# Supplementary Material (ESI) for Dalton Transactions # This journal is (c) The Royal Society of Chemistry 2010 data_global _journal_name_full 'Dalton Trans.' _journal_coden_Cambridge 0222 _publ_contact_author_name 'Spencer, Elinor' _publ_contact_author_email elinor.c.spencer@gmail.com _publ_section_title ; Re-determination of the Structure of an Anionic Oxovanadium Arsenate Framework ; _publ_author_name E.Spencer # Attachment '- Soghomonian_CIF.cif' data_complex_1 _database_code_depnum_ccdc_archive 'CCDC 776172' #TrackingRef '- Soghomonian_CIF.cif' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'As6 O51 V15' _chemical_formula_sum 'As6 O51 V15' _chemical_formula_weight 2029.62 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' V V 0.3005 0.5294 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' As As 0.0499 2.0058 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M Im-3m _symmetry_space_group_name_Hall '-I 4 2 3' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x, z' '-x, -y, z' 'y, -x, z' 'x, -z, y' 'x, -y, -z' 'x, z, -y' 'z, y, -x' '-x, y, -z' '-z, y, x' 'z, x, y' 'y, z, x' '-y, -z, x' 'z, -x, -y' '-y, z, -x' '-z, -x, y' '-z, x, -y' 'y, -z, -x' 'y, x, -z' '-y, -x, -z' '-x, z, y' '-x, -z, -y' 'z, -y, x' '-z, -y, -x' 'x+1/2, y+1/2, z+1/2' '-y+1/2, x+1/2, z+1/2' '-x+1/2, -y+1/2, z+1/2' 'y+1/2, -x+1/2, z+1/2' 'x+1/2, -z+1/2, y+1/2' 'x+1/2, -y+1/2, -z+1/2' 'x+1/2, z+1/2, -y+1/2' 'z+1/2, y+1/2, -x+1/2' '-x+1/2, y+1/2, -z+1/2' '-z+1/2, y+1/2, x+1/2' 'z+1/2, x+1/2, y+1/2' 'y+1/2, z+1/2, x+1/2' '-y+1/2, -z+1/2, x+1/2' 'z+1/2, -x+1/2, -y+1/2' '-y+1/2, z+1/2, -x+1/2' '-z+1/2, -x+1/2, y+1/2' '-z+1/2, x+1/2, -y+1/2' 'y+1/2, -z+1/2, -x+1/2' 'y+1/2, x+1/2, -z+1/2' '-y+1/2, -x+1/2, -z+1/2' '-x+1/2, z+1/2, y+1/2' '-x+1/2, -z+1/2, -y+1/2' 'z+1/2, -y+1/2, x+1/2' '-z+1/2, -y+1/2, -x+1/2' '-x, -y, -z' 'y, -x, -z' 'x, y, -z' '-y, x, -z' '-x, z, -y' '-x, y, z' '-x, -z, y' '-z, -y, x' 'x, -y, z' 'z, -y, -x' '-z, -x, -y' '-y, -z, -x' 'y, z, -x' '-z, x, y' 'y, -z, x' 'z, x, -y' 'z, -x, y' '-y, z, x' '-y, -x, z' 'y, x, z' 'x, -z, -y' 'x, z, y' '-z, y, -x' 'z, y, x' '-x+1/2, -y+1/2, -z+1/2' 'y+1/2, -x+1/2, -z+1/2' 'x+1/2, y+1/2, -z+1/2' '-y+1/2, x+1/2, -z+1/2' '-x+1/2, z+1/2, -y+1/2' '-x+1/2, y+1/2, z+1/2' '-x+1/2, -z+1/2, y+1/2' '-z+1/2, -y+1/2, x+1/2' 'x+1/2, -y+1/2, z+1/2' 'z+1/2, -y+1/2, -x+1/2' '-z+1/2, -x+1/2, -y+1/2' '-y+1/2, -z+1/2, -x+1/2' 'y+1/2, z+1/2, -x+1/2' '-z+1/2, x+1/2, y+1/2' 'y+1/2, -z+1/2, x+1/2' 'z+1/2, x+1/2, -y+1/2' 'z+1/2, -x+1/2, y+1/2' '-y+1/2, z+1/2, x+1/2' '-y+1/2, -x+1/2, z+1/2' 'y+1/2, x+1/2, z+1/2' 'x+1/2, -z+1/2, -y+1/2' 'x+1/2, z+1/2, y+1/2' '-z+1/2, y+1/2, -x+1/2' 'z+1/2, y+1/2, x+1/2' _cell_length_a 16.62170(10) _cell_length_b 16.62170(10) _cell_length_c 16.62170(10) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 4592.26(5) _cell_formula_units_Z 2 _cell_measurement_temperature 100(2) _cell_measurement_reflns_used 6774 _cell_measurement_theta_min 3.8534 _cell_measurement_theta_max 24.9980 _exptl_crystal_description Cube _exptl_crystal_colour 'Dark green' _exptl_crystal_size_max 0.0832 _exptl_crystal_size_mid 0.0801 _exptl_crystal_size_min 0.0720 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 1.468 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1902 _exptl_absorpt_coefficient_mu 3.657 _exptl_absorpt_correction_T_min 0.751 _exptl_absorpt_correction_T_max 0.791 _exptl_absorpt_correction_type analytical _exptl_absorpt_process_details ; CrysAlis RED, Oxford Diffraction Ltd., Version 1.171.32.29 (release 10-06-2008 CrysAlis171 .NET) (compiled Jun 10 2008,16:49:55) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897) ; _diffrn_ambient_temperature 100(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 '\k-geometry diffractometer' _diffrn_measurement_device_type 'Oxford Diffraction Gemini' _diffrn_detector CCD _diffrn_detector_type 'Oxford Diffraction Atlas CCD' _diffrn_source_voltage 50 _diffrn_source_current 40 _diffrn_measurement_method 'phi and omega scans' _diffrn_detector_area_resol_mean 10.2265 _diffrn_standards_number 2 _diffrn_standards_interval_count 50 _diffrn_standards_interval_time ? _diffrn_standards_decay_% <2% _diffrn_reflns_number 27190 _diffrn_reflns_av_R_equivalents 0.0755 _diffrn_reflns_av_sigmaI/netI 0.0204 _diffrn_reflns_limit_h_min -19 _diffrn_reflns_limit_h_max 19 _diffrn_reflns_limit_k_min -19 _diffrn_reflns_limit_k_max 19 _diffrn_reflns_limit_l_min -19 _diffrn_reflns_limit_l_max 19 _diffrn_reflns_theta_min 3.88 _diffrn_reflns_theta_max 25.11 _reflns_number_total 437 _reflns_number_gt 336 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'CrysAlisPro (Oxford Diffraction, 2009)' _computing_cell_refinement 'CrysAlisPro (Oxford Diffraction, 2009)' _computing_data_reduction 'CrysAlisPro (Oxford Diffraction, 2009)' _computing_structure_solution 'SHELXS-97 (Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.)' _computing_molecular_graphics 'CrystalMaker v2.0' _computing_publication_material 'SHELXTL (Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.)' _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^)+(0.1669P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens . _refine_ls_hydrogen_treatment . _refine_ls_extinction_method none _refine_ls_extinction_coef . _refine_ls_number_reflns 437 _refine_ls_number_parameters 33 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0878 _refine_ls_R_factor_gt 0.0791 _refine_ls_wR_factor_ref 0.2214 _refine_ls_wR_factor_gt 0.2160 _refine_ls_goodness_of_fit_ref 1.087 _refine_ls_restrained_S_all 1.087 _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 As1 As 0.5000 0.0000 0.2500 0.0432(9) Uani 1 8 d S . . V1 V 0.5000 0.1473(3) 0.5000 0.0403(14) Uani 0.50 8 d SP . . V2 V 0.61271(13) 0.0758(2) 0.38729(13) 0.0503(11) Uani 0.50 2 d SP . . O1 O 0.5838(4) 0.0000 0.3064(3) 0.0546(17) Uani 1 2 d S . . O2 O 0.5000 0.2426(14) 0.5000 0.069(9) Uani 0.50 8 d SP . . O3 O 0.6579(6) 0.1487(8) 0.3421(6) 0.059(3) Uani 0.50 2 d SP . . O4 O 0.6080(6) 0.1106(6) 0.5000 0.041(3) Uani 0.50 2 d SP . . 