# Supplementary Material (ESI) for ChemComm # This journal is © The Royal Society of Chemistry 2000 # CCDC Number: 182/1764 data_MoSb2Se _audit_creation_method SHELXL _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_formula_moiety ? _chemical_formula_structural ? _chemical_formula_analytical ? _chemical_formula_sum 'Mo Sb2 Se' _chemical_formula_weight 418.40 _chemical_melting_point ? _chemical_compound_source ? loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source 'Se' 'Se' -0.0929 2.2259 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Mo' 'Mo' -1.6832 0.6857 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Sb' 'Sb' -0.5866 1.5461 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting 1 _symmetry_space_group_name_H-M P21/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 6.5728(4) _cell_length_b 6.4941(3) _cell_length_c 18.2990(10) _cell_angle_alpha 90.00 _cell_angle_beta 94.246(8) _cell_angle_gamma 90.00 _cell_volume 778.94(7) _cell_formula_units_Z 8 _cell_measurement_temperature 293(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description needle _exptl_crystal_colour black _exptl_crystal_size_max 0.09 _exptl_crystal_size_mid 0.03 _exptl_crystal_size_min 0.02 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 7.136 _exptl_crystal_density_method ? _exptl_crystal_F_000 1424 _exptl_absorpt_coefficient_mu 26.035 _exptl_absorpt_correction_type numerical _exptl_absorpt_correction_T_min 0.25 _exptl_absorpt_correction_T_max 0.38 _exptl_special_details ; ? ; _diffrn_ambient_temperature 293(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 ? _diffrn_measurement_method ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 13328 _diffrn_reflns_av_R_equivalents 0.0338 _diffrn_reflns_av_sigmaI/netI 0.0199 _diffrn_reflns_limit_h_min -9 _diffrn_reflns_limit_h_max 9 _diffrn_reflns_limit_k_min -8 _diffrn_reflns_limit_k_max 8 _diffrn_reflns_limit_l_min -25 _diffrn_reflns_limit_l_max 25 _diffrn_reflns_theta_min 3.11 _diffrn_reflns_theta_max 30.27 _reflns_number_total 2214 _reflns_number_observed 1403 _reflns_observed_criterion 2sigma(I) _computing_data_collection ? _computing_cell_refinement ? _computing_data_reduction ? _computing_structure_solution 'SHELXS-86 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-93 (Sheldrick, 1993)' _computing_molecular_graphics ? _computing_publication_material ? _refine_special_details ; Refinement on F^2^ for ALL reflections except for 0 with very negative F^2^ or flagged by the user for potential systematic errors. Weighted R- factors wR and all goodnesses 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 observed criterion of F^2^ 2sigma(F^2^) is used only for calculating _R_factor_obs 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 w=1/[\s^2^(Fo^2^)+(0.0200P)^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 ? _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef 0.00029(5) _refine_ls_extinction_expression 'Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^' _refine_ls_number_reflns 2214 _refine_ls_number_parameters 74 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0384 _refine_ls_R_factor_obs 0.0205 _refine_ls_wR_factor_all 0.0468 _refine_ls_wR_factor_obs 0.0437 _refine_ls_goodness_of_fit_all 1.038 _refine_ls_goodness_of_fit_obs 1.229 _refine_ls_restrained_S_all 1.038 _refine_ls_restrained_S_obs 1.229 _refine_ls_shift/esd_max 0.193 _refine_ls_shift/esd_mean 0.031 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_thermal_displace_type _atom_site_occupancy _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_group Sb1 Sb 0.07475(3) 0.3744(3) 0.075975(13) 0.00471(7) Uani 1 d . . Sb2 Sb 0.07472(3) -0.1253(3) 0.075820(13) 0.00484(7) Uani 1 d . . Sb3 Sb 0.20296(7) 0.3499(2) 0.22816(3) 0.0119(2) Uani 1 d . . Sb4 Sb 0.20267(7) -0.1001(2) 0.22806(3) 0.0122(2) Uani 1 d . . Mo1 Mo 0.32480(4) 0.1251(3) -0.00586(2) 0.00324(8) Uani 1 d . . Mo2 Mo -0.32494(4) 0.3753(3) 0.00574(2) 0.00317(8) Uani 1 d . . Se1 Se 0.58605(5) 0.1249(4) 0.10200(2) 0.00530(8) Uani 1 d . . Se2 Se 0.41440(5) 0.3753(4) -0.10202(2) 0.00532(8) Uani 1 d . . 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 Sb1 0.00237(12) 0.00669(14) 0.00528(12) -0.0003(6) 0.00168(8) -0.0008(5) Sb2 0.00237(12) 0.00685(14) 0.00551(12) -0.0006(6) 0.00166(8) -0.0008(5) Sb3 0.01436(14) 0.0138(5) 0.00769(13) -0.0004(2) 0.00065(9) -0.0010(2) Sb4 0.01420(14) 0.0146(5) 0.00782(13) 0.0009(2) 0.00069(9) 0.0009(2) Mo1 0.00119(14) 0.0043(2) 0.00439(15) 0.0006(7) 0.00107(10) -0.0010(6) Mo2 0.00114(14) 0.0042(2) 0.00428(15) 0.0007(7) 0.00094(10) -0.0011(6) Se1 0.0054(2) 0.0057(2) 0.0050(2) 0.0007(9) 0.00110(12) -0.0008(8) Se2 0.0054(2) 0.0058(2) 0.0048(2) 0.0008(9) 0.00069(12) -0.0007(8) _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 Sb1 Mo1 2.816(2) . ? Sb1 