# Electronic Supplementary Material (ESI) for Dalton Transactions # This journal is © The Royal Society of Chemistry 2011 data_global _journal_name_full 'Dalton Trans.' _journal_coden_cambridge 0222 _journal_year ? _journal_volume ? _journal_page_first ? loop_ _publ_author_name G.Adamova R.L.Gardas M.Nieuwenhuyzen A.V.Puga L.P.N.Rebelo ; A.J.Robertson ; K.R.Seddon _publ_contact_author_name 'Gabriela Adamova' _publ_contact_author_email gadamova01@qub.ac.uk data_p10prr185 _database_code_depnum_ccdc_archive 'CCDC 818409' #TrackingRef '- p10prr185.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C15 H34 Cl P' _chemical_formula_weight 280.84 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 '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' P P 0.2955 0.4335 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Cl Cl 0.3639 0.7018 '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 9.9996(5) _cell_length_b 13.4309(12) _cell_length_c 13.3481(10) _cell_angle_alpha 90.00 _cell_angle_beta 91.331(5) _cell_angle_gamma 90.00 _cell_volume 1792.2(2) _cell_formula_units_Z 4 _cell_measurement_temperature 150(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description Plate _exptl_crystal_colour colourless _exptl_crystal_size_max 0.15 _exptl_crystal_size_mid 0.15 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.041 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 624 _exptl_absorpt_coefficient_mu 2.565 _exptl_absorpt_correction_type empirical _exptl_absorpt_correction_T_min 0.6996 _exptl_absorpt_correction_T_max 0.8825 _exptl_absorpt_process_details Multiscan _exptl_special_details ; Crystals showed weak diffraction and thus data were collected for max two-theta of 114 degrees ; _diffrn_ambient_temperature 150(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'multiwire proportional' _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 7858 _diffrn_reflns_av_R_equivalents 0.0821 _diffrn_reflns_av_sigmaI/netI 0.0560 _diffrn_reflns_limit_h_min -10 _diffrn_reflns_limit_h_max 10 _diffrn_reflns_limit_k_min -14 _diffrn_reflns_limit_k_max 14 _diffrn_reflns_limit_l_min -12 _diffrn_reflns_limit_l_max 14 _diffrn_reflns_theta_min 4.42 _diffrn_reflns_theta_max 56.65 _reflns_number_total 2329 _reflns_number_gt 1602 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker FRAMBO' _computing_cell_refinement 'Bruker FRAMBO' _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. The disorder model was fixed at 50:50 as this provides the best fit to the data taking into account the necessary chemical restraints.This data was not checked for twinning or psuedosymmetry. It was not necessary as a chemically reasonable model was obtained using the disorder model. Model was restrained using a combination of SAME and SADI instructions ; _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^)+(0.1629P)^2^+0.8109P] 