#------------------------------------------------------------------------------ #$Date: 2018-09-27 07:13:35 +0300 (Thu, 27 Sep 2018) $ #$Revision: 211196 $ #$URL: file:///home/coder/svn-repositories/cod/cif/2/10/61/2106133.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_2106133 loop_ _publ_author_name 'Arnberg, L.' _publ_section_title ; The structures of the gamma-phases in the Pd-Cd and Pt-Cd systems ; _journal_name_full 'Acta Crystallographica B (24,1968-38,1982)' _journal_page_first 527 _journal_page_last 532 _journal_volume 36 _journal_year 1980 _chemical_formula_sum 'Cd43 Pd8' _space_group_IT_number 215 _symmetry_space_group_name_Hall 'P -4 2 3' _symmetry_space_group_name_H-M 'P -4 3 m' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_formula_units_Z 1 _cell_length_a 9.9415 _cell_length_b 9.9415 _cell_length_c 9.9415 _cell_volume 982.552 _citation_journal_id_ASTM ACBCAR _cod_data_source_file Arnberg_ACBCAR_1980_704.cif _cod_data_source_block Cd43Pd8 _cod_original_cell_volume 982.5524 _cod_database_code 2106133 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 z,x,y x,-z,-y -z,-x,y -x,z,-y z,-x,-y -x,-z,y -z,x,-y x,z,y y,z,x y,-z,-x -z,-y,x -y,z,-x z,y,x -y,-z,x -z,y,-x z,-y,-x 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 Pd2 Pd 0.3292 0.3292 0.3292 1 0.0 Cd1 Cd 0.1048 0.1048 0.1048 0.75 0.0 Cd2 Cd 0.6073 0.6073 0.6073 1 0.0 Cd3 Cd 0.3493 0 0 1 0.0 Cd5 Cd 0.3038 0.3038 0.04474 1 0.0 Cd4 Cd 0.8556 0.5 0.5 1 0.0 Cd6 Cd 0.8076 0.8076 0.5448 1 0.0 Pd1 Pd 0.8266 0.8266 0.8266 1 0.0