# Supplementary Material (ESI) for Journal of Materials Chemistry # This journal is (C) The Royal Society of Chemistry 2010 data_global _journal_name_full J.Mater.Chem. _journal_coden_Cambridge 1145 _publ_contact_author_name 'Simona Fantacci' _publ_contact_author_address ; Via Elce di Sotto, 8 Perugia 06123 ; _publ_contact_author_email simona@thch.unipg.it _publ_contact_author 'Dr. N. Casati' _publ_requested_category FO loop_ _publ_author_name S.Fantacci F.Nunzi E.Cariati E.Tordin N.Casati P.Macchi # Attachment 'Casati.cif' #\#CIF_1.1 # CIF produced by WinGX routine CIF_UPDATE # Created on 2009-05-25 at 12:58:59 # Using CIFtbx version 2.6.2 16 Jun 1998 # Dictionary name : cif_core.dic # Dictionary vers : 2.3 # Request file : c:\wingx\files\archive.dat # CIF files read : ele65c data_ele65c _database_code_depnum_ccdc_archive 'CCDC 733632' #TrackingRef 'Casati.cif' _audit_creation_date 2009-05-25T12:58:59-00:00 _audit_creation_method 'WinGX routine CIF_UPDATE' _audit_conform_dict_name cif_core.dic _audit_conform_dict_version 2.3 _audit_conform_dict_location ftp://ftp.iucr.org/pub/cif_core.dic #----------------------------------------------------------------------------# # CHEMICAL INFORMATION # #----------------------------------------------------------------------------# _chemical_name_systematic ; ? ; _chemical_formula_sum 'C16 H19 I N2' _chemical_formula_weight 366.23 _chemical_absolute_configuration ad #----------------------------------------------------------------------------# # UNIT CELL INFORMATION # #----------------------------------------------------------------------------# loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x, -y, z+1/2' 'x+1/2, y+1/2, z' 'x+1/2, -y+1/2, z+1/2' _cell_length_a 8.777(2) _cell_length_b 34.912(7) _cell_length_c 6.2800(10) _cell_angle_alpha 90 _cell_angle_beta 90.459(2) _cell_angle_gamma 90 _cell_volume 1924.3(7) _cell_formula_units_Z 4 _cell_measurement_temperature 298(2) #----------------------------------------------------------------------------# # CRYSTAL INFORMATION # #----------------------------------------------------------------------------# _exptl_crystal_size_max 0.25 _exptl_crystal_size_mid 0.08 _exptl_crystal_size_min 0.05 _exptl_crystal_density_diffrn 1.264 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 728 #----------------------------------------------------------------------------# # ABSORPTION CORRECTION # #----------------------------------------------------------------------------# _exptl_absorpt_coefficient_mu 1.657 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.789 _exptl_absorpt_correction_T_max 0.92 #----------------------------------------------------------------------------# # DATA COLLECTION # #----------------------------------------------------------------------------# _diffrn_ambient_temperature 298(2) _diffrn_radiation_wavelength 0.71069 _diffrn_radiation_type MoK\a _diffrn_radiation_monochromator graphite _diffrn_reflns_av_R_equivalents 0.0226 _diffrn_reflns_av_unetI/netI 0.037 _diffrn_reflns_number 7486 _diffrn_reflns_limit_h_min -10 _diffrn_reflns_limit_h_max 10 _diffrn_reflns_limit_k_min -43 _diffrn_reflns_limit_k_max 43 _diffrn_reflns_limit_l_min -7 _diffrn_reflns_limit_l_max 7 _diffrn_reflns_theta_min 1.17 _diffrn_reflns_theta_max 26.39 _diffrn_reflns_theta_full 26.39 _diffrn_measured_fraction_theta_full 0.988 _diffrn_measured_fraction_theta_max 0.988 _reflns_number_total 3727 _reflns_number_gt 2825 _reflns_threshold_expression >2sigma(I) #----------------------------------------------------------------------------# # COMPUTER PROGRAMS USED # #----------------------------------------------------------------------------# _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' #----------------------------------------------------------------------------# # REFINEMENT INFORMATION # #----------------------------------------------------------------------------# _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^)+(0.0996P)^2^+0.8198P] 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_number_reflns 3727 _refine_ls_number_parameters 59 _refine_ls_number_restraints 2 _refine_ls_R_factor_all 0.0696 _refine_ls_R_factor_gt 0.0564 _refine_ls_wR_factor_ref 0.1859 _refine_ls_wR_factor_gt 