Mo2 2.819(2) 3_565 ? Sb1 Mo2 2.8379(4) . ? Sb1 Sb3 2.8536(6) . ? Sb1 Sb2 3.2451(3) . ? Sb1 Sb2 3.2490(3) 1_565 ? Sb1 Sb2 3.300(2) 3 ? Sb1 Sb1 3.310(2) 3_565 ? Sb2 Mo2 2.816(2) 3 ? Sb2 Mo1 2.819(2) . ? Sb2 Mo1 2.8349(4) 3 ? Sb2 Sb4 2.8545(6) . ? Sb2 Sb1 3.2490(3) 1_545 ? Sb2 Sb1 3.300(2) 3 ? Sb2 Sb2 3.303(2) 3 ? Sb3 Sb4 2.8587(4) 2 ? Sb3 Sb4 2.9224(4) . ? Sb4 Sb3 2.8587(4) 2_545 ? Mo1 Se1 2.495(2) 3_655 ? Mo1 Se2 2.497(2) . ? Mo1 Se1 2.5185(5) . ? Mo1 Mo1 2.814(3) 3_655 ? Mo1 Mo2 2.813(3) 1_655 ? Mo1 Sb2 2.8349(4) 3 ? Mo2 Se2 2.495(2) 3_565 ? Mo2 Se1 2.498(2) 1_455 ? Mo2 Se2 2.5146(5) 1_455 ? Mo2 Mo2 2.809(3) 3_465 ? Mo2 Mo1 2.813(3) 1_455 ? Mo2 Sb2 2.816(2) 3 ? Mo2 Sb1 2.819(2) 3_565 ? Se1 Mo1 2.495(2) 3_655 ? Se1 Mo2 2.498(2) 1_655 ? Se2 Mo2 2.495(2) 3_565 ? Se2 Mo2 2.5146(5) 1_655 ? 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 Mo1 Sb1 Mo2 70.306(11) . 3_565 ? Mo1 Sb1 Mo2 108.51(4) . . ? Mo2 Sb1 Mo2 108.39(4) 3_565 . ? Mo1 Sb1 Sb3 110.19(4) . . ? Mo2 Sb1 Sb3 114.08(4) 3_565 . ? Mo2 Sb1 Sb3 129.69(2) . . ? Mo1 Sb1 Sb2 54.88(5) . . ? Mo2 Sb1 Sb2 125.18(5) 3_565 . ? Mo2 Sb1 Sb2 90.09(6) . . ? Sb3 Sb1 Sb2 86.86(5) . . ? Mo1 Sb1 Sb2 125.06(5) . 1_565 ? Mo2 Sb1 Sb2 54.75(5) 3_565 1_565 ? Mo2 Sb1 Sb2 89.86(6) . 1_565 ? Sb3 Sb1 Sb2 93.24(5) . 1_565 ? Sb2 Sb1 Sb2 179.900(13) . 1_565 ? Mo1 Sb1 Sb2 54.53(3) . 3 ? Mo2 Sb1 Sb2 89.15(3) 3_565 3 ? Mo2 Sb1 Sb2 53.98(3) . 3 ? Sb3 Sb1 Sb2 147.35(10) . 3 ? Sb2 Sb1 Sb2 60.60(6) . 3 ? Sb2 Sb1 Sb2 119.30(6) 1_565 3 ? Mo1 Sb1 Sb1 89.15(3) . 3_565 ? Mo2 Sb1 Sb1 54.46(3) 3_565 3_565 ? Mo2 Sb1 Sb1 53.93(3) . 3_565 ? Sb3 Sb1 Sb1 153.53(10) . 3_565 ? Sb2 Sb1 Sb1 119.49(6) . 3_565 ? Sb2 Sb1 Sb1 60.42(6) 1_565 3_565 ? Sb2 Sb1 Sb1 58.881(9) 3 3_565 ? Mo2 Sb2 Mo1 70.440(11) 3 . ? Mo2 Sb2 Mo1 108.58(4) 3 3 ? Mo1 Sb2 Mo1 108.50(4) . 3 ? Mo2 Sb2 Sb4 114.13(4) 3 . ? Mo1 Sb2 Sb4 110.07(4) . . ? Mo1 Sb2 Sb4 129.55(2) 3 . ? Mo2 Sb2 Sb1 125.23(5) 3 . ? Mo1 Sb2 Sb1 54.79(5) . . ? Mo1 Sb2 Sb1 90.00(6) 3 . ? Sb4 Sb2 Sb1 86.66(5) . . ? Mo2 Sb2 Sb1 54.83(5) 3 1_545 ? Mo1 Sb2 Sb1 125.27(5) . 1_545 ? Mo1 Sb2 Sb1 90.04(6) 3 1_545 ? Sb4 Sb2 Sb1 93.24(5) . 1_545 ? Sb1 Sb2 Sb1 179.900(9) . 1_545 ? Mo2 Sb2 Sb1 54.59(3) 3 3 ? Mo1 Sb2 Sb1 89.17(3) . 3 ? Mo1 Sb2 Sb1 53.99(3) 3 3 ? Sb4 Sb2 Sb1 153.81(10) . 3 ? Sb1 Sb2 Sb1 119.40(6) . 3 ? Sb1 Sb2 Sb1 60.70(6) 1_545 3 ? Mo2 Sb2 Sb2 89.30(3) 3 3 ? Mo1 Sb2 Sb2 54.48(3) . 