TY - JOUR
T1 - Phonon precursors to the high temperature martensitic transformation in Ti50Pd42Cr8
AU - Shapiro, S. M.
AU - Winn, B. L.
AU - Schlagel, D. L.
AU - Lograsso, T. A.
AU - Erwin, R. L.
PY - 2003/10
Y1 - 2003/10
N2 - Inelastic neutron scattering measurements were carried out on the Ti50Pd50-xCrx alloy, which is a high temperature shape memory material. For x=0, the transformation temperature is ∼800K and for the composition studied (x=8 at.%) Ms ∼ 400K. The majority of the measurements were performed in the parent, B2-phase, up to 873K. Most of the phonons propagating along the three symmetry directions [ζ00], [ζζζ], and [ζζ0] were well defined with the exception of the [ζζ0] transverse acoustic mode with displacements along the [-ζζ0] corresponding to the C'=1/2(C11-C12) elastic constant in the ζ → 0 limit. These phonons are well defined for small ζ, but for ζ > 0.10 they are strongly overdamped near the transition temperature and become better defined at higher temperatures. An elastic peak develops in the cubic phase at ζ=0.22 and increases in intensity as Ms is approached. However, the dispersion curves show no anomaly at this particular wavevector, in marked contrast to the lattice dynamic studies of other systems exhibiting Martensitic transformations.
AB - Inelastic neutron scattering measurements were carried out on the Ti50Pd50-xCrx alloy, which is a high temperature shape memory material. For x=0, the transformation temperature is ∼800K and for the composition studied (x=8 at.%) Ms ∼ 400K. The majority of the measurements were performed in the parent, B2-phase, up to 873K. Most of the phonons propagating along the three symmetry directions [ζ00], [ζζζ], and [ζζ0] were well defined with the exception of the [ζζ0] transverse acoustic mode with displacements along the [-ζζ0] corresponding to the C'=1/2(C11-C12) elastic constant in the ζ → 0 limit. These phonons are well defined for small ζ, but for ζ > 0.10 they are strongly overdamped near the transition temperature and become better defined at higher temperatures. An elastic peak develops in the cubic phase at ζ=0.22 and increases in intensity as Ms is approached. However, the dispersion curves show no anomaly at this particular wavevector, in marked contrast to the lattice dynamic studies of other systems exhibiting Martensitic transformations.
UR - http://www.scopus.com/inward/record.url?scp=0242708895&partnerID=8YFLogxK
U2 - 10.1051/jp4:20031061
DO - 10.1051/jp4:20031061
M3 - Conference article
AN - SCOPUS:0242708895
SN - 1155-4339
VL - 112 II
SP - 1047
EP - 1050
JO - Journal De Physique. IV : JP
JF - Journal De Physique. IV : JP
T2 - International Conference on Martensitic Transformations
Y2 - 10 June 2002 through 14 June 2002
ER -