#------------------------------------------------------------------------------ #$Date: 2015-10-10 07:28:16 +0300 (Sat, 10 Oct 2015) $ #$Revision: 164948 $ #$URL: file:///home/coder/svn-repositories/cod/cif/1/53/70/1537007.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_1537007 loop_ _publ_author_name 'Reiser, S.' 'Brunklaus, G.' 'Hong, J.H.' 'Chan, J.C.C.' 'Pfitzner, A.' 'Eckert, H.' _publ_section_title ; (Cu I)3 P4 S4: preparation, structural and NMR spectroscopic characterization of a copper(I) halide adduct with beta- (P4 S4) ; _journal_name_full 'Chemistry - A European Journal' _journal_page_first 4228 _journal_page_last 4233 _journal_volume 8 _journal_year 2002 _chemical_formula_sum 'Cu3 I3 P4 S4' _chemical_name_systematic '(Cu I)3 (P4 S4)' _space_group_IT_number 185 _symmetry_space_group_name_Hall 'P 6c -2' _symmetry_space_group_name_H-M 'P 63 c m' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 120 _cell_formula_units_Z 6 _cell_length_a 19.082 _cell_length_b 19.082 _cell_length_c 6.691 _cell_volume 2109.937 _citation_journal_id_ASTM CEUJED _cod_data_source_file Reiser_CEUJED_2002_674.cif _cod_data_source_block Cu3I3P4S4 _cod_database_code 1537007 loop_ _symmetry_equiv_pos_as_xyz x,y,z x-y,x,z+1/2 -y,x-y,z -x,-y,z+1/2 -x+y,-x,z y,-x+y,z+1/2 y,x,z -x+y,y,z+1/2 -x,-x+y,z -y,-x,z+1/2 x-y,-y,z x,x-y,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 P1 P 0.33631 0.42757 0.0725 1 0.0 I2 I-1 0.1986 0.53194 0.08692 1 0.0 I1 I-1 0.13279 0.13279 0.70708 1 0.0 Cu1 Cu+1 0.12585 0.12585 0.3159 1 0.0 S3 S 0.41056 0.41056 -0.1338 1 0.0 S1 S 0.30521 0.30521 0.4649 1 0.0 P3 P 0.40082 0.40082 0.3173 1 0.0 S2 S 0.22096 0.32404 0.064 1 0.0 Cu2 Cu+1 0.3332 0.53916 -0.0155 1 0.0 P2 P 0.23724 0.23724 0.2182 1 0.0