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 none _refine_ls_number_reflns 2329 _refine_ls_number_parameters 139 _refine_ls_number_restraints 302 _refine_ls_R_factor_all 0.1140 _refine_ls_R_factor_gt 0.0821 _refine_ls_wR_factor_ref 0.2539 _refine_ls_wR_factor_gt 0.2273 _refine_ls_goodness_of_fit_ref 1.065 _refine_ls_restrained_S_all 1.136 _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 Cl1 Cl 0.44536(17) -0.18973(10) 0.41073(9) 0.0680(6) Uani 1 1 d . . . P1 P 0.60233(15) 0.09270(11) 0.31266(9) 0.0553(6) Uani 0.50 1 d PD A 1 C11 C 0.648(2) 0.0560(11) 0.1873(9) 0.044(7) Uiso 0.50 1 d PD A 1 H11A H 0.6065 0.1021 0.1380 0.053 Uiso 0.50 1 calc PR A 1 H11B H 0.7466 0.0609 0.1813 0.053 Uiso 0.50 1 calc PR A 1 C12 C 0.6035(16) -0.0510(10) 0.1634(9) 0.049(5) Uiso 0.50 1 d PD A 1 H12A H 0.6471 -0.0969 0.2121 0.059 Uiso 0.50 1 calc PR A 1 H12B H 0.5056 -0.0560 0.1720 0.059 Uiso 0.50 1 calc PR A 1 C13 C 0.6364(14) -0.0841(14) 0.0583(11) 0.048(5) Uiso 0.50 1 d PD A 1 H13A H 0.5783 -0.1400 0.0363 0.058 Uiso 0.50 1 calc PR A 1 H13B H 0.6260 -0.0285 0.0101 0.058 Uiso 0.50 1 calc PR A 1 C14 C 0.7808(13) -0.1167(12) 0.0678(12) 0.093(4) Uiso 0.50 1 d PD A 1 H14A H 0.8131 -0.1354 0.0017 0.140 Uiso 0.50 1 calc PR A 1 H14B H 0.7878 -0.1739 0.1131 0.140 Uiso 0.50 1 calc PR A 1 H14C H 0.8351 -0.0617 0.0948 0.140 Uiso 0.50 1 calc PR A 1 C21 C 0.6628(13) 0.2161(8) 0.3330(11) 0.042(5) Uiso 0.50 1 d PD A 1 H21A H 0.6039 0.2617 0.2941 0.050 Uiso 0.50 1 calc PR A 1 H21B H 0.6511 0.2319 0.4047 0.050 Uiso 0.50 1 calc PR A 1 C22 C 0.8048(12) 0.2409(9) 0.3081(11) 0.063(4) Uiso 0.50 1 d PD A 1 H22A H 0.8191 0.2251 0.2367 0.075 Uiso 0.50 1 calc PR A 1 H22B H 0.8659 0.1985 0.3489 0.075 Uiso 0.50 1 calc PR A 1 C23 C 0.8399(16) 0.3490(9) 0.3265(10) 0.078(4) Uiso 0.50 1 d PD A 1 H23A H 0.7768 0.3920 0.2882 0.094 Uiso 0.50 1 calc PR A 1 H23B H 0.9312 0.3623 0.3027 0.094 Uiso 0.50 1 calc PR A 1 C24 C 0.833(2) 0.3741(15) 0.4377(12) 0.122(6) Uiso 0.50 1 d PD A 1 H24A H 0.8534 0.4449 0.4476 0.184 Uiso 0.50 1 calc PR A 1 H24B H 0.8992 0.3339 0.4753 0.184 Uiso 0.50 1 calc PR A 1 H24C H 0.7436 0.3597 0.4616 0.184 Uiso 0.50 1 calc PR A 1 C31 C 0.4225(11) 0.0921(17) 0.3274(16) 0.070(9) Uiso 0.50 1 d PD A 1 H31A H 0.3917 0.0221 0.3237 0.084 Uiso 0.50 1 calc PR A 1 H31B H 0.4039 0.1164 0.3957 0.084 Uiso 0.50 1 calc PR A 1 C32 C 0.3391(16) 0.1515(15) 0.2550(14) 0.086(6) Uiso 0.50 1 d PD A 1 H32A H 0.3590 0.1289 0.1863 0.104 Uiso 0.50 1 calc PR A 1 H32B H 0.3668 0.2221 0.2603 0.104 Uiso 0.50 1 calc PR A 1 C33 C 0.1886(15) 0.1460(15) 0.2682(14) 0.099(7) Uiso 0.50 1 d PD A 1 H33A H 0.1435 0.1875 0.2174 0.149 Uiso 0.50 1 calc PR A 1 H33B H 0.1666 0.1702 0.3351 0.149 Uiso 0.50 1 calc PR A 1 H33C H 0.1588 0.0769 0.2606 0.149 Uiso 0.50 1 calc PR A 1 C41 C 0.6669(13) 0.0091(9) 0.4019(8) 0.043(4) Uiso 0.50 1 d PD