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Ti7Ni3N10

高熵材料 HEA 传统材料 TRA

MP-ID: mp-676800 · 空间群: Imm2 (#44)

基础信息

化学式
Ti7Ni3N10
MP-ID
mp-676800
元素数
3
位点数
20
密度
5.6532
g/cm³
体积
191.29
ų
晶胞参数 a
8.0072
Å
晶胞参数 b
8.0072
Å
晶胞参数 c
8.0072
Å
α 角
143.40
°
β 角
141.00
°
γ 角
54.55
°
空间群
Imm2
点群
mm2
晶体系统
Orthorhombic
布拉维格子
Orthorhombic I
稳定性
否
堆积分数
0.6800

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
18.72 4.7413 2.9 (1,0,-1)
25.10 3.5484 1.3 (1,2,-2)
27.39 3.2566 5.3 (2,0,-1)
33.53 2.6726 36.4 (1,-1,1)
35.71 2.5142 46.5 (1,-1,-1)
36.26 2.4773 78.7 (3,2,-3)
40.14 2.2466 2.2 (2,-1,-1)
44.10 2.0534 1.1 (3,1,-3)
44.15 2.0514 1.6 (3,0,-2)
49.79 1.8312 43.9 (2,-2,0)
50.22 1.8168 100.0 (1,4,-3)
59.21 1.5604 1.1 (3,-1,-2)
63.80 1.4588 1.1 (4,0,-3)
64.52 1.4444 20.7 (4,1,-4)
65.59 1.4234 11.4 (5,5,-5)
70.47 1.3363 9.1 (2,-2,2)
74.70 1.2707 11.4 (5,0,-3)
75.65 1.2571 2.6 (2,-2,-2)
75.71 1.2563 6.5 (4,6,-6)
76.98 1.2387 8.1 (6,4,-6)
81.59 1.1800 7.0 (3,-3,1)
81.91 1.1761 12.9 (0,5,-4)
85.33 1.1375 7.4 (3,-3,-1)
86.63 1.1238 14.7 (7,3,-5)
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能量属性

形成能/原子
-1.08185
eV/atom
能量/原子
-8.88143
eV/atom
凸包距离
0.2573
eV/atom
未修正能量
-8.7009
eV/atom
体积/原子
9.56
ų
c/a 比
-

电子属性

金属性
金属
带隙
0
eV
直接带隙
否
导带底 CBM
N/A
eV

磁性属性

磁性
否
总磁矩
0.0001
μB
磁有序
NM
磁性位点数
0
磁化强度/体积
0.000000
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
N · 0.500
元素家族
Metalloid-Nonmetal
溶质分数
0.500
间隙分数
0.500

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
0.9986
高熵判据(>1.0 视为高熵)
混合熵 ΔS
8.3022
J/mol·K
Ω 参数
0.0681
Ω > 1.1 利于固溶体形成
原子尺寸错配 δr
31.048%
δr < 6.6% 利于单相固溶
电负性差 Δχ
0.7048
越小混合越稳定
价电子浓度 VEC
5.400
价电子浓度,影响相稳定性
混合焓 ΔH_mix
-118.350
kJ/mol 且负值为放热混合
熵归一化
0.9089
固溶体倾向
0
相趋势
AM

传统材料特征

ROM 混合特征雷达
评级与分类
评级 Tier
C
评分
0.351
家族
Interstitial Alloy
基质元素
N · 0.500

关联任务

关联的计算任务 ID(3 个)

引用参考

Materials Project 官方页面
https://materialsproject.org/materials/mp-676800
参考引用

The crystal structure and related material properties of Ti7Ni3N10 were obtained from the Materials Project database (MP-ID: mp-676800, 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_Ti7Ni3N10
_symmetry_space_group_name_H-M   'P 1'
_cell_length_a   8.00715470
_cell_length_b   8.00715470
_cell_length_c   8.00715470
_cell_angle_alpha   143.39970106
_cell_angle_beta   141.00426854
_cell_angle_gamma   54.54895038
_symmetry_Int_Tables_number   1
_chemical_formula_structural   Ti7Ni3N10
_chemical_formula_sum   'Ti7 Ni3 N10'
_cell_volume   191.28521092
_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
  Ti  Ti0  1  0.90060100  0.40588100  0.50528000  1.0
  Ti  Ti1  1  0.79948700  0.80075800  0.00127100  1.0
  Ti  Ti2  1  0.60040100  0.58816400  0.98776300  1.0
  Ti  Ti3  1  0.50000000  0.99564200  0.49564200  1.0
  Ti  Ti4  1  0.39959900  0.38736100  0.98776300  1.0
  Ti  Ti5  1  0.20051300  0.20178400  0.00127100  1.0
  Ti  Ti6  1  0.09939900  0.60467800  0.50528000  1.0
  Ni  Ni7  1  0.00000000  0.06623200  0.06623200  1.0
  Ni  Ni8  1  0.70447400  0.21771200  0.51323800  1.0
  Ni  Ni9  1  0.29552600  0.80876400  0.51323800  1.0
  N  N10  1  0.95313000  0.85800000  0.41197000  1.0
  N  N11  1  0.85437700  0.26640400  0.92216100  1.0
  N  N12  1  0.73813200  0.64381800  0.38195000  1.0
  N  N13  1  0.65575700  0.06778400  0.92216100  1.0
  N  N14  1  0.55397000  0.45884000  0.41197000  1.0
  N  N15  1  0.44603000  0.85800000  0.90487000  1.0
  N  N16  1  0.34424300  0.26640400  0.41202600  1.0
  N  N17  1  0.26186800  0.64381800  0.90568600  1.0
  N  N18  1  0.14562300  0.06778400  0.41202600  1.0
  N  N19  1  0.04687000  0.45884000  0.90487000  1.0
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