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#$Date: 2018-09-27 07:13:35 +0300 (Thu, 27 Sep 2018) $
#$Revision: 211196 $
#$URL: file:///home/coder/svn-repositories/cod/cif/1/52/30/1523037.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_1523037
loop_
_publ_author_name
'Venturini, G.'
'Malaman, B.'
'Roques, B.'
_publ_section_title
;
 Evolution des coordinations dans les structures d'isotypes de U2 Co3 Si5:
 R2 T3 X5 (R= La, Y; T= Ru, Rh, Ir; X= Si, Ge, Sn)
;
_journal_name_full               'Journal of the Less-Common Metals'
_journal_page_first              51
_journal_page_last               66
_journal_volume                  152
_journal_year                    1989
_chemical_formula_sum            'La2 Rh3 Sn5'
_space_group_IT_number           72
_symmetry_space_group_name_Hall  '-I 2 2c'
_symmetry_space_group_name_H-M   'I b a m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   10.764
_cell_length_b                   12.912
_cell_length_c                   6.365
_cell_volume                     884.638
_citation_journal_id_ASTM        JCOMAH
_cod_data_source_file            Venturini_JCOMAH_1989_936.cif
_cod_data_source_block           La2Rh3Sn5
_cod_database_code               1523037
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z
x,-y,-z+1/2
-x,y,-z+1/2
-x,-y,-z
x,y,-z
-x,y,z-1/2
x,-y,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
-x+1/2,y+1/2,-z+1
-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
x+1/2,-y+1/2,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
Sn1 Sn 0 0 0.25 1 0.0
La1 La 0.2707 0.357 0 1 0.0
Sn2 Sn 0 0.2785 0.25 1 0.0
Rh2 Rh 0.1036 0.1411 0 1 0.0
Rh1 Rh 0.5 0 0.25 1 0.0
Sn3 Sn 0.3319 0.0877 0 1 0.0
