#------------------------------------------------------------------------------ #$Date: 2015-10-09 16:43:36 +0300 (Fri, 09 Oct 2015) $ #$Revision: 162182 $ #$URL: file:///home/coder/svn-repositories/cod/cif/2/10/68/2106885.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_2106885 loop_ _publ_author_name 'Marsh, R.E.' 'Herbstein, F.H.' _publ_section_title ; Some additional changes in space groups of published crystal structures ; _journal_name_full 'Acta Crystallographica B (39,1983-)' _journal_page_first 280 _journal_page_last 287 _journal_volume 39 _journal_year 1983 _chemical_formula_sum 'F3 I Sn2' _chemical_name_systematic 'Sn2 I F3' _space_group_IT_number 63 _symmetry_space_group_name_Hall '-C 2c 2 (y,-x,z)' _symmetry_space_group_name_H-M 'C m c m (b,-a,c)' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_formula_units_Z 4 _cell_length_a 13.502 _cell_length_b 4.371 _cell_length_c 9.34 _cell_volume 551.221 _citation_journal_id_ASTM ASBSDK _cod_data_source_file Marsh_ASBSDK_1983_582.cif _cod_data_source_block F3I1Sn2 _cod_cif_authors_sg_H-M 'C c m m' _cod_chemical_formula_sum_orig 'F3 I1 Sn2' _cod_database_code 2106885 loop_ _symmetry_equiv_pos_as_xyz x,y,z -x,-y,z+1/2 -x,y,-z x,-y,-z+1/2 -x,-y,-z x,y,-z-1/2 x,-y,z -x,y,z-1/2 x+1/2,y+1/2,z -x+1/2,-y+1/2,z+1/2 -x+1/2,y+1/2,-z x+1/2,-y+1/2,-z+1/2 -x+1/2,-y+1/2,-z x+1/2,y+1/2,-z-1/2 x+1/2,-y+1/2,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 F1 F-1 0.2085 0 0.538 1 0.0 I1 I-1 0.0167 0 0.25 1 0.0 F2 F-1 0.2887 0 0.25 1 0.0 Sn1 Sn+2 0.362 0 0.4359 1 0.0