# Supplementary Material (ESI) for Dalton Transactions # This journal is © The Royal Society of Chemistry 2001 # CCDC Number: 186/2331 _publ_contact_author_name 'Robin G. Pritchard' _publ_contact_author_address 'Department of Chemistry, UMIST, Manchester' _publ_requested_journal 'Dalton' _publ_section_title ; Structural Isomerism in R3PSe(Ph)I compounds Your code B008525L ; data_smg30a _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C12 H23 I1 N3 P1 Se1' _chemical_formula_sum 'C12 H29 I N3 P Se' _chemical_formula_weight 403.83 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' 'I' 'I' -0.4742 1.8119 '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' 'P' 'P' 0.1023 0.0942 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Se' 'Se' -0.0929 2.2259 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M 'C m c a' 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' 'x+1/2, y+1/2, z' '-x+1/2, -y+1, z+1/2' 'x+1/2, -y+1/2, -z' '-x+1/2, y+1, -z+1/2' '-x, -y, -z' 'x, y-1/2, -z-1/2' '-x, y, z' 'x, -y-1/2, z-1/2' '-x+1/2, -y+1/2, -z' 'x+1/2, y, -z-1/2' '-x+1/2, y+1/2, z' 'x+1/2, -y, z-1/2' _cell_length_a 10.164 _cell_length_b 12.526 _cell_length_c 26.427 _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 3364.7 _cell_formula_units_Z 8 _cell_measurement_temperature 203(2) _cell_measurement_reflns_used 0 _cell_measurement_theta_min 0 _cell_measurement_theta_max 0 _exptl_crystal_description prism _exptl_crystal_colour 'pale yellow' _exptl_crystal_size_max 0.25 _exptl_crystal_size_mid 0.25 _exptl_crystal_size_min 0.20 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.785 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1744 _exptl_absorpt_coefficient_mu 4.153 _exptl_absorpt_correction_type ? _exptl_absorpt_correction_T_min 0.4233 _exptl_absorpt_correction_T_max 0.4906 _exptl_absorpt_process_details ? _exptl_special_details ; ? ; _diffrn_ambient_temperature 203(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 'Enraf Nonius CAD4' _diffrn_measurement_method 'non-profiled omega scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number 3 _diffrn_standards_interval_count ? _diffrn_standards_interval_time 60 _diffrn_standards_decay_% 0 _diffrn_reflns_number 2949 _diffrn_reflns_av_R_equivalents 0.0647 _diffrn_reflns_av_sigmaI/netI 0.0603 _diffrn_reflns_limit_h_min -12 _diffrn_reflns_limit_h_max 12 _diffrn_reflns_limit_k_min 0 _diffrn_reflns_limit_k_max 14 _diffrn_reflns_limit_l_min 0 _diffrn_reflns_limit_l_max 31 _diffrn_reflns_theta_min 1.54 _diffrn_reflns_theta_max 24.97 _reflns_number_total 1569 _reflns_number_gt 1269 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CAD4 Express (Enraf Nonius, 1994)' _computing_cell_refinement 'CAD4 Express (Enraf Nonius, 1994)' _computing_data_reduction 'XCAD4 (Harms & Wocadlo, 1995)' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1997)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'Ortep-3 for Windows (Farrugia, 1997)' _computing_publication_material 'WinGX publication routines (Farrugia, 1999)' _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. The cation lies on a crystallographic