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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/1/52/31/1523101.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_1523101
loop_
_publ_author_name
'Yarmolyuk, Ya.P.'
'Grin', Yu.'
_publ_section_title
;
 Intermetallic compounds R Ga2 Ni and R Ga4 Ni in (Y, Sm, Gd, Tb, Ho, Er,
 Tm, Yb, Lu) - Ga - Ni systems
;
_journal_name_full               'Izvestiya Akademii Nauk SSSR, Metally'
_journal_page_first              228
_journal_page_last               234
_journal_volume                  1981
_journal_year                    1981
_chemical_formula_sum            'Ga2 Ni Y'
_space_group_IT_number           63
_symmetry_space_group_name_Hall  '-C 2c 2'
_symmetry_space_group_name_H-M   'C m c m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   4.131
_cell_length_b                   10.05
_cell_length_c                   6.62
_cell_volume                     274.840
_citation_journal_id_ASTM        IZNMAQ
_cod_data_source_file            Yarmolyuk_IZNMAQ_1981_292.cif
_cod_data_source_block           Ga2Ni1Y1
_cod_original_cell_volume        274.8396
_cod_original_formula_sum        'Ga2 Ni1 Y1'
_cod_database_code               1523101
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z+1/2
x,-y,-z
-x,y,-z+1/2
-x,-y,-z
x,y,-z-1/2
-x,y,z
x,-y,z-1/2
x+1/2,y+1/2,z
-x+1/2,-y+1/2,z+1/2
x+1/2,-y+1/2,-z
-x+1/2,y+1/2,-z+1/2
-x+1/2,-y+1/2,-z
x+1/2,y+1/2,-z-1/2
-x+1/2,y+1/2,z
x+1/2,-y+1/2,z-1/2
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
Ga1 Ga 0 0.356 0.056 1 0.0
Ni1 Ni 0 0.791 0.25 1 0.0
Y1 Y 0 0.072 0.25 1 0.0
