#------------------------------------------------------------------------------
#$Date: 2016-02-13 20:28:24 +0100 (Sat 13 de Feb de 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/1/52/52/1525207.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_1525207
loop_
_publ_author_name
'Schaefer, W.'
'Will, G.'
'Schober, T.'
_publ_section_title
;
 Neutron and electron diffraction of the Fe Ti - D (H) - gamma-phase
;
_journal_name_full               'Materials Research Bulletin'
_journal_page_first              627
_journal_page_last               634
_journal_volume                  15
_journal_year                    1980
_chemical_formula_sum            'D2 Fe Ti'
_chemical_name_systematic        'Fe Ti D2'
_space_group_IT_number           10
_symmetry_space_group_name_Hall  '-P 2'
_symmetry_space_group_name_H-M   'P 1 1 2/m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                97.05
_cell_formula_units_Z            2
_cell_length_a                   4.708
_cell_length_b                   4.697
_cell_length_c                   2.835
_cell_volume                     62.218
_citation_journal_id_ASTM        MRBUAC
_cod_data_source_file            Schaefer_MRBUAC_1980_433.cif
_cod_data_source_block           D2Fe1Ti1
_cod_original_cell_volume        62.21772
_cod_original_sg_symbol_Hall     '-P 2y (z,x,y)'
_cod_original_formula_sum        'D2 Fe1 Ti1'
_cod_database_code               1525207
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z
-x,-y,-z
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
D1 D 0 0 0 1 0.0
Ti1 Ti 0.274 0.231 0.5 1 0.0
D2 D 0.5 0 0 1 0.0
D4 D 0 0.5 0.5 1 0.0
D3 D 0.5 0.5 0 1 0.0
Fe1 Fe 0.2 0.736 0 1 0.0
