Supplementary Material (ESI) for Journal of Materials Chemistry This journal is (C) The Royal Society of Chemistry 2006 data_global _journal_name_full J.Mater.Chem. #============================================================================== # 1. SUBMISSION DETAILS _journal_coden_Cambridge 1145 #============================================================================== _audit_creation_date 16-Aug-2006 _audit_creation_method 'from SHELXL97 CIF and IUCr SHELXL97-template' _audit_update_record 4-Dec-2006 _publ_contact_author_name 'Wilhelm Klein' _publ_contact_author_address ; Institut fur Anorganische und Angewandte Chemie Universitat Hamburg Martin-Luther-King-Platz 6 20146 Hamburg Bundesrepublik Deutschland ; _publ_contact_author_phone '0049 40 42838-4308' _publ_contact_author_fax '0049 40 42838-6348' _publ_contact_author_email wilhelm.klein@chemie.uni-hamburg.de #============================================================================== # 3. TITLE AND AUTHOR LIST _publ_section_title ; Hg2Ru2O7, a new pyrochlore showing a metal/insulator transition ; _publ_section_title_footnote ; ? ; loop_ _publ_author_name _publ_author_footnote _publ_author_address 'Wilhelm Klein' ; ? ; ; Institut fur Anorganische und Angewandte Chemie Universitat Hamburg Martin-Luther-King-Platz 6 20146 Hamburg Bundesrepublik Deutschland ; 'Reinhard K. Kremer' ; ? ; ; Max-Planck-Institut fur Festkorperforschung Heisenbergstr. 1 70569 Stuttgart Bundesrepublik Deutschland ; 'Martin Jansen' ; ? ; ; Max-Planck-Institut fur Festkorperforschung Heisenbergstr. 1 70569 Stuttgart Bundesrepublik Deutschland ; #============================================================================== data_hg2ru2o7 _database_code_depnum_ccdc_archive 'CCDC 625829' _audit_creation_method SHELXL-97 _chemical_name_systematic ; Dimercury(II) Heptaoxodiruthenate(V) ; _chemical_name_common 'Dimercury(ii) Heptaoxodiruthenate(V)' _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'Hg2 O7 Ru2' _chemical_formula_weight 715.32 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source Hg Hg -2.3894 9.2266 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Ru Ru -1.2594 0.8363 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting cubic _symmetry_space_group_name_H-M Fd-3m _symmetry_Int_Tables_number 227 loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x, -y+1/4, -z+1/4' '-x+1/4, y, -z+1/4' '-x+1/4, -y+1/4, z' 'y, z, x' '-y+1/4, -z+1/4, x' 'y, -z+1/4, -x+1/4' '-y+1/4, z, -x+1/4' 'z, x, y' '-z+1/4, x, -y+1/4' '-z+1/4, -x+1/4, y' 'z, -x+1/4, -y+1/4' 'x, z, y' 'x, -z+1/4, -y+1/4' '-x+1/4, -z+1/4, y' '-x+1/4, z, -y+1/4' 'y, x, z' '-y+1/4, x, -z+1/4' 'y, -x+1/4, -z+1/4' '-y+1/4, -x+1/4, z' 'z, y, x' '-z+1/4, -y+1/4, x' '-z+1/4, y, -x+1/4' 'z, -y+1/4, -x+1/4' 'x, y+1/2, z+1/2' 'x, -y+3/4, -z+3/4' '-x+1/4, y+1/2, -z+3/4' '-x+1/4, -y+3/4, z+1/2' 'y, z+1/2, x+1/2' '-y+1/4, -z+3/4, x+1/2' 