#------------------------------------------------------------------------------
#$Date: 2018-09-27 06:13:35 +0200 (jue 27 de sep de 2018) $
#$Revision: 211196 $
#$URL: svn://www.crystallography.net/cod/cif/1/52/72/1527241.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_1527241
loop_
_publ_author_name
'Cirafici, S.'
'Palenzona, A.'
'Manfrinetti, P.'
_publ_section_title
;
 The Th-Sn phase diagram
;
_journal_name_full               'Journal of the Less-Common Metals'
_journal_page_first              49
_journal_page_last               56
_journal_volume                  90
_journal_year                    1983
_chemical_formula_sum            'Sn2 Th'
_space_group_IT_number           63
_symmetry_space_group_name_Hall  '-C 2c 2'
_symmetry_space_group_name_H-M   'C m c m'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   4.463
_cell_length_b                   17.062
_cell_length_c                   4.379
_cell_volume                     333.451
_citation_journal_id_ASTM        JCOMAH
_cod_data_source_file            Cirafici_JCOMAH_1983_61.cif
_cod_data_source_block           Sn2Th1
_cod_original_cell_volume        333.4508
_cod_original_formula_sum        'Sn2 Th1'
_cod_database_code               1527241
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x,-y,z+1/2
x,-y,-z
-x,y,-z+1/2
-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
-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
Sn2 Sn 0 0.4401 0.25 1 0.0
Sn1 Sn 0 0.7492 0.25 1 0.0
Th1 Th 0 0.1034 0.25 1 0.0
