# Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics # This journal is © The Owner Societies 2011 data_global _journal_name_full Phys.Chem.Chem.Phys.(PCCP) _journal_coden_cambridge 1326 _journal_year ? _journal_volume ? _journal_page_first ? _publ_contact_author_email morton@citrus.ucr.edu _publ_contact_author_name 'Thomas Morton' loop_ _publ_author_name 'Thomas Morton' 'Gregory J.O.Beran' 'Eric Chronister' 'Luke Daemen' 'Aaron Moehlig' 'Leonard Mueller' 'Jos Oomens' 'Andrew Rice' 'David Santiago-Dieppa' 'Fook Tham' 'Kelly Theel' 'Sepideh Yaghmaei' data_tm13-no-hsym _database_code_depnum_ccdc_archive 'CCDC 831398' #TrackingRef '- tm13-no-Hsym.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C8 H21 I N2' _chemical_formula_weight 272.17 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' I I -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Orthorhombic _symmetry_space_group_name_H-M Cmcm loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z+1/2' '-x, y, -z+1/2' 'x, -y, -z' 'x+1/2, y+1/2, z' '-x+1/2, -y+1/2, z+1/2' '-x+1/2, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z' '-x, -y, -z' 'x, y, -z-1/2' 'x, -y, z-1/2' '-x, y, z' '-x+1/2, -y+1/2, -z' 'x+1/2, y+1/2, -z-1/2' 'x+1/2, -y+1/2, z-1/2' '-x+1/2, y+1/2, z' _cell_length_a 8.8848(6) _cell_length_b 10.8203(7) _cell_length_c 11.8758(7) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1141.69(13) _cell_formula_units_Z 4 _cell_measurement_temperature 90(2) _cell_measurement_reflns_used 3730 _cell_measurement_theta_min 2.97 _cell_measurement_theta_max 30.37 _exptl_crystal_description 'thin plate frag' _exptl_crystal_colour colourless _exptl_crystal_size_max 0.16 _exptl_crystal_size_mid 0.16 _exptl_crystal_size_min 0.01 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 1.583 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 544 _exptl_absorpt_coefficient_mu 2.759 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.6713 _exptl_absorpt_correction_T_max 0.9729 _exptl_absorpt_process_details 'Bruker SADABS' _exptl_special_details ; ? ; _diffrn_ambient_temperature 90(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'Normal-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker APEX-II CCD' _diffrn_measurement_method '\f and \w scans' _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 6340 _diffrn_reflns_av_R_equivalents 0.0339 _diffrn_reflns_av_sigmaI/netI 0.0215 _diffrn_reflns_limit_h_min -12 _diffrn_reflns_limit_h_max 12 _diffrn_reflns_limit_k_min -15 _diffrn_reflns_limit_k_max 15 _diffrn_reflns_limit_l_min -16 _diffrn_reflns_limit_l_max 14 _diffrn_reflns_theta_min 2.97 _diffrn_reflns_theta_max 30.02 _reflns_number_total 923 _reflns_number_gt 863 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _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^)+(0.0211P)^2^+1.3735P] 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 none _refine_ls_extinction_coef ? _refine_ls_number_reflns 923 _refine_ls_number_parameters 55 _refine_ls_number_restraints 35 _refine_ls_R_factor_all 0.0230 _refine_ls_R_factor_gt 0.0200 _refine_ls_wR_factor_ref 0.0446 _refine_ls_wR_factor_gt 0.0437 _refine_ls_goodness_of_fit_ref 1.091 _refine_ls_restrained_S_all 1.071 _refine_ls_shift/su_max 0.001 _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 I1 I 0.5000 0.69496(2) 0.7500 0.01833(8) Uani 1 4 d S . . C1 C 0.6429(7) 0.6195(5) 0.3999(6) 0.0204(11) Uani 0.50 1 d PDU A -1 H1A H 0.6207 0.5347 0.3760 0.031 Uiso 0.50 1 calc PR A -1 H1B H 0.6487 0.6228 0.4822 0.031 Uiso 0.50 1 calc PR A -1 H1C H 0.7393 0.6457 0.3677 0.031 Uiso 0.50 1 calc PR A -1 C2 C 0.3760(6) 0.6640(5) 0.4074(5) 0.0220(11) Uani 0.50 1 d PDU A -1 H2A H 0.3559 0.5780 0.3862 0.033 Uiso 0.50 1 calc PR A -1 H2B H 0.2961 0.7172 0.3776 0.033 Uiso 0.50 1 calc PR A -1 H2C H 0.3788 0.6709 0.4897 0.033 Uiso 0.50 1 calc PR A -1 N1 N 0.5222(5) 0.7029(2) 0.3603(2) 0.0143(10) Uani 0.50 1 d PDU A -1 H1 H 0.518(2) 0.704(5) 0.288(5) 0.017 Uiso 0.25 1 d PD B -1 C3 C 0.5566(4) 0.8345(3) 0.3865(3) 0.0201(7) Uani 0.50 1 d PDU A -1 H3A H 0.6663 0.8479 0.3787 0.024 Uiso 0.50 1 calc PR A -1 H3B H 0.5294 0.8510 0.4660 0.024 Uiso 0.50 1 calc PR A -1 C4 C 0.4745(5) 0.9263(3) 0.3117(3) 0.0215(12) Uani 0.50 1 d PU A -1 H4A H 0.5100 1.0065 0.3339 0.026 Uiso 0.50 1 d PR A -1 H4B H 0.3707 0.9224 0.3339 0.026 Uiso 0.50 1 d PR A -1 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 0.01436(10) 0.01625(11) 0.02438(13) 0.000 0.000 0.000 C1 0.0162(19) 0.019(3) 0.026(2) 0.000(2) -0.0040(16) 0.0026(19) C2 0.018(2) 0.026(3) 0.022(2) 0.002(2) -0.0022(16) -0.003(2) N1 0.010(3) 0.0147(10) 0.0184(12) -0.0002(9) 0.0013(10) -0.0010(10) C3 0.0204(13) 0.0183(15) 0.0217(17) -0.0049(13) -0.0002(13) -0.0003(12) C4 0.023(4) 0.0136(12) 0.0281(16) -0.0037(12) -0.0008(13) 0.0026(13) _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 N1 1.478(6) . ? C1 H1A 0.9800 . ? C1 H1B 0.9800 . ? C1 H1C 0.9800 . ? C2 N1 1.476(6) . ? C2 H2A 0.9800 . ? C2 H2B 0.9800 . ? C2 H2C 0.9800 . ? N1 C3 1.490(4) . ? N1 H1 0.86(6) . ? C3 C4 1.519(5) . ? C3 H3A 0.9900 . ? C3 H3B 0.9900 . ? C4 H4A 0.9600 . ? C4 H4B 0.9600 . ? 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 C1 110.1(3) . . ? C2 N1 C3 111.9(3) . . ? C1 N1 C3 111.6(3) . . ? C2 N1 H1 110(2) . . ? C1 N1 H1 111(2) . . ? C3 N1 H1 102(4) . . ? N1 C3 C4 113.9(3) . . ? N1 C3 H3A 108.8 . . ? C4 C3 H3A 108.8 . . ? N1 C3 H3B 108.8 . . ? C4 C3 H3B 108.8 . . ? H3A C3 H3B 107.7 . . ? C3 C4 H4A 105.9 . . ? C3 C4 H4B 105.8 . . ? H4A C4 H4B 106.2 . . ? 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 C2 N1 C3 C4 -78.8(4) . . . . ? C1 N1 C3 C4 157.3(4) . . . . ? loop_ _geom_hbond_atom_site_label_D _geom_hbond_atom_site_label_H _geom_hbond_atom_site_label_A _geom_hbond_distance_DH _geom_hbond_distance_HA _geom_hbond_distance_DA _geom_hbond_angle_DHA _geom_hbond_site_symmetry_A N1 H1 N1 0.86(6) 1.79(6) 2.648(6) 171(2) 3_655 _diffrn_measured_fraction_theta_max 0.998 _diffrn_reflns_theta_full 30.02 _diffrn_measured_fraction_theta_full 0.998 _refine_diff_density_max 0.546 _refine_diff_density_min -1.074 _refine_diff_density_rms 0.096