Mg2CdSn11Ir6
高熵材料 HEAMP-ID: mp-3204690 · 空间群: C2 (#5)
基础信息
能量属性
电子属性
磁性属性
弹性属性
弹性数据暂不开放
特征分析
关联任务
引用参考
The crystal structure and related material properties of Mg2CdSn11Ir6 were obtained from the Materials Project database (MP-ID: mp-3204690, database version v2026.04.13).
Horton, M.K., Huck, P., Yang, R.X. et al. Accelerated data-driven materials science with the Materials Project. Nat. Mater. 24, 1522–1532 (2025). https://doi.org/10.1038/s41563-025-02272-0
晶体结构 3D 渲染
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# generated using pymatgen
data_Mg2CdSn11Ir6
_symmetry_space_group_name_H-M 'P 1'
_cell_length_a 8.12602270
_cell_length_b 8.15533681
_cell_length_c 8.15533648
_cell_angle_alpha 108.63121246
_cell_angle_beta 110.14570699
_cell_angle_gamma 110.14571065
_symmetry_Int_Tables_number 1
_chemical_formula_structural Mg2CdSn11Ir6
_chemical_formula_sum 'Mg2 Cd1 Sn11 Ir6'
_cell_volume 413.33890239
_cell_formula_units_Z 1
loop_
_symmetry_equiv_pos_site_id
_symmetry_equiv_pos_as_xyz
1 'x, y, z'
loop_
_atom_site_type_symbol
_atom_site_label
_atom_site_symmetry_multiplicity
_atom_site_fract_x
_atom_site_fract_y
_atom_site_fract_z
_atom_site_occupancy
Mg Mg0 1 0.68939135 0.99553084 0.99667740 1.0
Mg Mg1 1 0.31060865 0.00332260 0.00446916 1.0
Cd Cd2 1 0.50000000 0.75772732 0.24227268 1.0
Sn Sn3 1 0.50000000 0.24200547 0.75799453 1.0
Sn Sn4 1 0.26114823 0.52093863 0.76522994 1.0
Sn Sn5 1 0.74195714 0.49012357 0.24545844 1.0
Sn Sn6 1 0.73885177 0.23477006 0.47906137 1.0
Sn Sn7 1 0.25804286 0.75454156 0.50987643 1.0
Sn Sn8 1 0.32990347 0.32383119 0.32123176 1.0
Sn Sn9 1 0.67009653 0.67876824 0.67616881 1.0
Sn Sn10 1 0.00111729 0.99713478 0.67483114 1.0
Sn Sn11 1 0.00905429 0.67861656 0.00086601 1.0
Sn Sn12 1 0.99094571 0.99913399 0.32138344 1.0
Sn Sn13 1 0.99888271 0.32516886 0.00286522 1.0
Ir Ir14 1 0.00829144 0.34858138 0.34899468 1.0
Ir Ir15 1 0.99170856 0.65100532 0.65141862 1.0
Ir Ir16 1 0.33715492 0.00656389 0.35391321 1.0
Ir Ir17 1 0.66211036 0.00639554 0.66024559 1.0
Ir Ir18 1 0.33788964 0.33975441 0.99360446 1.0
Ir Ir19 1 0.66284508 0.64608679 0.99343611 1.0
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