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Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X2MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni)
In this work, we investigated the phase transition and electronic structures of some newly designed all- d -metal Heusler compounds, X 2 MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni), by means of the first principles. The competition between the XA and L2 1 structures of these materials was studied, and we...
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Published in: | Frontiers in chemistry 2020-12, Vol.8, p.546947-546947 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In this work, we investigated the phase transition and electronic structures of some newly designed all-
d
-metal Heusler compounds, X
2
MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni), by means of the first principles. The competition between the XA and L2
1
structures of these materials was studied, and we found that X
2
MnTi favors to feature the L2
1
-type structure, which is consistent with the well-known site-preference rule (SPR). Under the L2
1
structure, we have studied the most stable magnetic state of these materials, and we found that the ferromagnetic state is the most stable due to its lower energy. Through tetragonal deformation, we found that the L2
1
structure is no longer the most stable structure, and a more stable tetragonal L1
0
structure appeared. That is, under the tetragonal strain, the material enjoys a tetragonal phase transformation (i.e., from cubic L2
1
to tetragonal L1
0
structure). This mechanism of L2
1
-L1
0
structure transition is discussed in detail based on the calculated density of states. Moreover, we found that the energy difference between the most stable phases of L1
0
and L2
1
, defined as Δ
E
M
(Δ
E
M
=
E
Cubic
-
E
Tetragonal
), can be adjusted by the uniform strain. Finally, the phonon spectra of all tetragonal X
2
MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni) phases are exhibited, which provides a powerful evidence for the stability of the tetragonal L1
0
state. We hope that our research can provide a theoretical guidance for future experimental investigations. |
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ISSN: | 2296-2646 2296-2646 |
DOI: | 10.3389/fchem.2020.546947 |