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Ba2Ni2F11

高熵材料 HEA 传统材料 TRA

MP-ID: mp-1041199 · 空间群: P3_2 (#145)

基础信息

化学式
Ba2Ni2F11
MP-ID
mp-1041199
元素数
3
位点数
45
密度
4.2928
g/cm³
体积
697.46
ų
晶胞参数 a
7.6012
Å
晶胞参数 b
7.6012
Å
晶胞参数 c
13.9390
Å
α 角
90.00
°
β 角
90.00
°
γ 角
120.00
°
空间群
P3_2
点群
3
晶体系统
Trigonal
布拉维格子
Trigonal P
稳定性
否
堆积分数
0.7400

X 射线衍射

衍射图谱
横轴为 2θ (°),纵轴为相对强度,CuKa , λ=1.5406 Å
衍射峰(Top 24)
2θd (Å)Ihkl
13.45 6.5828 14.4 (1,0,-1,0)
14.88 5.9524 27.7 (1,0,-1,1)
18.54 4.7856 37.5 (1,0,-1,2)
19.10 4.6463 2.3 (0,0,0,3)
23.41 3.8006 1.9 (2,-1,-1,0)
23.44 3.7960 82.8 (1,0,-1,3)
24.27 3.6667 100.0 (2,-1,-1,1)
26.72 3.3367 46.6 (2,-1,-1,2)
27.85 3.2033 55.4 (2,0,-2,1)
28.99 3.0798 34.6 (1,0,-1,4)
30.02 2.9762 44.2 (2,0,-2,2)
30.38 2.9418 14.4 (2,-1,-1,3)
34.95 2.5671 15.4 (1,0,-1,5)
36.10 2.4881 8.3 (3,-1,-2,0)
36.69 2.4494 5.4 (3,-1,-2,1)
37.59 2.3928 13.2 (2,0,-2,4)
38.42 2.3432 55.2 (3,-1,-2,2)
38.76 2.3232 13.6 (0,0,0,6)
40.11 2.2479 11.1 (2,-1,-1,5)
41.14 2.1943 3.3 (3,0,-3,0)
41.16 2.1934 44.5 (3,-1,-2,3)
41.21 2.1907 24.3 (1,0,-1,6)
41.67 2.1676 13.4 (3,0,-3,1)
42.49 2.1273 21.7 (2,0,-2,5)
获取直接链接

能量属性

形成能/原子
-2.63774
eV/atom
能量/原子
-5.06831
eV/atom
凸包距离
0.1529
eV/atom
未修正能量
-4.3907
eV/atom
体积/原子
15.50
ų
c/a 比
1.8338

电子属性

金属性
金属
带隙
0
eV
直接带隙
是
导带底 CBM
N/A
eV

磁性属性

磁性
是
总磁矩
21.0013
μB
磁有序
FM
磁性位点数
15
磁化强度/体积
0.030110
μB/ų

弹性属性

弹性数据暂不开放

特征分析

组成概览

元素组成(原子分数)
组成信息
主元 / 基质元素
F · 0.733
元素家族
Metalloid-Nonmetal
溶质分数
0.267
间隙分数
0.000

高熵合金特征

综合指标雷达(归一化)
元素类别占比
混合熵 ΔS/R
0.7648
高熵判据(>1.0 视为高熵)
混合熵 ΔS
6.3582
J/mol·K
Ω 参数
0.0000
Ω > 1.1 利于固溶体形成
原子尺寸错配 δr
70.643%
δr < 6.6% 利于单相固溶
电负性差 Δχ
1.1709
越小混合越稳定
价电子浓度 VEC
5.267
价电子浓度,影响相稳定性
混合焓 ΔH_mix
0.000
kJ/mol 且负值为放热混合
熵归一化
0.6961
固溶体倾向
0
相趋势
IM

传统材料特征

ROM 混合特征雷达
评级与分类
评级 Tier
B
评分
0.518
家族
F-rich Multi-Component
基质元素
F · 0.733

关联任务

关联的计算任务 ID(2 个)

引用参考

Materials Project 官方页面
https://materialsproject.org/materials/mp-1041199
参考引用

The crystal structure and related material properties of Ba2Ni2F11 were obtained from the Materials Project database (MP-ID: mp-1041199, database version v2026.04.13).

