#------------------------------------------------------------------------------ #$Date: 2016-02-13 21:28:24 +0200 (Sat, 13 Feb 2016) $ #$Revision: 176429 $ #$URL: file:///home/coder/svn-repositories/cod/cif/1/52/13/1521399.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_1521399 loop_ _publ_author_name 'Kim, J.-S.' 'Cheon, C.-I.' 'Nam, S.' 'Lee, C.-H.' 'Kang, H.-J.' 'Kim, K.-Y.' 'Byun Jae Dong' _publ_section_title ; Crystal structure and microwave dielectric properties of Ca Ti O3 -(Li1/2 Nd1/2) Ti O3 - (Ln1/3 Nd1/3) Ti O3 (Ln = La, Dy) ceramics ; _journal_name_full 'Japanese Journal of Applied Physics, Part 1' _journal_page_first 5633 _journal_page_last 5637 _journal_volume 38 _journal_year 1999 _chemical_formula_sum 'Li0.479 Nd0.521 O2.604 Ti' _chemical_name_systematic '(Li0.479 Nd0.521) Ti O2.604' _space_group_IT_number 117 _symmetry_space_group_name_Hall 'P -4 -2ab' _symmetry_space_group_name_H-M 'P -4 b 2' _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_formula_units_Z 4 _cell_length_a 5.377 _cell_length_b 5.377 _cell_length_c 7.622 _cell_volume 220.368 _citation_journal_id_ASTM JAPNDE _cod_data_source_file Kim_JAPNDE_1999_59.cif _cod_data_source_block Li0.479Nd0.521O2.604Ti1 _cod_original_cell_volume 220.3682 _cod_original_formula_sum 'Li0.479 Nd0.521 O2.604 Ti1' _cod_database_code 1521399 loop_ _symmetry_equiv_pos_as_xyz x,y,z y,-x,-z -x,-y,z -y,x,-z -x+1/2,y+1/2,z y+1/2,x+1/2,-z x+1/2,-y+1/2,z -y+1/2,-x+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 O3 O-2 0.5 0 0 0.653 0.0 Nd1 Nd+3 0 0 0 0.2144 0.0 O1 O-2 0.2829 0.2998 0.2687 1 0.0 Ti1 Ti+3 0.5 0 0.2358 1 0.0 Nd2 Nd+3 0 0 0.5 0.8276 0.0 Li2 Li+1 0 0 0.5 0.1724 0.0 Li1 Li+1 0 0 0 0.7856 0.0 O2 O-2 0.5 0 0.5 0.556 0.0