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#$Date: 2015-10-14 19:24:10 +0300 (Wed, 14 Oct 2015) $
#$Revision: 168954 $
#$URL: file:///home/coder/svn-repositories/cod/cif/1/53/98/1539873.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_1539873
loop_
_publ_author_name
'Bronger, W.'
'Auffermann, G.'
_publ_section_title
;
 Darstellung, Struktur und Phasenumwandlung von Rb2 Pd H4 und Cs2 Pd H4
;
_journal_name_full               'Journal of Alloys Compd.'
_journal_page_first              87
_journal_page_last               93
_journal_volume                  187
_journal_year                    1992
_chemical_formula_sum            'D4 Pd Rb2'
_chemical_name_systematic        'Pd Rb2 D4'
_space_group_IT_number           136
_symmetry_space_group_name_Hall  '-P 4n 2n'
_symmetry_space_group_name_H-M   'P 42/m n m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            2
_cell_length_a                   5.827
_cell_length_b                   5.827
_cell_length_c                   8.495
_cell_volume                     288.439
_citation_journal_id_ASTM        JALCEU
_cod_data_source_file            Bronger_JALCEU_1992_755.cif
_cod_data_source_block           D4Pd1Rb2
_cod_original_cell_volume        288.4386
_cod_chemical_formula_sum_orig   'D4 Pd1 Rb2'
_cod_database_code               1539873
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-y+1/2,x+1/2,z+1/2
-x,-y,z
y+1/2,-x+1/2,z+1/2
x+1/2,-y+1/2,-z+1/2
y,x,-z
-x+1/2,y+1/2,-z+1/2
-y,-x,-z
-x,-y,-z
y-1/2,-x-1/2,-z-1/2
x,y,-z
-y-1/2,x-1/2,-z-1/2
-x-1/2,y-1/2,z-1/2
-y,-x,z
x-1/2,-y-1/2,z-1/2
y,x,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
Pd1 Pd 0 0 0 1 0.0
D2 D 0.2023 0.2023 0 1 0.0
D1 D 0 0 0.1971 1 0.0
Rb1 Rb 0 0.5 0.25 1 0.0