#------------------------------------------------------------------------------ #$Date: 2015-07-12 17:19:57 +0300 (Sun, 12 Jul 2015) $ #$Revision: 146746 $ #$URL: file:///home/coder/svn-repositories/cod/cif/1/52/57/1525711.cif $ #------------------------------------------------------------------------------ # # This file is available in the Crystallography Open Database (COD), # http://www.crystallography.net/ # # All data on this site have been placed in the public domain by the # contributors. # data_1525711 loop_ _publ_author_name 'Bramnik, K.G.' 'Ehrenberg, H.' 'Fuess, H.' _publ_section_title ; Preparation, crystal structure, and magnetic studies of a new Sr7 Re4 O19 double oxide and its relation to the structure of Ba7 Ir6 O19 ; _journal_name_full 'Journal of Solid State Chemistry' _journal_page_first 45 _journal_page_last 49 _journal_volume 160 _journal_year 2001 _chemical_formula_sum 'O19 Re4 Sr7' _chemical_name_systematic 'Sr7 Re4 O19' _space_group_IT_number 12 _symmetry_space_group_name_Hall '-C 2y' _symmetry_space_group_name_H-M 'C 1 2/m 1' _cell_angle_alpha 90 _cell_angle_beta 98.3504 _cell_angle_gamma 90 _cell_formula_units_Z 2 _cell_length_a 13.6432 _cell_length_b 5.60509 _cell_length_c 10.37483 _cell_volume 784.966 _citation_journal_id_ASTM JSSCBI _cod_data_source_file Bramnik_JSSCBI_2001_1652.cif _cod_data_source_block O19Re4Sr7 _cod_original_cell_volume 784.9664 _cod_database_code 1525711 loop_ _symmetry_equiv_pos_as_xyz x,y,z -x,y,-z -x,-y,-z x,-y,z x+1/2,y+1/2,z -x+1/2,y+1/2,-z -x+1/2,-y+1/2,-z x+1/2,-y+1/2,z loop_ _atom_site_label _atom_site_type_symbol _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_occupancy _atom_site_U_iso_or_equiv Sr1 Sr+2 0.7923 0 0.4061 1 0.0 O7 O-2 0 0 0.5 1 0.0 Re1 Re+6 0.0354 0 0.319 1 0.0 O4 O-2 0.392 0 0.071 1 0.0 Sr2 Sr+2 0.5839 0 0.1588 1 0.0 O5 O-2 0.048 0 0.145 1 0.0 O1 O-2 0.624 0.752 0.376 1 0.0 O3 O-2 0.426 0.26 0.287 1 0.0 Sr4 Sr+2 0 0.5 0.5 1 0.0 O2 O-2 0.24 0.748 0.157 1 0.0 O6 O-2 0.69 0 0.61 1 0.0 Re2 Re+6 0.328 0 0.2164 1 0.0 Sr3 Sr+2 0.8593 0 0.047 1 0.0