#------------------------------------------------------------------------------
#$Date: 2016-02-14 15:26:36 +0100 (dom 14 de feb de 2016) $
#$Revision: 176435 $
#$URL: svn://www.crystallography.net/cod/cif/1/51/07/1510720.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_1510720
loop_
_publ_author_name
'Nowotny, H.'
'Rogl, P.'
'Benesovsky, F.'
_publ_section_title
;
 Ueber einige Komplexboride mit Platinmetallen
;
_journal_name_full               'Monatshefte fuer Chemie (-108,1977)'
_journal_page_first              965
_journal_page_last               989
_journal_volume                  103
_journal_year                    1972
_chemical_formula_sum            'B2 Ir Mo2'
_chemical_name_systematic        'Mo2 Ir B2'
_space_group_IT_number           58
_symmetry_space_group_name_Hall  '-P 2 2n'
_symmetry_space_group_name_H-M   'P n n m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   9.422
_cell_length_b                   7.356
_cell_length_c                   3.231
_cell_volume                     223.935
_citation_journal_id_ASTM        MOCHAP
_cod_data_source_file            boron_205.cif
_cod_data_source_block           B2Ir1Mo2
_cod_original_cell_volume        223.9349
_cod_original_formula_sum        'B2 Ir1 Mo2'
_cod_database_code               1510720
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z
x+1/2,-y+1/2,-z+1/2
-x+1/2,y+1/2,-z+1/2
-x,-y,-z
x,y,-z
-x-1/2,y-1/2,z-1/2
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
Mo2 Mo 0.6397 0.0703 0 1 0.0
Mo1 Mo 0.3676 0.3121 0 1 0.0
B2 B 0.2282 0.622 0 1 0.0
Ir1 Ir 0.1087 0.122 0 1 0.0
B1 B 0.0353 0.6161 0 1 0.0