3 ? Mo1 Sb2 Sb2 54.02(3) 3 3 ? Sb4 Sb2 Sb2 147.08(10) . 3 ? Sb1 Sb2 Sb2 60.53(6) . 3 ? Sb1 Sb2 Sb2 119.57(6) 1_545 3 ? Sb1 Sb2 Sb2 58.868(9) 3 3 ? Sb1 Sb3 Sb4 93.04(2) . 2 ? Sb1 Sb3 Sb4 93.15(5) . . ? Sb4 Sb3 Sb4 96.50(2) 2 . ? Sb2 Sb4 Sb3 93.07(2) . 2_545 ? Sb2 Sb4 Sb3 93.33(5) . . ? Sb3 Sb4 Sb3 96.55(2) 2_545 . ? Se1 Mo1 Se2 81.177(15) 3_655 . ? Se1 Mo1 Se1 111.71(6) 3_655 . ? Se2 Mo1 Se1 111.72(6) . . ? Se1 Mo1 Mo1 56.25(5) 3_655 3_655 ? Se2 Mo1 Mo1 101.25(4) . 3_655 ? Se1 Mo1 Mo1 55.47(5) . 3_655 ? Se1 Mo1 Mo2 101.27(4) 3_655 1_655 ? Se2 Mo1 Mo2 56.16(5) . 1_655 ? Se1 Mo1 Mo2 55.56(5) . 1_655 ? Mo1 Mo1 Mo2 70.557(12) 3_655 1_655 ? Se1 Mo1 Sb1 157.78(3) 3_655 . ? Se2 Mo1 Sb1 100.26(9) . . ? Se1 Mo1 Sb1 88.54(5) . . ? Mo1 Mo1 Sb1 142.95(2) 3_655 . ? Mo2 Mo1 Sb1 97.73(10) 1_655 . ? Se1 Mo1 Sb2 100.08(9) 3_655 . ? Se2 Mo1 Sb2 157.86(3) . . ? Se1 Mo1 Sb2 88.54(5) . . ? Mo1 Mo1 Sb2 97.61(9) 3_655 . ? Mo2 Mo1 Sb2 143.07(2) 1_655 . ? Sb1 Mo1 Sb2 70.330(10) . . ? Se1 Mo1 Sb2 86.55(4) 3_655 3 ? Se2 Mo1 Sb2 86.59(4) . 3 ? Se1 Mo1 Sb2 155.36(2) . 3 ? Mo1 Mo1 Sb2 139.48(10) 3_655 3 ? Mo2 Mo1 Sb2 139.42(10) 1_655 3 ? Sb1 Mo1 Sb2 71.48(4) . 3 ? Sb2 Mo1 Sb2 71.50(4) . 3 ? Se2 Mo2 Se1 81.082(15) 3_565 1_455 ? Se2 Mo2 Se2 111.79(6) 3_565 1_455 ? Se1 Mo2 Se2 111.80(6) 1_455 1_455 ? Se2 Mo2 Mo2 56.22(5) 3_565 3_465 ? Se1 Mo2 Mo2 101.23(4) 1_455 3_465 ? Se2 Mo2 Mo2 55.57(5) 1_455 3_465 ? Se2 Mo2 Mo1 101.18(4) 3_565 1_455 ? Se1 Mo2 Mo1 56.24(5) 1_455 1_455 ? Se2 Mo2 Mo1 55.57(5) 1_455 1_455 ? Mo2 Mo2 Mo1 70.489(12) 3_465 1_455 ? Se2 Mo2 Sb2 157.78(3) 3_565 3 ? Se1 Mo2 Sb2 100.07(9) 1_455 3 ? Se2 Mo2 Sb2 88.58(5) 1_455 3 ? Mo2 Mo2 Sb2 143.13(2) 3_465 3 ? Mo1 Mo2 Sb2 97.70(10) 1_455 3 ? Se2 Mo2 Sb1 100.22(9) 3_565 3_565 ? Se1 Mo2 Sb1 157.75(3) 1_455 3_565 ? Se2 Mo2 Sb1 88.53(5) 1_455 3_565 ? Mo2 Mo2 Sb1 97.73(9) 3_465 3_565 ? Mo1 Mo2 Sb1 143.07(2) 1_455 3_565 ? Sb2 Mo2 Sb1 70.416(10) 3 3_565 ? Se2 Mo2 Sb1 86.57(4) 3_565 . ? Se1 Mo2 Sb1 86.37(4) 1_455 . ? Se2 Mo2 Sb1 155.40(2) 1_455 . ? Mo2 Mo2 Sb1 139.53(10) 3_465 . ? Mo1 Mo2 Sb1 139.30(10) 1_455 . ? Sb2 Mo2 Sb1 71.43(4) 3 . ? Sb1 Mo2 Sb1 71.61(4) 3_565 . ? Mo1 Se1 Mo2 81.200(15) 3_655 1_655 ? Mo1 Se1 Mo1 68.29(6) 3_655 . ? Mo2 Se1 Mo1 68.20(6) 1_655 . ? Mo2 Se2 Mo1 81.058(15) 3_565 . ? Mo2 Se2 Mo2 68.21(6) 3_565 1_655 ? Mo1 Se2 Mo2 68.28(6) . 1_655 ? _refine_diff_density_max 1.276 _refine_diff_density_min -1.459 _refine_diff_density_rms 0.267