Cu(BrN3)2
高熵材料 HEA 传统材料 TRAMP-ID: mp-1079457 · 空间群: Fm-3m (#225)
基础信息
X 射线衍射
| 2θ | d (Å) | I | hkl |
|---|---|---|---|
| 22.04 | 4.0328 | 4.1 | (1,1,0) |
| 31.37 | 2.8516 | 100.0 | (2,1,1) |
| 36.96 | 2.4319 | 8.8 | (2,2,1) |
| 38.67 | 2.3284 | 9.0 | (2,2,2) |
| 44.96 | 2.0164 | 21.0 | (2,2,0) |
| 49.24 | 1.8504 | 9.3 | (3,1,1) |
| 50.61 | 1.8035 | 8.1 | (3,2,1) |
| 55.84 | 1.6464 | 25.3 | (3,3,2) |
| 59.56 | 1.5522 | 3.8 | (3,2,0) |
| 65.46 | 1.4258 | 9.3 | (4,2,2) |
| 68.87 | 1.3633 | 3.5 | (4,2,1) |
| 69.99 | 1.3443 | 6.0 | (4,3,3) |
| 74.39 | 1.2753 | 17.9 | (4,3,1) |
| 77.62 | 1.2300 | 2.4 | (4,4,3) |
| 78.69 | 1.2159 | 2.1 | (4,4,2) |
| 82.94 | 1.1642 | 2.3 | (4,4,4) |
| 87.14 | 1.1185 | 1.2 | (5,3,2) |
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
组成概览
高熵合金特征
传统材料特征
关联任务
引用参考
The crystal structure and related material properties of Cu(BrN3)2 were obtained from the Materials Project database (MP-ID: mp-1079457, 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
加载 3D 结构...
# generated using pymatgen
data_Cu(BrN3)2
_symmetry_space_group_name_H-M 'P 1'
_cell_length_a 5.70327298
_cell_length_b 5.70327298
_cell_length_c 5.70327298
_cell_angle_alpha 60.00000000
_cell_angle_beta 60.00000000
_cell_angle_gamma 60.00000000
_symmetry_Int_Tables_number 1
_chemical_formula_structural Cu(BrN3)2
_chemical_formula_sum 'Cu1 Br2 N6'
_cell_volume 131.17693511
_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
Cu Cu0 1 0.00000000 0.00000000 0.00000000 1.0
Br Br1 1 0.75000000 0.75000000 0.75000000 1.0
Br Br2 1 0.25000000 0.25000000 0.25000000 1.0
N N3 1 0.65109500 0.65109500 0.34890500 1.0
N N4 1 0.34890500 0.65109500 0.34890500 1.0
N N5 1 0.65109500 0.34890500 0.34890500 1.0
N N6 1 0.34890500 0.34890500 0.65109500 1.0
N N7 1 0.65109500 0.34890500 0.65109500 1.0
N N8 1 0.34890500 0.65109500 0.65109500 1.0
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