'y, -z+3/4, -x+3/4' '-y+1/4, z+1/2, -x+3/4' 'z, x+1/2, y+1/2' '-z+1/4, x+1/2, -y+3/4' '-z+1/4, -x+3/4, y+1/2' 'z, -x+3/4, -y+3/4' 'x, z+1/2, y+1/2' 'x, -z+3/4, -y+3/4' '-x+1/4, -z+3/4, y+1/2' '-x+1/4, z+1/2, -y+3/4' 'y, x+1/2, z+1/2' '-y+1/4, x+1/2, -z+3/4' 'y, -x+3/4, -z+3/4' '-y+1/4, -x+3/4, z+1/2' 'z, y+1/2, x+1/2' '-z+1/4, -y+3/4, x+1/2' '-z+1/4, y+1/2, -x+3/4' 'z, -y+3/4, -x+3/4' 'x+1/2, y, z+1/2' 'x+1/2, -y+1/4, -z+3/4' '-x+3/4, y, -z+3/4' '-x+3/4, -y+1/4, z+1/2' 'y+1/2, z, x+1/2' '-y+3/4, -z+1/4, x+1/2' 'y+1/2, -z+1/4, -x+3/4' '-y+3/4, z, -x+3/4' 'z+1/2, x, y+1/2' '-z+3/4, x, -y+3/4' '-z+3/4, -x+1/4, y+1/2' 'z+1/2, -x+1/4, -y+3/4' 'x+1/2, z, y+1/2' 'x+1/2, -z+1/4, -y+3/4' '-x+3/4, -z+1/4, y+1/2' '-x+3/4, z, -y+3/4' 'y+1/2, x, z+1/2' '-y+3/4, x, -z+3/4' 'y+1/2, -x+1/4, -z+3/4' '-y+3/4, -x+1/4, z+1/2' 'z+1/2, y, x+1/2' '-z+3/4, -y+1/4, x+1/2' '-z+3/4, y, -x+3/4' 'z+1/2, -y+1/4, -x+3/4' 'x+1/2, y+1/2, z' 'x+1/2, -y+3/4, -z+1/4' '-x+3/4, y+1/2, -z+1/4' '-x+3/4, -y+3/4, z' 'y+1/2, z+1/2, x' '-y+3/4, -z+3/4, x' 'y+1/2, -z+3/4, -x+1/4' '-y+3/4, z+1/2, -x+1/4' 'z+1/2, x+1/2, y' '-z+3/4, x+1/2, -y+1/4' '-z+3/4, -x+3/4, y' 'z+1/2, -x+3/4, -y+1/4' 'x+1/2, z+1/2, y' 'x+1/2, -z+3/4, -y+1/4' '-x+3/4, -z+3/4, y' '-x+3/4, z+1/2, -y+1/4' 'y+1/2, x+1/2, z' '-y+3/4, x+1/2, -z+1/4' 'y+1/2, -x+3/4, -z+1/4' '-y+3/4, -x+3/4, z' 'z+1/2, y+1/2, x' '-z+3/4, -y+3/4, x' '-z+3/4, y+1/2, -x+1/4' 'z+1/2, -y+3/4, -x+1/4' '-x, -y, -z' '-x, y-1/4, z-1/4' 'x-1/4, -y, z-1/4' 'x-1/4, y-1/4, -z' '-y, -z, -x' 'y-1/4, z-1/4, -x' '-y, z-1/4, x-1/4' 'y-1/4, -z, x-1/4' '-z, -x, -y' 'z-1/4, -x, y-1/4' 'z-1/4, x-1/4, -y' '-z, x-1/4, y-1/4' '-x, -z, -y' '-x, z-1/4, y-1/4' 'x-1/4, z-1/4, -y' 'x-1/4, -z, y-1/4' '-y, -x, -z' 'y-1/4, -x, z-1/4' '-y, x-1/4, z-1/4' 'y-1/4, x-1/4, -z' '-z, -y, -x' 'z-1/4, y-1/4, -x' 'z-1/4, -y, x-1/4' '-z, y-1/4, x-1/4' '-x, -y+1/2, -z+1/2' '-x, y+1/4, z+1/4' 'x-1/4, -y+1/2, z+1/4' 'x-1/4, y+1/4, -z+1/2' '-y, -z+1/2, -x+1/2' 'y-1/4, z+1/4, -x+1/2' '-y, z+1/4, x+1/4' 'y-1/4, -z+1/2, x+1/4' '-z, -x+1/2, -y+1/2' 'z-1/4, -x+1/2, y+1/4' 'z-1/4, x+1/4, -y+1/2' '-z, x+1/4, y+1/4' '-x, -z+1/2, -y+1/2' '-x, z+1/4, y+1/4' 'x-1/4, z+1/4, -y+1/2' 'x-1/4, -z+1/2, y+1/4' '-y, -x+1/2, -z+1/2' 'y-1/4, -x+1/2, z+1/4' '-y, x+1/4, z+1/4' 'y-1/4, x+1/4, -z+1/2' '-z, -y+1/2, -x+1/2' 'z-1/4, y+1/4, -x+1/2' 'z-1/4, -y+1/2, x+1/4' '-z, y+1/4, x+1/4' '-x+1/2, -y, -z+1/2' '-x+1/2, y-1/4, z+1/4' 'x+1/4, -y, z+1/4' 'x+1/4, y-1/4, -z+1/2' '-y+1/2, -z, -x+1/2' 'y+1/4, z-1/4, -x+1/2' '-y+1/2, z-1/4, x+1/4' 'y+1/4, -z, x+1/4' '-z+1/2, -x, -y+1/2' 'z+1/4, -x, y+1/4' 'z+1/4, x-1/4, -y+1/2' '-z+1/2, x-1/4, y+1/4' '-x+1/2, -z, -y+1/2' '-x+1/2, z-1/4, y+1/4' 'x+1/4, z-1/4, -y+1/2' 'x+1/4, -z, y+1/4' '-y+1/2, -x, -z+1/2' 'y+1/4, -x, z+1/4' '-y+1/2, x-1/4, z+1/4' 'y+1/4, x-1/4, -z+1/2' '-z+1/2, -y, -x+1/2' 'z+1/4, y-1/4, -x+1/2' 