#------------------------------------------------------------------------------
#$Date: 2018-09-27 07:13:35 +0300 (Thu, 27 Sep 2018) $
#$Revision: 211196 $
#$URL: file:///home/coder/svn-repositories/cod/cif/8/10/41/8104102.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_8104102
loop_
_publ_author_name
'Pani, M.'
'Merlo, F.'
'Fornasini, M.L.'
_publ_section_title
;
 Structure and transport properties of the R2 Co2 Al compounds (R= Pr, Nd,
 Sm, Gd, Tb, Dy, Ho, Er, Tm, Y)
;
_journal_name_full
'Zeitschrift fuer Kristallographie (149,1979-)'
_journal_page_first              415
_journal_page_last               419
_journal_volume                  217
_journal_year                    2002
_chemical_formula_sum            'Al Co2 Pr2'
_space_group_IT_number           15
_symmetry_space_group_name_Hall  '-C 2yc'
_symmetry_space_group_name_H-M   'C 1 2/c 1'
_cell_angle_alpha                90
_cell_angle_beta                 103.89
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   9.595
_cell_length_b                   5.609
_cell_length_c                   7.758
_cell_volume                     405.314
_citation_journal_id_ASTM        ZEKRDZ
_cod_data_source_file            Pani_ZEKRDZ_2002_680.cif
_cod_data_source_block           Al1Co2Pr2
_cod_original_cell_volume        405.3138
_cod_original_formula_sum        'Al1 Co2 Pr2'
_cod_database_code               8104102
loop_
_symmetry_equiv_pos_as_xyz
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
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
Co1 Co 0.13982 0.14124 0.00595 1 0.0
Pr1 Pr 0.35425 0.14594 0.35429 1 0.0
Al1 Al 0 0.1252 0.25 1 0.0