A 1 H41A H 0.6717 0.0420 0.4683 0.052 Uiso 0.50 1 calc PR A 1 H41B H 0.6061 -0.0488 0.4069 0.052 Uiso 0.50 1 calc PR A 1 C42 C 0.8046(14) -0.0266(10) 0.3748(10) 0.055(4) Uiso 0.50 1 d PD A 1 H42A H 0.8682 0.0298 0.3774 0.066 Uiso 0.50 1 calc PR A 1 H42B H 0.8022 -0.0533 0.3056 0.066 Uiso 0.50 1 calc PR A 1 C43 C 0.8511(15) -0.1072(10) 0.4472(10) 0.070(4) Uiso 0.50 1 d PD A 1 H43A H 0.8567 -0.0789 0.5156 0.083 Uiso 0.50 1 calc PR A 1 H43B H 0.7839 -0.1612 0.4472 0.083 Uiso 0.50 1 calc PR A 1 C44 C 0.9836(19) -0.1500(17) 0.4221(17) 0.126(8) Uiso 0.50 1 d PD A 1 H44A H 1.0085 -0.2011 0.4715 0.189 Uiso 0.50 1 calc PR A 1 H44B H 1.0512 -0.0971 0.4232 0.189 Uiso 0.50 1 calc PR A 1 H44C H 0.9783 -0.1799 0.3552 0.189 Uiso 0.50 1 calc PR A 1 P1' P 0.60233(15) 0.09270(11) 0.31266(9) 0.0553(6) Uani 0.50 1 d P B 2 C11' C 0.626(2) 0.0540(13) 0.1855(10) 0.054(9) Uiso 0.50 1 d PD B 2 H11C H 0.5873 0.1056 0.1405 0.065 Uiso 0.50 1 calc PR B 2 H11D H 0.7234 0.0517 0.1737 0.065 Uiso 0.50 1 calc PR B 2 C12' C 0.5663(17) -0.0461(11) 0.1554(10) 0.058(5) Uiso 0.50 1 d PD B 2 H12C H 0.4710 -0.0371 0.1359 0.070 Uiso 0.50 1 calc PR B 2 H12D H 0.5709 -0.0919 0.2135 0.070 Uiso 0.50 1 calc PR B 2 C13' C 0.642(3) -0.093(2) 0.0664(18) 0.125(15) Uiso 0.50 1 d PD B 2 H13C H 0.6029 -0.1579 0.0497 0.187 Uiso 0.50 1 calc PR B 2 H13D H 0.7367 -0.1017 0.0855 0.187 Uiso 0.50 1 calc PR B 2 H13E H 0.6348 -0.0489 0.0080 0.187 Uiso 0.50 1 calc PR B 2 C21' C 0.6330(14) 0.2232(9) 0.3347(14) 0.063(6) Uiso 0.50 1 d PD B 2 H21C H 0.5943 0.2624 0.2783 0.076 Uiso 0.50 1 calc PR B 2 H21D H 0.5879 0.2439 0.3966 0.076 Uiso 0.50 1 calc PR B 2 C22' C 0.7841(13) 0.2458(10) 0.3455(12) 0.074(5) Uiso 0.50 1 d PD B 2 H22C H 0.8241 0.2020 0.3978 0.089 Uiso 0.50 1 calc PR B 2 H22D H 0.8276 0.2306 0.2814 0.089 Uiso 0.50 1 calc PR B 2 C23' C 0.8112(13) 0.3537(10) 0.3732(15) 0.085(4) Uiso 0.50 1 d PD B 2 H23C H 0.7778 0.3970 0.3180 0.102 Uiso 0.50 1 calc PR B 2 H23D H 0.7605 0.3705 0.4338 0.102 Uiso 0.50 1 calc PR B 2 C24' C 0.9561(16) 0.3757(16) 0.3929(16) 0.139(7) Uiso 0.50 1 d PD B 2 H24D H 0.9673 0.4467 0.4077 0.209 Uiso 0.50 1 calc PR B 2 H24E H 1.0073 0.3584 0.3337 0.209 Uiso 0.50 1 calc PR B 2 H24F H 0.9885 0.3364 0.4503 0.209 Uiso 0.50 1 calc PR B 2 C31' C 0.4296(10) 0.0759(16) 0.3340(12) 0.053(7) Uiso 0.50 1 d PD B 2 H31C H 0.4112 0.0038 0.3409 0.063 Uiso 0.50 1 calc PR B 2 H31D H 0.4073 0.1083 0.3981 0.063 Uiso 0.50 1 calc PR B 2 C32' C 0.3388(11) 0.1183(11) 0.2506(9) 0.047(4) Uiso 0.50 1 d PD B 2 H32C H 0.3571 0.0833 0.1871 0.056 Uiso 0.50 1 calc PR B 2 H32D H 0.3601 0.1896 0.2411 0.056 Uiso 0.50 1 calc PR B 2 C33' C 0.1898(11) 0.1079(13) 0.2736(10) 0.065(4) Uiso 0.50 1 d PD B 2 H33C H 0.1712 0.0378 0.2918 0.078 Uiso 0.50 1 calc PR B 2 H33D H 0.1695 0.1499 0.3323 0.078 Uiso 0.50 1 calc PR B 2 C34' C 0.1009(15) 0.1367(13) 0.1894(11) 0.108(5) Uiso 