'z+1/4, -y, x+1/4' '-z+1/2, y-1/4, x+1/4' '-x+1/2, -y+1/2, -z' '-x+1/2, y+1/4, z-1/4' 'x+1/4, -y+1/2, z-1/4' 'x+1/4, y+1/4, -z' '-y+1/2, -z+1/2, -x' 'y+1/4, z+1/4, -x' '-y+1/2, z+1/4, x-1/4' 'y+1/4, -z+1/2, x-1/4' '-z+1/2, -x+1/2, -y' 'z+1/4, -x+1/2, y-1/4' 'z+1/4, x+1/4, -y' '-z+1/2, x+1/4, y-1/4' '-x+1/2, -z+1/2, -y' '-x+1/2, z+1/4, y-1/4' 'x+1/4, z+1/4, -y' 'x+1/4, -z+1/2, y-1/4' '-y+1/2, -x+1/2, -z' 'y+1/4, -x+1/2, z-1/4' '-y+1/2, x+1/4, z-1/4' 'y+1/4, x+1/4, -z' '-z+1/2, -y+1/2, -x' 'z+1/4, y+1/4, -x' 'z+1/4, -y+1/2, x-1/4' '-z+1/2, y+1/4, x-1/4' _cell_length_a 10.20109(9) _cell_length_b 10.20109(9) _cell_length_c 10.20109(9) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 1061.548(16) _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 octahedron _exptl_crystal_colour black _exptl_crystal_size_max 0.1 _exptl_crystal_size_mid 0.1 _exptl_crystal_size_min 0.1 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 8.952 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2432 _exptl_absorpt_coefficient_mu 63.234 _exptl_absorpt_correction_type integration _exptl_absorpt_correction_T_min 0.0229 _exptl_absorpt_correction_T_max 0.0772 _exptl_absorpt_process_details ; absorption correction with STOE X-SHAPE 2.03. ; _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 'plane graphite' _diffrn_measurement_device '2-circle goniometer' _diffrn_measurement_device_type 'STOE IPDS 2' _diffrn_detector 'image plate (34 cm diameter)' _diffrn_detector_type STOE _diffrn_detector_area_resol_mean 6.67 _diffrn_measurement_method 'rotation method' _diffrn_standards_number 0 _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% 0 _diffrn_reflns_number 961 _diffrn_reflns_av_R_equivalents 0.0609 _diffrn_reflns_av_sigmaI/netI 0.0308 _diffrn_reflns_limit_h_min -12 _diffrn_reflns_limit_h_max 12 _diffrn_reflns_limit_k_min -12 _diffrn_reflns_limit_k_max 12 _diffrn_reflns_limit_l_min 0 _diffrn_reflns_limit_l_max 12 _diffrn_reflns_theta_min 3.46 _diffrn_reflns_theta_max 25.70 _reflns_number_total 69 _reflns_number_gt 58 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'STOE X-AREA' _computing_cell_refinement 'STOE X-AREA' _computing_data_reduction 'STOE X-RED' _computing_structure_solution 'SHELXS-97 (Sheldrick, 1990)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'Diamond 2.1e' _computing_publication_material ? _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^)+(0.0195P)^2^+1.4429P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _refine_ls_extinction_method SHELXL _refine_ls_extinction_coef 0.00053(7) _refine_ls_extinction_expression Fc^*^=kFc[1+0.001xFc^2^\l^3^/sin(2\q)]^-1/4^ _refine_ls_number_reflns 69 _refine_ls_number_parameters 11 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0283 _refine_ls_R_factor_gt 0.0213 _refine_ls_wR_factor_ref 0.0506 _refine_ls_wR_factor_gt 0.0483 _refine_ls_goodness_of_fit_ref 1.429 _refine_ls_restrained_S_all 1.429 _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 Hg Hg 0.5000 0.5000 0.5000 0.0143(5) Uani 1 12 d S . . Ru Ru 0.0000 0.0000 0.0000 0.0092(7) Uani 1 12 d S . . O1 O 0.3170(7) 0.1250 0.1250 0.0136(15) Uani 1 4 d S . . O2 O 0.3750 0.3750 0.3750 0.015(4) Uani 1 24 d S . . 