#------------------------------------------------------------------------------
#$Date: 2015-10-11 16:12:58 +0300 (Sun, 11 Oct 2015) $
#$Revision: 165723 $
#$URL: svn://www.crystallography.net/cod/cif/8/10/42/8104220.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_8104220
loop_
_publ_author_name
'Kihara, K.'
'Sudo, T.'
_publ_section_title
;
 The structure of alpha-type cesium antimony nonachloride, Cs3 Sb2 Cl9
;
_journal_name_full
;
Zeitschrift fuer Kristallographie, Kristallgeometrie, Kristallphysik, 
Kristallchemie (-144,1977)
;
_journal_page_first              142
_journal_page_last               144
_journal_volume                  134
_journal_year                    1971
_chemical_formula_sum            'Cl9 Cs3 Sb2'
_chemical_name_systematic        'Cs3 (Sb2 Cl9)'
_space_group_IT_number           150
_symmetry_space_group_name_Hall  'P 3 2"'
_symmetry_space_group_name_H-M   'P 3 2 1'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                120
_cell_formula_units_Z            1
_cell_length_a                   7.633
_cell_length_b                   7.633
_cell_length_c                   9.345
_cell_volume                     471.520
_citation_journal_id_ASTM        ZEKGAX
_cod_data_source_file            Kihara_ZEKGAX_1971_1042.cif
_cod_data_source_block           Cl9Cs3Sb2
_cod_original_cell_volume        471.5204
_cod_database_code               8104220
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-y,x-y,z
-x+y,-x,z
y,x,-z
-x,-x+y,-z
x-y,-y,-z
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
Cs2 Cs+1 0.3333 0.6667 0.3241 1 0.0
Cl2 Cl-1 0.3569 0.2053 0.3219 1 0.0
Cl1 Cl-1 0.4705 0 0 1 0.0
Cs1 Cs+1 0 0 0 1 0.0
Sb1 Sb+3 0.3333 0.6667 0.8139 1 0.0
