#------------------------------------------------------------------------------
#$Date: 2016-02-13 20:28:24 +0100 (Sat 13 de Feb de 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/8/10/36/8103600.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_8103600
loop_
_publ_author_name
'Voellenkle, H.'
_publ_section_title
;
 Verfeinerung der Kristallstrukturen von Li2 Si O3 und Li2 Ge O3
;
_journal_name_full
'Zeitschrift fuer Kristallographie (149,1979-)'
_journal_page_first              77
_journal_page_last               81
_journal_volume                  154
_journal_year                    1981
_chemical_formula_sum            'Ge Li2 O3'
_chemical_name_systematic        'Li2 (Ge O3)'
_space_group_IT_number           36
_symmetry_space_group_name_Hall  'C 2c -2'
_symmetry_space_group_name_H-M   'C m c 21'
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_formula_units_Z            4
_cell_length_a                   9.634
_cell_length_b                   5.481
_cell_length_c                   4.843
_cell_volume                     255.730
_citation_journal_id_ASTM        ZEKRDZ
_cod_data_source_file            Voellenkle_ZEKRDZ_1981_320.cif
_cod_data_source_block           Ge1Li2O3
_cod_original_cell_volume        255.7295
_cod_original_formula_sum        'Ge1 Li2 O3'
_cod_database_code               8103600
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
Ge1 Ge+4 0 0.1782 0.5 1 0.0
O1 O-2 0 0.1315 0.8703 1 0.0
Li1 Li+1 0.1758 0.344 0.0153 1 0.0
O2 O-2 0.1522 0.3173 0.4086 1 0.0
