Changes in the electronic structure upon the B2–B19′ martensitic transformation in titanium-nickel

2001 ◽  
Vol 43 (4) ◽  
pp. 737-745 ◽  
Author(s):  
S. E. Kulkova ◽  
D. V. Valujsky ◽  
I. Yu. Smolin
Keyword(s):  
Electronic Structure ◽  
Martensitic Transformation ◽  
Titanium Nickel

scholarly journals EELS Study of the Electronic Structure Changes Associated with the Martensitic Transformation in a Cu-Al-Be Alloy

2003 ◽  
Vol 9 (S02) ◽  
pp. 580-581
Author(s):  
D. Ríos-Jara ◽  
H. Flores-Zúñiga ◽  
M.T. Ochoa ◽  
F. Espinosa-Magaña
Keyword(s):  
Electronic Structure ◽  
Martensitic Transformation ◽  
Structure Changes

scholarly journals An Interpretation of Martensitic Transformation in L12-Type Fe3Pt from Its Electronic Structure

2010 ◽  
Vol 51 (5) ◽  
pp. 896-898 ◽  
Author(s):  
Takuya Yamamoto ◽  
Masataka Yamamoto ◽  
Takashi Fukuda ◽  
Tomoyuki Kakeshita ◽  
Hisazumi Akai
Keyword(s):  
Electronic Structure ◽  
Martensitic Transformation

Martensitic transformation and magnetic properties in Pd2MnGa Heusler alloy by DFT study

2019 ◽  
Vol 33 (07) ◽  
pp. 1950074
Author(s):  
Bin Yang ◽  
Zhinan Li ◽  
Fanghui Zhu ◽  
Liwu Jiang ◽  
Chuan-Hui Zhang
Keyword(s):  
Magnetic Properties ◽  
Electronic Structure ◽  
Martensitic Transformation ◽  
Magnetic Moment ◽  
First Principles ◽  
Heusler Alloy ◽  
Theoretical Calculations ◽  
Text Structure ◽  
Dft Study ◽  
First Principles Calculations

The electronic structure, martensitic transformation and magnetic properties of [Formula: see text] Heusler alloy were studied by first-principles calculations. It is found that the stable structure of austenitic [Formula: see text] is the ferromagnetic [Formula: see text] structure, and a martensitic transformation is possible to occur with the distortion degree of 1.26. By the analysis of the electronic structure, some results of magnetic moment are consistent with previous theoretical calculations.

scholarly journals Martensitic transformation, electronic structure and magnetism in D03-ordered Heusler Mn3 Z (Z = B, Al, Ga, Ge, Sb) alloys

2018 ◽  
Vol 74 (6) ◽  
pp. 673-680 ◽  
Author(s):  
Tingzhou Li ◽  
R. Khenata ◽  
Zhenxiang Cheng ◽  
Hong Chen ◽  
Hongkuan Yuan ◽  
...  
Keyword(s):  
Thin Films ◽  
Electronic Structure ◽  
Martensitic Transformation ◽  
Compressive Strain ◽  
First Principles Calculations ◽  
Ferromagnetic Shape Memory Alloy ◽  
Half Metallic ◽  
Magnetic Metal ◽  
Zero Moment ◽  
Ferromagnetic Shape Memory

Recently, 50-nm Heusler Mn3Al thin films were experimentally synthesized by Jamer et al. [Phys. Rev. Appl. (2017), 7, 064036] and the nominal zero moment, i.e. the fully compensated ferrimagnetic property, of these thin films was confirmed. That work motivated the current investigation on the martensitic transformation, electronic structure and magnetism of D03-ordered Mn3Al using first-principles calculations. Owing to tetragonal distortion, the martensitic transformation only occurs with tensile strain rather than with compressive strain and the half-metallic-type Mn3Al becomes a magnetic metal. Consequently, Mn3Al shows great potential for application as a ferromagnetic shape memory alloy. Moreover, not only did the martensitic transformation occur in Mn3Al, it was also observed in similar D03-ordered Mn3 Z (Z = B, Ga, Ge, Sb) compounds.

First-principles investigation of possible martensitic transformation and magnetic properties of Heusler-type Pt2-xMn1+xIn alloys

2015 ◽  
Vol 08 (06) ◽  
pp. 1550064 ◽  
Author(s):  
Lin Feng ◽  
Wenxing Zhang ◽  
Enke Liu ◽  
Wenhong Wang ◽  
Guangheng Wu
Keyword(s):  
Magnetic Properties ◽  
Phase Transformation ◽  
Electronic Structure ◽  
Martensitic Transformation ◽  
Phase Stability ◽  
First Principles ◽  
Electronic Structures ◽  
First Principles Calculations ◽  
Magnetic Structures

The phase stability, electronic structure and magnetism of Pt 2-x Mn 1+x In (x = 0, 0.25, 0.5, 0.75, 1) alloys are studied by first-principles calculations. The possible magnetic martensitic transformation in this series has been investigated. For all the five compounds, the energy minimums occur around c/a = 1.30, and the energy differences between the austenitic and martensitic phases are large enough to overcome the resistance of phase transformation. By comparing the electronic structures of austenitic and martensitic phases, we can find that the phase stability is enhanced by the martensitic transformation. The magnetic structures of the austenitic and martensitic phases are also discussed.

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