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#$Date: 2016-02-13 21:28:24 +0200 (Sat, 13 Feb 2016) $
#$Revision: 176429 $
#$URL: svn://www.crystallography.net/cod/cif/1/53/70/1537042.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_1537042
loop_
_publ_author_name
'Riou, A.'
'Gerault, Y.'
'Cudennec, Y.'
_publ_section_title
;
 Etude structurale de gamma-Cd (O H)2 ou Cd2 O (O H)2 (H2 O)
;
_journal_name_full               'Materials Research Bulletin'
_journal_page_first              987
_journal_page_last               996
_journal_volume                  25
_journal_year                    1990
_chemical_formula_sum            'Cd2 H4 O4'
_chemical_name_systematic        'Cd2 O (O H)2 (H2 O)'
_space_group_IT_number           8
_symmetry_space_group_name_Hall  'I -2y'
_symmetry_space_group_name_H-M   'I 1 m 1'
_cell_angle_alpha                90
_cell_angle_beta                 91.52
_cell_angle_gamma                90
_cell_formula_units_Z            2
_cell_length_a                   5.664
_cell_length_b                   10.223
_cell_length_c                   3.404
_cell_volume                     197.033
_citation_journal_id_ASTM        MRBUAC
_cod_data_source_file            Riou_MRBUAC_1990_1794.cif
_cod_data_source_block           H4Cd2O4
_cod_original_cell_volume        197.0327
_cod_original_sg_symbol_Hall     'C -2y (x,y,-x+z)'
_cod_original_formula_sum        'H4 Cd2 O4'
_cod_database_code               1537042
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
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
Cd1 Cd+2 0 0.15254 0 1 0.0
H3 H+1 0 0.332 0.5 1 0.0
H1 H+1 0 0.5 0.332 1 0.0
O1 O-2 0.115 0 0.489 1 0.0
O3 O-2 0.879 0.2796 0.495 1 0.0
H2 H+1 0.666 0 0.25 1 0.0
O2 O-2 0.687 0 0.942 1 0.0
