#------------------------------------------------------------------------------ #$Date: 2016-02-13 21:28:24 +0200 (Sat, 13 Feb 2016) $ #$Revision: 176429 $ #$URL: file:///home/coder/svn-repositories/cod/cif/2/31/08/2310817.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_2310817 loop_ _publ_author_name 'Meller, F.' 'Fankuchen, I.' _publ_section_title ; The crystal structure of tin tetraiodide ; _journal_name_full 'Acta Crystallographica (1,1948-23,1967)' _journal_page_first 343 _journal_page_last 344 _journal_volume 8 _journal_year 1955 _chemical_formula_sum 'I4 Sn' _chemical_name_systematic 'Sn I4' _space_group_IT_number 205 _symmetry_space_group_name_Hall '-P 2ac 2ab 3' _symmetry_space_group_name_H-M 'P a -3' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_formula_units_Z 8 _cell_length_a 12.26 _cell_length_b 12.26 _cell_length_c 12.26 _cell_volume 1842.771 _citation_journal_id_ASTM ACCRA9 _cod_data_source_file Meller_ACCRA9_1955_526.cif _cod_data_source_block I4Sn1 _cod_original_formula_sum 'I4 Sn1' _cod_database_code 2310817 loop_ _symmetry_equiv_pos_as_xyz x,y,z -x+1/2,-y,z+1/2 x+1/2,-y+1/2,-z -x,y+1/2,-z+1/2 z,x,y -z+1/2,-x,y+1/2 z+1/2,-x+1/2,-y -z,x+1/2,-y+1/2 y,z,x y+1/2,-z+1/2,-x -y,z+1/2,-x+1/2 -y+1/2,-z,x+1/2 -x,-y,-z x-1/2,y,-z-1/2 -x-1/2,y-1/2,z x,-y-1/2,z-1/2 -z,-x,-y z-1/2,x,-y-1/2 -z-1/2,x-1/2,y z,-x-1/2,y-1/2 -y,-z,-x -y-1/2,z-1/2,x y,-z-1/2,x-1/2 y-1/2,z,-x-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 I1 I-1 0.252 0.252 0.252 1 0.0 I2 I-1 -0.002 -0.002 0.252 1 0.0 Sn1 Sn+4 0.125 0.125 0.125 1 0.0