#------------------------------------------------------------------------------
#$Date: 2018-09-27 07:13:35 +0300 (Thu, 27 Sep 2018) $
#$Revision: 211196 $
#$URL: file:///home/coder/svn-repositories/cod/cif/1/54/02/1540220.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_1540220
loop_
_publ_author_name
'Land, C.C.'
'Peterson, D.E.'
'Roof, R.B.'
_publ_section_title
;
 Phase investigations of the Pu - Pt, Pu - Rh, and Pu - Pt - Rh systems
;
_journal_name_full               'Journal of Nuclear Materials'
_journal_page_first              262
_journal_page_last               273
_journal_volume                  75
_journal_year                    1978
_chemical_formula_sum            'Pt4 Pu'
_space_group_IT_number           65
_symmetry_space_group_name_Hall  '-C 2 2'
_symmetry_space_group_name_H-M   'C m m m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            2
_cell_length_a                   5.258
_cell_length_b                   8.759
_cell_length_c                   4.563
_cell_volume                     210.148
_citation_journal_id_ASTM        JNUMAM
_cod_data_source_file            Land_JNUMAM_1978_1292.cif
_cod_data_source_block           Pt4Pu1
_cod_original_cell_volume        210.1481
_cod_original_formula_sum        'Pt4 Pu1'
_cod_database_code               1540220
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
-x+1/2,-y+1/2,z
x+1/2,-y+1/2,-z
-x+1/2,y+1/2,-z
-x+1/2,-y+1/2,-z
x+1/2,y+1/2,-z
-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
Pt1 Pt 0.25 0.25 0.5 1 0.0
Pu1 Pu 0 0 0 1 0.0
Pt2 Pt 0 0.333 0 1 0.0
