) . . ? C3' C2' H2' 126.0 . . ? C1 C2' H2' 126.0 . . ? C4 C3' C2' 121(2) . . ? C4 C3' H3' 119.3 . . ? C2' C3' H3' 119.3 . . ? C3 C4 C5 122.2(11) . . ? C5 C4 C3' 119.9(13) . . ? C3 C4 H4 118.9 . . ? C5 C4 H4 118.9 . . ? C3' C4 H4 111.7 . . ? C4 C5 C6 123.7(8) . . ? C4 C5 H5 118.1 . . ? C6 C5 H5 118.1 . . ? N1 C6 C1 120.3(8) . . ? N1 C6 C5 123.3(8) . . ? C1 C6 C5 116.4(7) . . ? N1 C7 C8 112.0(6) . . ? N1 C7 H7A 109.2 . . ? C8 C7 H7A 109.2 . . ? N1 C7 H7B 109.2 . . ? C8 C7 H7B 109.2 . . ? H7A C7 H7B 107.9 . . ? C9 C8 C9 120.4(8) 3_675 . ? C9 C8 C7 120.5(7) 3_675 . ? C9 C8 C7 118.9(7) . . ? C8 C9 C8 119.3(8) 2_765 . ? C8 C9 C10 122.2(7) 2_765 . ? C8 C9 C10 117.8(7) . . ? C11 C10 C9 113.3(8) . . ? C11 C10 H10A 108.9 . . ? C9 C10 H10A 108.9 . . ? C11 C10 H10B 108.9 . . ? C9 C10 H10B 108.9 . . ? H10A C10 H10B 107.7 . . ? C10 C11 H11A 109.5 . . ? C10 C11 H11B 109.5 . . ? H11A C11 H11B 109.5 . . ? C10 C11 H11C 109.5 . . ? H11A C11 H11C 109.5 . . ? H11B C11 H11C 109.5 . . ? C6 N1 C7 123.1(6) . . ? C6 N1 H1 118.5 . . ? C7 N1 H1 118.5 . . ? C1 S2 S2 105.2(3) . 5_675 ? _diffrn_measured_fraction_theta_max 0.994 _diffrn_reflns_theta_full 25.08 _diffrn_measured_fraction_theta_full 0.994 _refine_diff_density_max 0.631 _refine_diff_density_min -1.092 _refine_diff_density_rms 0.130 _diffrn_standards_number 0 _diffrn_standards_interval_count 0 _diffrn_standards_interval_time 0 _diffrn_standards_decay_% 0