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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/1/53/78/1537872.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_1537872
loop_
_publ_author_name
'Bozzolo, A.'
'Rey, J.'
'Laffitte, M.'
_publ_section_title
;
 Domaine de stabilite de la phase hexagonale dans le diagramme ternaire
 Ni-Co-Te a 500 C
;
_journal_name_full
;
Journal de Chimie Physique et de Physico-Chimie Biologique
;
_journal_page_first              655
_journal_page_last               661
_journal_volume                  67
_journal_year                    1970
_chemical_formula_sum            'Ni Te'
_space_group_IT_number           194
_symmetry_space_group_name_Hall  '-P 6c 2c'
_symmetry_space_group_name_H-M   'P 63/m m c'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                120
_cell_formula_units_Z            2
_cell_length_a                   3.964
_cell_length_b                   3.964
_cell_length_c                   5.351
_cell_volume                     72.817
_citation_journal_id_ASTM        JCPBAN
_cod_data_source_file            Bozzolo_JCPBAN_1970_1098.cif
_cod_data_source_block           Ni1Te1
_cod_original_cell_volume        72.81701
_cod_original_formula_sum        'Ni1 Te1'
_cod_database_code               1537872
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
x-y,x,z+1/2
-y,x-y,z
-x,-y,z+1/2
-x+y,-x,z
y,-x+y,z+1/2
-y,-x,-z+1/2
x-y,-y,-z
x,x-y,-z+1/2
y,x,-z
-x+y,y,-z+1/2
-x,-x+y,-z
-x,-y,-z
-x+y,-x,-z-1/2
y,-x+y,-z
x,y,-z-1/2
x-y,x,-z
-y,x-y,-z-1/2
y,x,z-1/2
-x+y,y,z
-x,-x+y,z-1/2
-y,-x,z
x-y,-y,z-1/2
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
Ni1 Ni 0 0 0 1 0.0
Te1 Te 0.3333 0.6667 0.25 1 0.0