0.50 1 d PD B 2 H34C H 0.0078 0.1345 0.2105 0.161 Uiso 0.50 1 calc PR B 2 H34D H 0.1129 0.0904 0.1335 0.161 Uiso 0.50 1 calc PR B 2 H34E H 0.1229 0.2044 0.1678 0.161 Uiso 0.50 1 calc PR B 2 C41' C 0.7046(13) 0.0109(10) 0.3969(9) 0.051(5) Uiso 0.50 1 d PD B 2 H41C H 0.7130 0.0453 0.4623 0.061 Uiso 0.50 1 calc PR B 2 H41D H 0.6515 -0.0502 0.4081 0.061 Uiso 0.50 1 calc PR B 2 C42' C 0.8450(13) -0.0226(10) 0.3692(10) 0.056(4) Uiso 0.50 1 d PD B 2 H42C H 0.8411 -0.0539 0.3020 0.068 Uiso 0.50 1 calc PR B 2 H42D H 0.9040 0.0364 0.3656 0.068 Uiso 0.50 1 calc PR B 2 C43' C 0.9039(14) -0.0953(9) 0.4433(10) 0.063(4) Uiso 0.50 1 d PD B 2 H43C H 0.8431 -0.1531 0.4496 0.075 Uiso 0.50 1 calc PR B 2 H43D H 0.9128 -0.0631 0.5099 0.075 Uiso 0.50 1 calc PR B 2 C44' C 1.0391(18) -0.1310(16) 0.4111(16) 0.118(7) Uiso 0.50 1 d PD B 2 H44D H 1.0744 -0.1794 0.4598 0.176 Uiso 0.50 1 calc PR B 2 H44E H 1.1004 -0.0742 0.4075 0.176 Uiso 0.50 1 calc PR B 2 H44F H 1.0305 -0.1625 0.3451 0.176 Uiso 0.50 1 calc PR B 2 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 Cl1 0.1035(14) 0.0587(10) 0.0424(9) -0.0063(6) 0.0112(7) -0.0150(8) P1 0.0775(12) 0.0551(10) 0.0334(8) 0.0011(6) 0.0044(6) -0.0073(7) P1' 0.0775(12) 0.0551(10) 0.0334(8) 0.0011(6) 0.0044(6) -0.0073(7) _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 P1 C41 1.750(9) . ? P1 C21 1.783(9) . ? P1 C31 1.814(11) . ? P1 C11 1.814(10) . ? C11 C12 1.537(12) . ? C12 C13 1.515(11) . ? C13 C14 1.511(14) . ? C21 C22 1.503(12) . ? C22 C23 1.512(12) . ? C23 C24 1.524(13) . ? C31 C32 1.493(13) . ? C32 C33 1.521(13) . ? C41 C42 1.510(12) . ? C42 C43 1.517(11) . ? C43 C44 1.489(14) . ? C11' C12' 1.522(13) . ? C12' C13' 1.558(14) . ? C21' C22' 1.544(13) . ? C22' C23' 1.519(12) . ? C23' C24' 1.496(13) . ? C31' C32' 1.531(12) . ? C32' C33' 1.535(11) . ? C33' C34' 1.469(13) . ? C41' C42' 1.528(12) . ? C42' C43' 1.501(11) . ? C43' C44' 1.507(14) . ? 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 C41 P1 C21 112.0(7) . . ? C41 P1 C31 105.9(7) . . ? C21 P1 C31 108.7(9) . . ? C41 P1 C11 110.9(8) . . ? C21 P1 C11 107.5(7) . . ? C31 P1 C11 111.9(10) . . ? C12 C11 P1 111.5(9) . . ? C13 C12 C11 113.4(10) . . ? C14 C13 C12 103.6(11) . . ? C22 C21 P1 119.4(9) . . ? C21 C22 C23 113.2(10) . . ? C22 C23 C24 110.9(12) . . ? C32 C31 P1 117.9(12) . . ? C31 C32 C33 116.0(13) . . ? C42 C41 P1 111.4(8) . . ? C41 C42 C43 110.0(10) . . ? C44 C43 C42 113.2(12) . . ? C11' C12' C13' 111.3(14) . . ? C23' C22' C21' 112.3(10) . . ? C24' C23' C22' 113.4(12) . . ? C31' C32' C33' 112.5(9) . . ? C34' C33' C32' 113.3(11) . . ? C43' C42' C41' 112.4(10) . . ? C42' C43' C44' 111.1(12) . . ? _diffrn_measured_fraction_theta_max 0.976 _diffrn_reflns_theta_full 56.65 _diffrn_measured_fraction_theta_full 0.976 _refine_diff_density_max 0.576 _refine_diff_density_min -0.377 _refine_diff_density_rms 0.080