mirror plane , which bisects the P atom and two of the N(Me)2 groups. This has led to the remaining N(Me)2 and the SePh being disordered so that half of each occupies each side of the mirror plane ; _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^)+(0.0730P)^2^+6.7690P] 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 0.00058(16) _refine_ls_extinction_expression 'Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^' _refine_ls_number_reflns 1569 _refine_ls_number_parameters 136 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0628 _refine_ls_R_factor_gt 0.0478 _refine_ls_wR_factor_ref 0.1321 _refine_ls_wR_factor_gt 0.1217 _refine_ls_goodness_of_fit_ref 1.092 _refine_ls_restrained_S_all 1.092 _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 I1 I 0.0000 0.52336(6) 0.33267(2) 0.0494(3) Uani 1 2 d S . . Se1 Se 0.31262(15) 0.59166(12) 0.40641(6) 0.0310(4) Uani 0.50 1 d P . . P1 P 0.5000 0.57412(15) 0.36185(7) 0.0238(5) Uani 1 2 d S . . N1 N 0.5000 0.6691(5) 0.3206(3) 0.0301(15) Uani 1 2 d S . . N2 N 0.5000 0.4507(6) 0.3422(3) 0.0323(15) Uani 1 2 d S . . C1 C 0.3866(9) 0.6923(9) 0.4534(4) 0.026(2) Uani 0.50 1 d P . . C2 C 0.4135(11) 0.7958(9) 0.4381(4) 0.034(3) Uani 0.50 1 d P . . H2 H 0.4001 0.8171 0.4044 0.041 Uiso 0.50 1 calc PR . . C3 C 0.4616(12) 0.8682(9) 0.4744(5) 0.048(4) Uani 0.50 1 d P . . H3 H 0.4833 0.9382 0.4647 0.057 Uiso 0.50 1 calc PR . . C4 C 0.477(3) 0.8369(9) 0.5248(5) 0.039(7) Uani 0.50 1 d P . . H4 H 0.5071 0.8862 0.5491 0.047 Uiso 0.50 1 calc PR . . C5 C 0.4499(12) 0.7351(9) 0.5385(4) 0.040(3) Uani 0.50 1 d P . . H5 H 0.4625 0.7138 0.5722 0.048 Uiso 0.50 1 calc PR . . C6 C 0.4026(12) 0.6603(10) 0.5029(4) 0.037(3) Uani 0.50 1 d P . . H6 H 0.3825 0.5901 0.5128 0.044 Uiso 0.50 1 calc PR . . C7 C 0.3809(6) 0.6990(6) 0.2927(3) 0.0517(18) Uani 1 1 d . . . H7A H 0.3738 0.7762 0.2915 0.078 Uiso 1 1 calc R . . H7B H 0.3043 0.6697 0.3096 0.078 Uiso 1 1 calc R . . H7C H 0.3857 0.6710 0.2585 0.078 Uiso 1 1 calc R . . C8 C 0.6187(7) 0.4071(6) 0.3185(3) 0.065(2) Uani 1 1 d . . . H8A H 0.6170 0.3298 0.3206 0.098 Uiso 1 1 calc R . . H8B H 0.6958 0.4339 0.3360 0.098 Uiso 1 1 calc R . . H8C H 0.6220 0.4287 0.2833 0.098 Uiso 1 1 calc R . . N3 N 0.6281(12) 0.5858(9) 0.3933(5) 0.033(3) Uani 0.50 1 d P . . C9 C 0.6971(11) 0.6853(10) 0.4051(5) 0.042(3) Uani 0.50 1 d P . . H9A H 0.6572 0.7437 0.3865 0.064 Uiso 1 1 calc R . . H9B H 0.7889 0.6788 0.3956 0.064 Uiso 1 1 calc R . . H9C H 0.6910 0.6994 0.4412 0.064 Uiso 1 1 calc R . . C10 C 0.6785(13) 0.4996(11) 0.4257(5) 0.046(3) Uani 0.50 1 d P . . H10A H 0.6140 0.4426 0.4276 0.068 Uiso 1 1 calc R . . H10B H 0.6951 0.5272 0.4594 0.068 Uiso 1 1 calc R . . H10C H 0.7598 0.4720 0.4116 0.068 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 0.0568(5) 0.0528(5) 0.0385(4) 0.0004(3) 0.000 0.000 Se1 0.0213(7) 0.0333(8) 0.0383(8) -0.0077(6) 0.0039(6) -0.0059(7) P1 0.0193(9) 0.0253(10) 0.0268(10) -0.0037(8) 0.000 0.000 N1 0.022(3) 0.029(3) 0.039(4) 0.003(3) 0.000 0.000 N2 0.026(3) 0.028(3) 0.043(4) -0.009(3) 0.000 0.000 C1 0.016(5) 0.032(6) 0.032(5) -0.002(5) 0.002(4) 0.000(4) C2 0.040(6) 0.032(6) 