data_global _amcsd_formula_title 'TlAlSi3O8' loop_ _publ_author_name 'Kyono A' 'Kimata M' _journal_name_full 'European Journal of Mineralogy' _journal_volume 13 _journal_year 2001 _journal_page_first 849 _journal_page_last 856 _publ_section_title ; The crystal structure of synthetic TlAlSi3O8: Influence of the inert-pair effect of thallium on the feldspar structure ; _database_code_amcsd 0006900 _chemical_formula_sum 'Tl (Al Si3) O8' _cell_length_a 8.882 _cell_length_b 13.048 _cell_length_c 7.202 _cell_angle_alpha 90 _cell_angle_beta 116.88 _cell_angle_gamma 90 _cell_volume 744.476 _exptl_crystal_density_diffrn 3.958 _symmetry_space_group_name_H-M 'C 1 2/m 1' loop_ _space_group_symop_operation_xyz 'x,y,z' '1/2+x,1/2+y,z' 'x,-y,z' '1/2+x,1/2-y,z' '-x,y,-z' '1/2-x,1/2+y,-z' '-x,-y,-z' '1/2-x,1/2-y,-z' loop_ _atom_site_label _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_occupancy _atom_site_U_iso_or_equiv Tl 0.29680 0.00000 0.15680 1.00000 0.07630 AlT1 0.00810 0.19280 0.22220 0.26100 0.04590 SiT1 0.00810 0.19280 0.22220 0.73900 0.04590 AlT2 0.72230 0.12270 0.33950 0.23900 0.04480 SiT2 0.72230 0.12270 0.33950 0.76100 0.04480 OA1 0.00000 0.14940 0.00000 1.00000 0.05050 OA2 0.67670 0.00000 0.28170 1.00000 0.06700 OB 0.82790 0.16060 0.22120 1.00000 0.05780 OC 0.04100 0.31630 0.26030 1.00000 0.05110 OD 0.17300 0.12840 0.40760 1.00000 0.05540 loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_12 _atom_site_aniso_U_13 _atom_site_aniso_U_23 Tl 0.06200 0.11630 0.04830 0.00000 0.02300 0.00000 AlT1 0.04090 0.07160 0.02740 0.00170 0.01740 0.00150 SiT1 0.04090 0.07160 0.02740 0.00170 0.01740 0.00150 AlT2 0.04120 0.06370 0.03490 0.00200 0.02210 0.00190 SiT2 0.04120 0.06370 0.03490 0.00200 0.02210 0.00190 OA1 0.08790 0.05480 0.01670 0.00000 0.03060 0.00000 OA2 0.05990 0.03590 0.09910 0.00000 0.03060 0.00000 OB 0.05590 0.07430 0.03690 0.00310 0.01550 -0.00350 OC 0.04950 0.06480 0.03100 -0.00320 0.01110 -0.01430 OD 0.08870 0.05460 0.01950 -0.00260 0.02150 -0.00680