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 As1 0.0488(10) 0.0488(10) 0.0320(11) 0.000 0.000 0.000 V1 0.044(2) 0.032(3) 0.044(2) 0.000 0.000 0.000 V2 0.0438(12) 0.063(2) 0.0438(12) -0.0007(10) 0.0012(13) 0.0007(10) O1 0.052(4) 0.073(4) 0.039(3) 0.000 -0.004(3) 0.000 O2 0.087(14) 0.035(14) 0.087(14) 0.000 0.000 0.000 O3 0.056(5) 0.067(8) 0.056(5) 0.017(5) -0.012(6) -0.017(5) O4 0.037(6) 0.039(6) 0.048(7) 0.000 0.000 -0.008(5) _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 As1 O1 1.678(6) 74 ? As1 O1 1.678(6) . ? As1 O1 1.678(6) 76_545 ? As1 O1 1.678(6) 3_655 ? V1 O2 1.58(2) . ? V1 O4 1.896(11) 8_556 ? V1 O4 1.896(11) 54_655 ? V1 O4 1.896(11) 10_655 ? V1 O4 1.896(11) . ? V1 V2 2.903(4) 54_655 ? V1 V2 2.903(4) . ? V1 V2 2.903(4) 51_556 ? V1 V2 2.903(4) 9_656 ? V2 O3 1.612(13) . ? V2 O1 1.905(5) . ? V2 O1 1.905(5) 71_656 ? V2 O4 1.962(4) . ? V2 O4 1.962(4) 8_556 ? V2 V2 2.520(7) 57 ? O1 V2 1.905(5) 57 ? O4 V2 1.962(4) 51_556 ? 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 O1 As1 O1 108.18(19) 74 . ? O1 As1 O1 112.1(4) 74 76_545 ? O1 As1 O1 108.18(19) . 76_545 ? O1 As1 O1 108.18(19) 74 3_655 ? O1 As1 O1 112.1(4) . 3_655 ? O1 As1 O1 108.18(19) 76_545 3_655 ? O2 V1 O4 108.8(3) . 8_556 ? O2 V1 O4 108.8(3) . 54_655 ? O4 V1 O4 84.1(2) 8_556 54_655 ? O2 V1 O4 108.8(3) . 10_655 ? O4 V1 O4 142.5(7) 8_556 10_655 ? O4 V1 O4 84.1(2) 54_655 10_655 ? O2 V1 O4 108.8(3) . . ? O4 V1 O4 84.1(2) 8_556 . ? O4 V1 O4 142.5(7) 54_655 . ? O4 V1 O4 84.1(2) 10_655 . ? O2 V1 V2 114.15(12) . 54_655 ? O4 V1 V2 42.05(9) 8_556 54_655 ? O4 V1 V2 42.05(9) 54_655 54_655 ? O4 V1 V2 118.6(3) 10_655 54_655 ? O4 V1 V2 118.6(3) . 54_655 ? O2 V1 V2 114.15(12) . . ? O4 V1 V2 42.05(9) 8_556 . ? O4 V1 V2 118.6(3) 54_655 . ? O4 V1 V2 118.6(3) 10_655 . ? O4 V1 V2 42.05(9) . . ? V2 V1 V2 80.36(9) 54_655 . ? O2 V1 V2 114.15(12) . 51_556 ? O4 V1 V2 118.6(3) 8_556 51_556 ? O4 V1 V2 118.6(3) 54_655 51_556 ? O4 V1 V2 42.05(9) 10_655 51_556 ? O4 V1 V2 42.05(9) . 51_556 ? V2 V1 V2 131.7(2) 54_655 51_556 ? V2 V1 V2 80.36(9) . 51_556 ? O2 V1 V2 114.15(12) . 9_656 ? O4 V1 V2 118.6(3) 8_556 9_656 ? O4 V1 V2 42.05(9) 54_655 9_656 ? O4 V1 V2 42.05(9) 10_655 9_656 ? O4 V1 V2 118.6(3) . 9_656 ? V2 V1 V2 80.36(9) 54_655 9_656 ? V2 V1 V2 131.7(2) . 9_656 ? V2 V1 V2 80.36(9) 51_556 9_656 ? O3 V2 O1 106.6(4) . . ? O3 V2 O1 106.6(4) . 71_656 ? O1 V2 O1 85.3(3) . 71_656 ? O3 V2 O4 104.0(5) . . ? O1 V2 O4 149.2(4) . . ? O1 V2 O4 89.0(4) 71_656 . ? O3 V2 O4 104.0(5) . 8_556 ? O1 V2 O4 89.0(4) . 8_556 ? O1 V2 O4 149.2(4) 71_656 8_556 ? O4 V2 O4 80.6(6) . 8_556 ? O3 V2 V2 138.7(5) . 57 ? O1 V2 V2 48.57(14) . 57 ? O1 V2 V2 48.57(14) 71_656 57 ? O4 V2 V2 107.1(3) . 57 ? O4 V2 V2 107.1(3) 8_556 57 ? O3 V2 V1 107.1(5) . . ? O1 V2 V1 124.3(2) . . ? O1 V2 V1 124.3(2) 71_656 . ? O4 V2 V1 40.3(3) . . ? O4 V2 V1 40.3(3) 8_556 . ? V2 V2 V1 114.15(12) 57 . ? As1 O1 V2 127.2(2) . . ? As1 O1 V2 127.2(2) . 57 ? V2 O1 V2 82.9(3) . 57 ? V1 O4 V2 97.6(3) . . ? V1 O4 V2 97.6(3) . 51_556 ? V2 O4 V2 145.4(6) . 51_556 ? _diffrn_measured_fraction_theta_max 0.986 _diffrn_reflns_theta_full 25.11 _diffrn_measured_fraction_theta_full 0.986 _refine_diff_density_max 1.835 _refine_diff_density_min -0.656 _refine_diff_density_rms 0.205