0.1766 _refine_ls_goodness_of_fit_ref 1.079 _refine_ls_restrained_S_all 1.079 _refine_ls_shift/su_max 0 _refine_ls_shift/su_mean 0 _refine_ls_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.01(6) _refine_diff_density_max 0.87 _refine_diff_density_min -0.57 _refine_diff_density_rms 0.096 #----------------------------------------------------------------------------# # ATOMIC TYPES, COORDINATES AND THERMAL PARAMETERS # #----------------------------------------------------------------------------# 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 0 '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' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 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 0.5635(7) 0.28395(15) 0.0379(7) 0.0614(16) Uiso 1 1 d G . . C2 C 0.4187(6) 0.2919(2) 0.1141(11) 0.072(3) Uiso 1 1 d G . . H2 H 0.3332 0.2833 0.04 0.086 Uiso 1 1 calc R . . C3 C 0.4017(7) 0.3128(2) 0.3008(12) 0.070(3) Uiso 1 1 d G . . H3 H 0.3048 0.3181 0.3517 0.084 Uiso 1 1 calc R . . C4 C 0.5295(9) 0.32571(17) 0.4114(9) 0.070(2) Uiso 1 1 d G . . C5 C 0.6744(8) 0.3177(2) 0.3353(11) 0.084(4) Uiso 1 1 d G . . H5 H 0.7599 0.3264 0.4093 0.1 Uiso 1 1 calc R . . C6 C 0.6914(6) 0.2969(2) 0.1486(11) 0.082(3) Uiso 1 1 d G . . H6 H 0.7883 0.2915 0.0976 0.098 Uiso 1 1 calc R . . C11 C 0.5289(10) 0.38679(19) 0.9133(8) 0.081(3) Uiso 1 1 d G . . C12 C 0.6615(7) 0.3989(2) 1.0154(11) 0.083(3) Uiso 1 1 d G . . H12 H 0.756 0.3923 0.9606 0.1 Uiso 1 1 calc R . . C13 C 0.6527(5) 0.4209(2) 1.1995(11) 0.087(3) Uiso 1 1 d G . . H13 H 0.7414 0.429 1.2679 0.104 Uiso 1 1 calc R . . C14 C 0.5114(6) 0.43072(15) 1.2815(8) 0.0463(17) Uiso 1 1 d G . . C15 C 0.3788(5) 0.4186(2) 1.1794(12) 0.097(4) Uiso 1 1 d G . . H15 H 0.2843 0.4252 1.2343 0.117 Uiso 1 1 calc R . . C16 C 0.3876(8) 0.3966(3) 0.9953(12) 0.105(4) Uiso 1 1 d G . . H16 H 0.2989 0.3885 0.927 0.126 Uiso 1 1 calc R . . C20 C 0.6428(18) 0.4654(5) 1.569(3) 0.111(5) Uiso 1 1 d . . . H20A H 0.6192 0.4806 1.6913 0.166 Uiso 1 1 calc R . . H20B H 0.703 0.4802 1.4718 0.166 Uiso 1 1 calc R . . H20C H 0.6991 0.4431 1.6123 0.166 Uiso 1 1 calc R . . C21 C 0.332(2) 0.4590(5) 1.552(3) 0.126(5) Uiso 1 1 d . . . H21A H 0.3374 0.4749 1.6767 0.189 Uiso 1 1 calc R . . H21B H 0.2889 0.4346 1.5891 0.189 Uiso 1 1 calc R . . H21C H 0.268 0.4712 1.4469 0.189 Uiso 1 1 calc R . . N2 N 0.4966(14) 0.4531(3) 1.459(2) 0.104(3) Uiso 1 1 d . . . I1 I 0.04577(16) 0.312437(16) 0.79947(16) 0.0825(3) Uani 1 1 d . . . C10 C 0.5812(15) 0.2624(3) -0.1487(18) 0.092(4) Uiso 1 1 d . . . H10A H 0.6877 0.2597 -0.179 0.138 Uiso 1 1 calc R . . H10B H 0.5314 0.2753 -0.2651 0.138 Uiso 1 1 calc R . . H10C H 0.5366 0.2376 -0.1298 0.138 Uiso 1 1 calc R . . C7' C 0.5810(15) 0.3638(3) 0.7323(18) 0.087(3) Uiso 1 1 d . . . H7' H 0.6852 0.3611 0.7118 0.104 Uiso 1 1 calc R . . C7 C 0.4912(14) 0.3477(3) 0.6031(19) 0.084(3) Uiso 1 1 d . . . H7 H 0.388 0.3499 0.6328 0.101 Uiso 1 1 calc R . . 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 I1 0.0674(3) 0.0965(4) 0.0835(4) -0.0183(4) -0.0043(4) 0.0007(5) #----------------------------------------------------------------------------# # MOLECULAR GEOMETRY # #----------------------------------------------------------------------------# _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 C2 1.39 . ? N1 C6 1.39 . ? N1 C10 1.401(12) . ? C2 C3 1.39 . ? C3 C4 1.39 . ? C4 C5 1.39 . ? C4 C7 1.469(13) . ? C5 C6 1.39 . ? C11 C12 1.39 . ? C11 C16 1.39 . ? C11 C7' 1.467(12) . ? C12 C13 1.39 . ? C13 C14 1.39 . ? C14 N2 1.369(14) . ? C14 C15 1.39 . ? C15 C16 1.39 . ? C20 N2 1.513(18) . ? C21 N2 1.58(2) . ? C7' C7 1.260(16) . ? 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 N1 C6 120 . . ? C2 N1 C10 120.2(7) . . ? C6 N1 C10 119.8(7) . . ? N1 C2 C3 120 . . ? C4 C3 C2 120 . . ? C5 C4 C3 120 . . ? C5 C4 C7 127.1(7) . . ? C3 C4 C7 112.9(7) . . ? C4 C5 C6 120 . . ? C5 C6 N1 120 . . ? C12 C11 C16 120 . . ? C12 C11 C7' 105.0(7) . . ? C16 C11 C7' 135.0(7) . . ? C13 C12 C11 120 . . ? C14 C13 C12 120 . . ? N2 C14 C13 122.3(6) . . ? N2 C14 C15 117.7(6) . . ? C13 C14 C15 120 . . ? C16 C15 C14 120 . . ? C15 C16 C11 120 . . ? C14 N2 C20 116.5(10) . . ? C14 N2 C21 117.9(12) . . ? C20 N2 C21 124.9(13) . . ? C7 C7' C11 123.1(11) . . ? C7' C7 C4 128.0(11) . . ?