Phason mode in the incommensurate martensitic phase of Ni2MnGa - observed by neutron spectroscopy
dc.contributor.author | Vorderwisch, P | en_AU |
dc.contributor.author | Shapiro, SM | en_AU |
dc.contributor.author | Habicht, K | en_AU |
dc.contributor.author | Hradil, K | en_AU |
dc.contributor.author | Schneider, H | en_AU |
dc.date.accessioned | 2021-09-21T01:30:04Z | en_AU |
dc.date.available | 2021-09-21T01:30:04Z | en_AU |
dc.date.issued | 2006-12-04 | en_AU |
dc.date.statistics | 2021-08-31 | en_AU |
dc.description.abstract | The ferromagnetic shape-memory alloy Ni2MnGa, of technological interest as a magnetically driven actuator, undergoes a martensitic transformation from a cubic austenite to a tetragonally distorted martensite structure. Previous inelastic neutron scattering experiments, performed in the martensite phase, show an anomaly in the phonon dispersion for the [110] transverse acoustic branch TA2 [1]. This anomaly is identified (in ab-initio calculations through examination of Fermi-surface nesting and electron-phonon coupling) as a Kohn anomaly [2] and occurs at a wave vector incommensurate with the underlying lattice. Elastic neutron scattering reveals a modulation of the martensite phase with this incommensurate wave vector [1]. In very recent inelastic experiments, performed with cold- and thermal-neutron triple-axis-spectrometers, in addition to the known acoustic branch a new dispersive branch was found, showing all characteristics of a phason mode. In our interpretation, the new mode is caused by a charge-density-wave in the incommensurately distorted lattice. Inelastic neutron scattering is the only technique able to unambiguously detect a phason branch - and successful examples are rare. [1] P. Vorderwisch and S.M. Shapiro, submitted [2] C. Bungaro et al., Phys. Rev. B 68 (2003) 134104 | en_AU |
dc.identifier.citation | Vorderwisch, P., Shapiro, S., Habicht, K., Hradil, K., & Schneider, H. (2006). Phason mode in the incommensurate martensitic phase of Ni2MnGa - observed by neutron spectroscopy. Paper presented at the Australian Instute of Physics 17th National Congress 2006, Brisbane Convention and Exhibition Centre, Brisbane Australia, Sunday 3 - Friday 8 December 2006. Retrieved from: https://www.aip.org.au/resources/Documents/Congress/AIPCongress-2006-Program.pdf | en_AU |
dc.identifier.conferenceenddate | 8 December 2006 | en_AU |
dc.identifier.conferencename | Australian Instute of Physics 17th National Congress 2006 | en_AU |
dc.identifier.conferenceplace | Brisbane, Australia | en_AU |
dc.identifier.conferencestartdate | 3 December 2006 | en_AU |
dc.identifier.uri | https://www.aip.org.au/resources/Documents/Congress/AIPCongress-2006-Program.pdf | en_AU |
dc.identifier.uri | https://apo.ansto.gov.au/dspace/handle/10238/11754 | en_AU |
dc.language.iso | en | en_AU |
dc.publisher | Australian Institute of Physics | en_AU |
dc.subject | Ferromagnetic materials | en_AU |
dc.subject | Alloys | en_AU |
dc.subject | Actuators | en_AU |
dc.subject | Martensitic steels | en_AU |
dc.subject | Transformations | en_AU |
dc.subject | Austenite | en_AU |
dc.subject | Inelastic scattering | en_AU |
dc.subject | Spectrometers | en_AU |
dc.title | Phason mode in the incommensurate martensitic phase of Ni2MnGa - observed by neutron spectroscopy | en_AU |
dc.type | Conference Abstract | en_AU |