0.030(6) 0.000(5) 0.003(5) 0.002(5) C3 0.059(12) 0.025(5) 0.060(7) -0.007(5) -0.004(6) -0.008(5) C4 0.03(2) 0.037(5) 0.046(6) -0.015(4) -0.015(7) -0.003(6) C5 0.053(7) 0.037(6) 0.030(6) -0.003(5) -0.004(5) 0.009(5) C6 0.042(6) 0.029(6) 0.038(6) 0.001(5) 0.002(5) 0.006(6) C7 0.032(3) 0.073(5) 0.050(4) 0.020(4) -0.002(3) 0.010(3) C8 0.056(5) 0.037(4) 0.102(6) -0.028(4) 0.029(5) -0.001(4) N3 0.018(6) 0.030(6) 0.052(7) 0.004(5) -0.004(5) 0.000(5) C9 0.017(5) 0.062(9) 0.048(7) -0.016(7) -0.007(5) -0.002(6) C10 0.041(7) 0.061(8) 0.034(6) 0.021(6) -0.009(6) 0.000(6) _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 Se1 N3 0.699(13) 11_655 ? Se1 C9 1.178(13) 11_655 ? Se1 C10 1.265(13) 11_655 ? Se1 C1 1.923(11) . ? Se1 P1 2.2500(19) . ? P1 N3 1.551(14) . ? P1 N3 1.551(14) 11_655 ? P1 N1 1.614(7) . ? P1 N2 1.631(7) . ? P1 Se1 2.2500(19) 11_655 ? N1 C7 1.466(7) 11_655 ? N1 C7 1.466(7) . ? N2 C8 1.465(8) 11_655 ? N2 C8 1.465(8) . ? C1 C6 1.377(15) . ? C1 C2 1.386(15) . ? C1 C9 1.536(15) 11_655 ? C2 C3 1.406(16) . ? C2 C2 1.76(2) 11_655 ? C2 C3 1.830(17) 11_655 ? C2 C9 1.985(16) 11_655 ? C3 C4 1.399(18) . ? C4 C5 1.354(18) . ? C5 C6 1.411(17) . ? N3 Se1 0.699(12) 11_655 ? N3 C9 1.465(16) . ? N3 C10 1.471(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 N3 Se1 C9 99.4(12) 11_655 11_655 ? N3 Se1 C10 92.4(12) 11_655 11_655 ? C9 Se1 C10 157.8(8) 11_655 11_655 ? N3 Se1 C1 93.0(11) 11_655 . ? C9 Se1 C1 53.0(7) 11_655 . ? C10 Se1 C1 108.0(7) 11_655 . ? N3 Se1 P1 1.9(10) 11_655 . ? C9 Se1 P1 98.8(6) 11_655 . ? C10 Se1 P1 93.6(6) 11_655 . ? C1 Se1 P1 94.1(3) . . ? N3 P1 N3 114.1(9) . 11_655 ? N3 P1 N1 107.0(5) . . ? N3 P1 N1 107.0(4) 11_655 . ? N3 P1 N2 105.1(4) . . ? N3 P1 N2 105.1(5) 11_655 . ? N1 P1 N2 118.9(4) . . ? N3 P1 Se1 0.9(5) . 11_655 ? N3 P1 Se1 114.9(4) 11_655 11_655 ? N1 P1 Se1 106.36(14) . 11_655 ? N2 P1 Se1 105.05(14) . 11_655 ? N3 P1 Se1 114.9(4) . . ? N3 P1 Se1 0.9(5) 11_655 . ? N1 P1 Se1 106.36(14) . . ? N2 P1 Se1 105.05(14) . . ? Se1 P1 Se1 115.66(11) 11_655 . ? C7 N1 C7 111.3(7) 11_655 . ? C7 N1 P1 121.9(4) 11_655 . ? C7 N1 P1 121.9(4) . . ? C8 N2 C8 111.0(7) 11_655 . ? C8 N2 P1 119.3(4) 11_655 . ? C8 N2 P1 119.3(4) . . ? C6 C1 C2 121.7(10) . . ? C6 C1 C9 146.9(11) . 11_655 ? C2 C1 C9 85.4(9) . 11_655 ? C6 C1 Se1 118.0(9) . . ? C2 C1 Se1 120.2(8) . . ? C9 C1 Se1 37.8(6) 11_655 . ? C1 C2 C3 118.2(10) . . ? C1 C2 C2 101.4(6) . 11_655 ? C3 C2 C2 69.7(7) . 11_655 ? C1 C2 C3 116.6(9) . 11_655 ? C3 C2 C3 23.6(8) . 11_655 ? C2 C2 C3 46.1(5) 11_655 11_655 ? C1 C2 C9 50.5(7) . 11_655 ? C3 C2 C9 161.0(10) . 11_655 ? C2 C2 C9 124.5(5) 11_655 11_655 ? C3 C2 C9 165.5(8) 11_655 11_655 ? C4 C3 C2 120.6(11) . . ? C5 C4 C3 119.6(12) . . ? C4 C5 C6 121.2(11) . . ? C1 C6 C5 118.7(11) . . ? Se1 N3 C9 52.5(10) 11_655 . ? Se1 N3 C10 59.2(11) 11_655 . ? C9 N3 C10 109.5(12) . . ? Se1 N3 P1 177.2(15) 11_655 . ? C9 N3 P1 126.6(9) . . ? C10 N3 P1 122.4(10) . . ? _diffrn_measured_fraction_theta_max 0.999 _diffrn_reflns_theta_full 24.97 _diffrn_measured_fraction_theta_full 0.999 _refine_diff_density_max 1.377 _refine_diff_density_min -1.523 _refine_diff_density_rms 0.144