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#$Date: 2016-02-13 20:28:24 +0100 (Sat 13 de Feb de 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/1/52/18/1521887.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_1521887
loop_
_publ_author_name
'Schinzer, C.'
'Demazeau, G.'
_publ_section_title
;
 Structure and properties of new perovskites La2 M Rh O6 (M = Mg,Zn)
;
_journal_name_full               'Journal of Materials Science'
_journal_page_first              251
_journal_page_last               256
_journal_volume                  34
_journal_year                    1999
_chemical_formula_sum            'La2 O6 Rh Zn'
_chemical_name_systematic        'La2 Zn (Rh O6)'
_space_group_IT_number           14
_symmetry_space_group_name_Hall  '-P 2yn'
_symmetry_space_group_name_H-M   'P 1 21/n 1'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            2
_cell_length_a                   5.584
_cell_length_b                   5.659
_cell_length_c                   7.914
_cell_volume                     250.081
_citation_journal_id_ASTM        JMTSAS
_cod_data_source_file            Schinzer_JMTSAS_1999_182.cif
_cod_data_source_block           La2O6Rh1Zn1
_cod_original_cell_volume        250.0813
_cod_original_sg_symbol_Hall     '-P 2ybc (x-z,y,z)'
_cod_original_formula_sum        'La2 O6 Rh1 Zn1'
_cod_database_code               1521887
loop_
_symmetry_equiv_pos_as_xyz
x,y,z
-x+1/2,y+1/2,-z+1/2
-x,-y,-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
O1 O-2 0.203 0.213 -0.0481 1 0.0
O2 O-2 0.295 0.697 -0.0395 1 0.0
Zn1 Zn+2 0.5 0 0 1 0.0
La1 La+3 0.512 0.545 0.249 1 0.0
Rh1 Rh+4 0 0.5 0 1 0.0
O3 O-2 0.4118 -0.0208 0.251 1 0.0