文献引用

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

BibTeX
@article{Horton2025,
  author  = {Horton, Matthew K. and Huck, Patrick and Yang, Ruo Xi and Munro, Jason M. and Dwaraknath, Shyam and Ganose, Alex M. and Kingsbury, Ryan S. and Wen, Mingjian and Shen, Jimmy X. and Mathis, Tyler S. and Kaplan, Aaron D. and Berket, Karlo and Riebesell, Janosh and George, Janine and Rosen, Andrew S. and Spotte-Smith, Evan W. C. and McDermott, Matthew J. and Cohen, Orion A. and Dunn, Alex and Kuner, Matthew C. and Rignanese, Gian-Marco and Petretto, Guido and Waroquiers, David and Griffin, Sinead M. and Neaton, Jeffrey B. and Chrzan, Daryl C. and Asta, Mark and Hautier, Geoffroy and Cholia, Shreyas and Ceder, Gerbrand and Ong, Shyue Ping and Jain, Anubhav and Persson, Kristin A.},
  title   = {Accelerated data-driven materials science with the Materials Project},
  journal = {Nature Materials},
  year    = {2025},
  volume  = {24},
  number  = {10},
  pages   = {1522--1532},
  month   = {oct},
  doi     = {10.1038/s41563-025-02272-0},
  issn    = {1476-4660},
  url     = {https://doi.org/10.1038/s41563-025-02272-0},
  abstract = {The Materials Project was launched formally in 2011 to drive materials discovery forwards through high-throughput computation and open data. More than a decade later, the Materials Project has become an indispensable tool used by more than 600,000 materials researchers around the world. This Perspective describes how the Materials Project, as a data platform and a software ecosystem, has helped to shape research in data-driven materials science. We cover how sustainable software and computational methods have accelerated materials design while becoming more open source and collaborative in nature. Next, we present cases where the Materials Project was used to understand and discover functional materials. We then describe our efforts to meet the needs of an expanding user base, through technical infrastructure updates ranging from data architecture and cloud resources to interactive web applications. Finally, we discuss opportunities to better aid the research community, with the vision that more accessible and easy-to-understand materials data will result in democratized materials knowledge and an increasingly collaborative community.}
}

晶体结构 3D 渲染

加载 3D 结构...

样式: Ball & Stick
原始 CIF 数据
# generated using pymatgen
data_Ba2Ni2F11
_symmetry_space_group_name_H-M   'P 1'
_cell_length_a   7.60116389
_cell_length_b   7.60116389
_cell_length_c   13.93896200
_cell_angle_alpha   90.00000000
_cell_angle_beta   90.00000000
_cell_angle_gamma   119.99999908
_symmetry_Int_Tables_number   1
_chemical_formula_structural   Ba2Ni2F11
_chemical_formula_sum   'Ba6 Ni6 F33'
_cell_volume   697.46314437
_cell_formula_units_Z   3
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
  Ba  Ba0  1  0.53000600  0.18136700  0.67569500  1.0
  Ba  Ba1  1  0.15370800  0.47749900  0.82763100  1.0
  Ba  Ba2  1  0.65136100  0.46999400  0.00902900  1.0
  Ba  Ba3  1  0.52250100  0.67620900  0.49429700  1.0
  Ba  Ba4  1  0.32379100  0.84629200  0.16096400  1.0
  Ba  Ba5  1  0.81863300  0.34863900  0.34236200  1.0
  Ni  Ni6  1  0.64928600  0.97589300  0.88180800  1.0
  Ni  Ni7  1  0.85634400  0.77511700  0.72628800  1.0
  Ni  Ni8  1  0.22488300  0.08122700  0.39295400  1.0
  Ni  Ni9  1  0.32660700  0.35071400  0.21514100  1.0
  Ni  Ni10  1  0.91877300  0.14365600  0.05962100  1.0
  Ni  Ni11  1  0.02410700  0.67339300  0.54847500  1.0
  F  F12  1  0.63210800  0.05091900  0.01548600  1.0
  F  F13  1  0.51882900  0.71166200  0.93027800  1.0
  F  F14  1  0.41881000  0.36789200  0.34881900  1.0
  F  F15  1  0.10922100  0.50531500  0.48601800  1.0
  F  F16  1  0.51862000  0.26995800  0.18122600  1.0
  F  F17  1  0.93730400  0.60485900  0.18539100  1.0
  F  F18  1  0.49468500  0.60390600  0.15268500  1.0
  F  F19  1  0.39514100  0.33244500  0.85205800  1.0
  F  F20  1  0.75133700  0.48138000  0.51456000  1.0
  F  F21  1  0.20825800  0.26768400  0.08966300  1.0
  F  F22  1  0.39609400  0.89077900  0.81935200  1.0
  F  F23  1  0.94908100  0.58119000  0.68215300  1.0
  F  F24  1  0.32786900  0.04338700  0.99904600  1.0
  F  F25  1  0.99230200  0.41456800  0.01419000  1.0
  F  F26  1  0.71551800  0.67213100  0.33237900  1.0
  F  F27  1  0.28833800  0.80716700  0.59694500  1.0
  F  F28  1  0.93682800  0.09163600  0.92099400  1.0
  F  F29  1  0.05942600  0.79174200  0.42299600  1.0
  F  F30  1  0.01207600  0.12660300  0.40589900  1.0
  F  F31  1  0.95661300  0.28448200  0.66571300  1.0
  F  F32  1  0.11452600  0.98792400  0.73923300  1.0
  F  F33  1  0.58543200  0.57773500  0.68085600  1.0
  F  F34  1  0.42226500  0.00769800  0.34752300  1.0
  F  F35  1  0.15480800  0.06317200  0.25432700  1.0
  F  F36  1  0.73231600  0.94057400  0.75632900  1.0
  F  F37  1  0.73004200  0.24866300  0.84789300  1.0
  F  F38  1  0.19283300  0.48117100  0.26361200  1.0
  F  F39  1  0.83718200  0.66816800  0.84645200  1.0
  F  F40  1  0.83098700  0.16281800  0.17978500  1.0
  F  F41  1  0.87339700  0.88547400  0.07256600  1.0
  F  F42  1  0.66755500  0.06269600  0.51872500  1.0
  F  F43  1  0.90836400  0.84519200  0.58766100  1.0
  F  F44  1  0.33183200  0.16901300  0.51311900  1.0
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