#------------------------------------------------------------------------------
#$Date: 2018-09-27 07:13:35 +0300 (Thu, 27 Sep 2018) $
#$Revision: 211196 $
#$URL: file:///home/coder/svn-repositories/cod/cif/1/53/43/1534323.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_1534323
loop_
_publ_author_name
'Bronger, W.'
'Guenther, O.'
_publ_section_title
;
 Darstellung und Struktur von K2 Pt S2 und Rb2 Pt S2
;
_journal_name_full               'Journal of the Less-Common Metals'
_journal_page_first              73
_journal_page_last               79
_journal_volume                  27
_journal_year                    1972
_chemical_formula_sum            'K2 Pt S2'
_space_group_IT_number           71
_symmetry_space_group_name_Hall  '-I 2 2'
_symmetry_space_group_name_H-M   'I m m m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            2
_cell_length_a                   9.37
_cell_length_b                   7.08
_cell_length_c                   3.59
_cell_volume                     238.159
_citation_journal_id_ASTM        JCOMAH
_cod_data_source_file            Bronger_JCOMAH_1972_1197.cif
_cod_data_source_block           K2Pt1S2
_cod_original_cell_volume        238.1591
_cod_original_formula_sum        'K2 Pt1 S2'
_cod_database_code               1534323
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z
x,-y,-z
-x,y,-z
-x,-y,-z
x,y,-z
-x,y,z
x,-y,z
x+1/2,y+1/2,z+1/2
-x+1/2,-y+1/2,z+1/2
x+1/2,-y+1/2,-z+1/2
-x+1/2,y+1/2,-z+1/2
-x+1/2,-y+1/2,-z+1/2
x+1/2,y+1/2,-z+1/2
-x+1/2,y+1/2,z+1/2
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
K1 K+1 0.192 0.5 0 1 0.0
Pt1 Pt+2 0 0 0 1 0.0
S1 S-2 0 0.216 0.5 1 0.0
