#------------------------------------------------------------------------------
#$Date: 2016-02-13 21:28:24 +0200 (Sat, 13 Feb 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/1/52/14/1521471.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_1521471
loop_
_publ_author_name
'Kuz'ma, Yu.B.'
'Chikhrii, S.I.'
'Budnyk, S.L.'
_publ_section_title
;
 Yb - Ni - P system
;
_journal_name_full               'Journal of Alloys Compd.'
_journal_page_first              190
_journal_page_last               194
_journal_volume                  298
_journal_year                    2000
_chemical_formula_sum            'Ni4 P2 Yb'
_chemical_name_systematic        'Yb Ni4 P2'
_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                   7.0523
_cell_length_b                   7.0523
_cell_length_c                   3.5879
_cell_volume                     178.444
_citation_journal_id_ASTM        JALCEU
_cod_data_source_file            Kuzma_JALCEU_2000_1277.cif
_cod_data_source_block           Ni4P2Yb1
_cod_original_formula_sum        'Ni4 P2 Yb1'
_cod_database_code               1521471
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
Ni1 Ni 0.3367 0.0867 0 1 0.0
P1 P 0.2126 0.7874 0 1 0.0
Yb1 Yb 0 0 0.5 1 0.0
