#------------------------------------------------------------------------------ #$Date: 2015-10-10 06:36:48 +0300 (Sat, 10 Oct 2015) $ #$Revision: 164733 $ #$URL: file:///home/coder/svn-repositories/cod/cif/1/53/68/1536846.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_1536846 loop_ _publ_author_name 'Rastsvetaeva, R.K.' 'Tamazyan, R.A.' 'Sokolova, E.V.' 'Belakovskii, D.I.' _publ_section_title ; Crystal structures of two modifications of natural Ba, Mn-titanium silicate. ; _journal_name_full Kristallografiya _journal_page_first 354 _journal_page_last 360 _journal_volume 36 _journal_year 1991 _chemical_formula_sum 'Ba H2 Mn2 O10 Si2 Ti' _chemical_name_systematic 'Ba Mn2 (Ti O) (Si2 O7) (O H)2' _space_group_IT_number 11 _symmetry_space_group_name_Hall '-P 2yb' _symmetry_space_group_name_H-M 'P 1 21/m 1' _cell_angle_alpha 90 _cell_angle_beta 119.8 _cell_angle_gamma 90 _cell_formula_units_Z 2 _cell_length_a 5.361 _cell_length_b 6.906 _cell_length_c 12.556 _cell_volume 403.391 _citation_journal_id_ASTM KRISAJ _cod_data_source_file Rastsvetaeva_KRISAJ_1991_1117.cif _cod_data_source_block H2Ba1Mn2O10Si2Ti1 _cod_original_cell_volume 403.3908 _cod_chemical_formula_sum_orig 'H2 Ba1 Mn2 O10 Si2 Ti1' _cod_database_code 1536846 loop_ _symmetry_equiv_pos_as_xyz x,y,z -x,y+1/2,-z -x,-y,-z x,-y-1/2,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 Mn2 Mn+2 0 0 0 1 0.0 Ba1 Ba+2 0.2896 0.25 0.5343 1 0.0 Mn1 Mn+2 0.5081 0.25 0.0092 1 0.0 O2 O-2 0.746 0.25 0.919 1 0.0 O7 O-2 0.28 0.05 0.316 1 0.0 O4 O-2 0.316 0.25 0.122 1 0.0 Ti1 Ti+4 0.5008 0.25 0.2884 1 0.0 O6 O-2 0.795 0.051 0.314 1 0.0 Si1 Si+4 0.042 0.027 0.7489 1 0.0 O5 O-2 0.887 0.25 0.72 1 0.0 O1 O-2 0.781 -0.003 0.102 1 0.0 O3 O-2 0.726 0.25 0.481 1 0.0