2002
DOI: 10.1063/1.1478131
|View full text |Cite
|
Sign up to set email alerts
|

Influence of structural transition on transport and optical properties of Ni2MnGa alloy

Abstract: The transport and optical properties of Ni2MnGa alloy in the martensitic and austenitic states were investigated. The dependence of the temperature coefficient of resistivity on temperature shows kinks at the structural and ferroparamagnetic transitions. Electron-magnon and electron-phonon scattering are analyzed to be the dominant scattering mechanisms of the Ni2MnGa alloy in the martensitic and austenitic states, respectively. It was observed that the martensite reveals a higher Debye temperature compared to… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
14
0

Year Published

2003
2003
2017
2017

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 28 publications
(14 citation statements)
references
References 19 publications
0
14
0
Order By: Relevance
“…The transport property of Ni 2 MnGa is dominated by electron-magnon and electron-phonon scattering 47 . The resistivity behaviour of Ni 2+x Mn 1-x Ga is metallic with sudden increase in resistivity at the martensitic transition (see Biswas et al 30 , figure 1 a).…”
Section: Transport Analysismentioning
confidence: 99%
“…The transport property of Ni 2 MnGa is dominated by electron-magnon and electron-phonon scattering 47 . The resistivity behaviour of Ni 2+x Mn 1-x Ga is metallic with sudden increase in resistivity at the martensitic transition (see Biswas et al 30 , figure 1 a).…”
Section: Transport Analysismentioning
confidence: 99%
“…Moreover, 10 M214 M is accompanied by a decrease in r in both the forward and the reverse transformations. Since both IMTs have a large temperature hysteresis, these unusual features of the transport properties could be explained by assuming that electron-phonon and electron-magnon contributions to the electrical resistivity depend considerably on temperature [15] but to different extent for the different martensitic phases.…”
mentioning
confidence: 99%
“…The time-resolved x-ray diffraction was performed at an x-ray energy of 5 keV using a synchrotron slicing source (200 ph/pulse, 2 kHz and 1.2 %bw) as probe and an 800 nm, 120 fs 1 kHz p-polarized laser pulse at 12 o incidence as pump (absorption length δ = 20 nm [20]), giving a total time resolution of 200 fs [21]. The x-ray spot was focused horizontally to 400 µm, vertically to 10 µm and the gracing incidence angle was set to 0.65 (absorption length α = 20 nm [22]) to match the penetration depth of the x-ray probe to the laser pump.…”
mentioning
confidence: 99%
“…The MT structure is modulated [7, 9,19] but unlike the single modulation wavevector q = [ξξ0] with ξ = 0.428 of single crystal Ni 2 MnGa, the film has two modulation wavevectors with ξ = 0.311(2) and 0.51(1) in reciprocal lattice units of the orthorhombic lattice. The first wavevector is close to the ξ = 0.308 found for the 7M structure [8].The time-resolved x-ray diffraction was performed at an x-ray energy of 5 keV using a synchrotron slicing source (200 ph/pulse, 2 kHz and 1.2 %bw) as probe and an 800 nm, 120 fs 1 kHz p-polarized laser pulse at 12 o incidence as pump (absorption length δ = 20 nm [20]), giving a total time resolution of 200 fs [21]. The x-ray spot was focused horizontally to 400 µm, vertically to 10 µm and the gracing incidence angle was set to 0.65 o…”
mentioning
confidence: 99%