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 Hg 0.0143(5) 0.0143(5) 0.0143(5) -0.00050(19) -0.00050(19) -0.00050(19) Ru 0.0092(7) 0.0092(7) 0.0092(7) -0.0004(4) -0.0004(4) -0.0004(4) O1 0.016(4) 0.012(2) 0.012(2) 0.002(3) 0.000 0.000 O2 0.015(4) 0.015(4) 0.015(4) 0.000 0.000 0.000 _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 Hg O2 2.2086 97_666 ? Hg O2 2.2086 . ? Hg O1 2.596(5) 25 ? Hg O1 2.596(5) 57 ? Hg O1 2.596(5) 77 ? Hg O1 2.596(5) 121_655 ? Hg O1 2.596(5) 173_556 ? Hg O1 2.596(5) 153_565 ? Ru O1 1.928(3) 11 ? Ru O1 1.928(3) 3 ? Ru O1 1.928(3) 7 ? Ru O1 1.928(3) 107 ? Ru O1 1.928(3) 103 ? Ru O1 1.928(3) 99 ? O1 Ru 1.928(3) 4 ? O1 Ru 1.928(3) 3 ? O1 Hg 2.596(5) 26 ? O1 Hg 2.596(5) 25_544 ? O2 Hg 2.2086 76 ? O2 Hg 2.2086 26 ? O2 Hg 2.2086 51 ? 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 O2 Hg O2 180.0 97_666 . ? O2 Hg O1 81.26(11) 97_666 25 ? O2 Hg O1 98.74(11) . 25 ? O2 Hg O1 81.26(11) 97_666 57 ? O2 Hg O1 98.74(11) . 57 ? O1 Hg O1 117.73(6) 25 57 ? O2 Hg O1 81.26(11) 97_666 77 ? O2 Hg O1 98.74(11) . 77 ? O1 Hg O1 117.73(6) 25 77 ? O1 Hg O1 117.73(6) 57 77 ? O2 Hg O1 98.74(11) 97_666 121_655 ? O2 Hg O1 81.26(11) . 121_655 ? O1 Hg O1 180.0 25 121_655 ? O1 Hg O1 62.27(6) 57 121_655 ? O1 Hg O1 62.27(6) 77 121_655 ? O2 Hg O1 98.74(11) 97_666 173_556 ? O2 Hg O1 81.26(11) . 173_556 ? O1 Hg O1 62.27(6) 25 173_556 ? O1 Hg O1 62.27(6) 57 173_556 ? O1 Hg O1 180.0 77 173_556 ? O1 Hg O1 117.73(6) 121_655 173_556 ? O2 Hg O1 98.74(11) 97_666 153_565 ? O2 Hg O1 81.26(11) . 153_565 ? O1 Hg O1 62.27(6) 25 153_565 ? O1 Hg O1 180.0 57 153_565 ? O1 Hg O1 62.27(6) 77 153_565 ? O1 Hg O1 117.73(6) 121_655 153_565 ? O1 Hg O1 117.73(6) 173_556 153_565 ? O1 Ru O1 91.8(3) 11 3 ? O1 Ru O1 91.8(3) 11 7 ? O1 Ru O1 91.8(3) 3 7 ? O1 Ru O1 180.0 11 107 ? O1 Ru O1 88.2(3) 3 107 ? O1 Ru O1 88.2(3) 7 107 ? O1 Ru O1 88.2(3) 11 103 ? O1 Ru O1 88.2(3) 3 103 ? O1 Ru O1 180.0 7 103 ? O1 Ru O1 91.8(3) 107 103 ? O1 Ru O1 88.2(3) 11 99 ? O1 Ru O1 180.0 3 99 ? O1 Ru O1 88.2(3) 7 99 ? O1 Ru O1 91.8(3) 107 99 ? O1 Ru O1 91.8(3) 103 99 ? Ru O1 Ru 138.5(4) 4 3 ? Ru O1 Hg 104.76(11) 4 26 ? Ru O1 Hg 104.76(11) 3 26 ? Ru O1 Hg 104.76(11) 4 25_544 ? Ru O1 Hg 104.76(11) 3 25_544 ? Hg O1 Hg 88.0(2) 26 25_544 ? Hg O2 Hg 109.5 . 76 ? Hg O2 Hg 109.5 . 26 ? Hg O2 Hg 109.5 76 26 ? Hg O2 Hg 109.5 . 51 ? Hg O2 Hg 109.5 76 51 ? Hg O2 Hg 109.5 26 51 ? _diffrn_measured_fraction_theta_max 1.000 _diffrn_reflns_theta_full 25.70 _diffrn_measured_fraction_theta_full 1.000 _refine_diff_density_max 0.639 _refine_diff_density_min -0.965 _refine_diff_density_rms 0.271