#------------------------------------------------------------------------------ #$Date: 2016-02-13 14:50:18 +0200 (Sat, 13 Feb 2016) $ #$Revision: 176428 $ #$URL: file:///home/coder/svn-repositories/cod/cif/2/30/05/2300527.cif $ #------------------------------------------------------------------------------ # # This file is available in the Crystallography Open Database (COD), # http://www.crystallography.net/. The original data for this entry # were provided by IUCr Journals, http://journals.iucr.org/. # # The file may be used within the scientific community so long as # proper attribution is given to the journal article from which the # data were obtained. # data_2300527 loop_ _publ_author_name 'Nord, A.G.' _publ_section_title ; Use of the Rietveld technique for estimating cation distributions ; _journal_name_full 'Journal of Applied Crystallography' _journal_page_first 55 _journal_page_last 60 _journal_volume 17 _journal_year 1984 _chemical_formula_sum 'Fe0.9 O8 P2 Zn2.1' _chemical_name_systematic '(Zn.70 Fe.30)3 (P O4)2' _space_group_IT_number 14 _symmetry_space_group_name_Hall '-P 2yn' _symmetry_space_group_name_H-M 'P 1 21/n 1' _cell_angle_alpha 90 _cell_angle_beta 95.4 _cell_angle_gamma 90 _cell_formula_units_Z 2 _cell_length_a 7.558 _cell_length_b 8.536 _cell_length_c 5.042 _cell_volume 323.841 _citation_journal_id_ASTM JACGAR _cod_data_source_file Nord_JACGAR_1984_1102.cif _cod_data_source_block Fe0.9O8P2Zn2.1 _cod_original_cell_volume 323.8415 _cod_original_sg_symbol_Hall '-P 2ybc (x-z,y,z)' _cod_database_code 2300527 loop_ _symmetry_equiv_pos_as_xyz x,y,z -x+1/2,y+1/2,-z+1/2 -x,-y,-z x-1/2,-y-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 Fe2 Fe+2 0 0 0.5 0.724 0.0 O3 O-2 0.255 0.356 0.93 1 0.0 Zn1 Zn+2 0.619 0.137 0.072 0.912 0.0 Zn2 Zn+2 0 0 0.5 0.276 0.0 Fe1 Fe+2 0.619 0.137 0.072 0.088 0.0 O2 O-2 0.129 0.201 0.304 1 0.0 O1 O-2 0.05 0.13 0.824 1 0.0 O4 O-2 0.364 0.081 0.052 1 0.0 P1 P+5 0.201 0.191 0.026 1 0.0