#------------------------------------------------------------------------------ #$Date: 2015-09-28 14:29:13 +0100 (Mon, 28 Sep 2015) $ #$Revision: 158715 $ #$URL: svn://www.crystallography.net/cod/cif/1/53/27/1532738.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_1532738 loop_ _publ_author_name 'Brisi, C.' 'Rolando, P.' _publ_section_title ; Preparazione e caratteristiche cristallografiche del composto K3 Zn2 F7 ; _journal_name_full 'Ricerca Scientifica' _journal_page_first 48 _journal_page_last 50 _journal_volume 36 _journal_year 1966 _chemical_formula_sum 'F7 K3 Zn2' _chemical_name_systematic 'K3 Zn2 F7' _space_group_IT_number 139 _symmetry_space_group_name_Hall '-I 4 2' _symmetry_space_group_name_H-M 'I 4/m m m' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_formula_units_Z 2 _cell_length_a 4.063 _cell_length_b 4.063 _cell_length_c 21.22 _cell_volume 350.299 _citation_journal_id_ASTM RISCAZ _cod_data_source_file Brisi_RISCAZ_1966_1504.cif _cod_data_source_block F7K3Zn2 _cod_original_cell_volume 350.2991 _cod_database_code 1532738 loop_ _symmetry_equiv_pos_as_xyz x,y,z -y,x,z -x,-y,z y,-x,z x,-y,-z y,x,-z -x,y,-z -y,-x,-z -x,-y,-z y,-x,-z x,y,-z -y,x,-z -x,y,z -y,-x,z x,-y,z y,x,z 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,-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,-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,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 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 Zn1 Zn+2 0 0 0.094 1 0.0 K1 K+1 0 0 0.5 1 0.0 F1 F-1 0 0 0 1 0.0 F3 F-1 0 0 0.188 1 0.0 K2 K+1 0 0 0.312 1 0.0 F2 F-1 0 0.5 0.094 1 0.0