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#$Date: 2016-02-13 21:28:24 +0200 (Sat, 13 Feb 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/1/53/11/1531165.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_1531165
loop_
_publ_author_name
'Brinks, H.W.'
'Yartys', V.A.'
'Hauback, B.C.'
'Ouladdiaf, B.'
'Fjellvag, H.'
_publ_section_title
;
 The magnetic structure of Tb Ni Si D1.78
;
_journal_name_full               'Journal of Alloys Compd.'
_journal_page_first              62
_journal_page_last               66
_journal_volume                  340
_journal_year                    2002
_chemical_formula_sum            'D1.78 Ni Si Tb'
_chemical_name_systematic        'Tb Ni Si D1.78'
_space_group_IT_number           62
_symmetry_space_group_name_Hall  '-P 2ac 2n'
_symmetry_space_group_name_H-M   'P n m a'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   7.9505
_cell_length_b                   4.02502
_cell_length_c                   6.9823
_cell_volume                     223.440
_citation_journal_id_ASTM        JALCEU
_cod_data_source_file            Brinks_JALCEU_2002_509.cif
_cod_data_source_block           D1.78Ni1Si1Tb1
_cod_original_cell_volume        223.44
_cod_original_formula_sum        'D1.78 Ni1 Si1 Tb1'
_cod_database_code               1531165
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x+1/2,-y,z+1/2
x+1/2,-y+1/2,-z+1/2
-x,y+1/2,-z
-x,-y,-z
x-1/2,y,-z-1/2
-x-1/2,y-1/2,z-1/2
x,-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
D1 D 0.9632 0.25 0.085 0.89 0.0
Tb1 Tb -0.0083 0.25 0.7515 1 0.0
Si1 Si 0.244 0.25 0.082 1 0.0
D2 D 0.5535 0.25 0.084 0.89 0.0
Ni1 Ni 0.2483 0.25 0.418 1 0.0
