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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/1/52/77/1527753.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_1527753
loop_
_publ_author_name
'Maletta, H.'
'Robinson, R.A.'
'Lawson, A.C.'
'Burlet, P.'
'Brueck, E.'
'Jirman, L.'
'Sechovsky, V.'
'Divis, M.'
'Havela, L.'
'Andreev, A.V.'
'Buschow, K.H.J.'
'de Boer, F.R.'
_publ_section_title
;
 On the magnetic structure of U Ni Ga
;
_journal_name_full               'Journal of Magnetism and Magnetic Materials'
_journal_page_first              21
_journal_page_last               22
_journal_volume                  104
_journal_year                    1992
_chemical_formula_sum            'Ga Ni U'
_space_group_IT_number           189
_symmetry_space_group_name_Hall  'P -6 -2'
_symmetry_space_group_name_H-M   'P -6 2 m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                120
_cell_formula_units_Z            3
_cell_length_a                   6.7012
_cell_length_b                   6.7012
_cell_length_c                   4.00878
_cell_volume                     155.901
_citation_journal_id_ASTM        JMMMDC
_cod_data_source_file            Maletta_JMMMDC_1992_519.cif
_cod_data_source_block           Ga1Ni1U1
_cod_original_cell_volume        155.9007
_cod_original_formula_sum        'Ga1 Ni1 U1'
_cod_database_code               1527753
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x+y,-x,-z
-y,x-y,z
x,y,-z
-x+y,-x,z
-y,x-y,-z
y,x,z
x-y,-y,-z
-x,-x+y,z
y,x,-z
x-y,-y,z
-x,-x+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
U1 U 0.57754 0 0.5 1 0.0
Ga1 Ga 0.24041 0 0 1 0.0
Ni2 Ni 0.3333 0.6667 0 1 0.0
Ni1 Ni 0 0 0.5 1 0.0
