TY - JOUR
T1 - History-dependent nucleation and growth of the martensitic phase in the magnetic shape memory alloy Ni 45Co 5Mn 38Sn 12
AU - Banerjee, A.
AU - Chaddah, P.
AU - Dash, S.
AU - Kumar, Kranti
AU - Lakhani, Archana
AU - Chen, X.
AU - Ramanujan, R. V.
PY - 2011/12/12
Y1 - 2011/12/12
N2 - We study through the time evolution of magnetization the low-temperature (T) dynamics of the metastable coexisting phases created by traversing different paths in magnetic field H and T space in a shape memory alloy system, Ni 45Co 5Mn 38Sn 12. It is shown that these coexisting phases consisting of a fraction of kinetically arrested austenite phase and a remaining fraction of low-T equilibrium martensitic phase undergo a slow relaxation to low magnetization (martensitic) state but with very different thermomagnetic history-dependent rates at the same T and H. We discovered that, when the nucleation of the martensitic phase is initiated at much lower T through the de-arrest of the glasslike arrested state contrasted with the respective first-order transformation (through supercooling at much higher T), the long-time relaxation rate scales with the nonequilibrium phase fraction but has a very weak dependence on T. This is explained on the basis of the H-T path dependent size of the critical radii of the nuclei and the subsequent growth of the equilibrium phase through the motion of the interface.
AB - We study through the time evolution of magnetization the low-temperature (T) dynamics of the metastable coexisting phases created by traversing different paths in magnetic field H and T space in a shape memory alloy system, Ni 45Co 5Mn 38Sn 12. It is shown that these coexisting phases consisting of a fraction of kinetically arrested austenite phase and a remaining fraction of low-T equilibrium martensitic phase undergo a slow relaxation to low magnetization (martensitic) state but with very different thermomagnetic history-dependent rates at the same T and H. We discovered that, when the nucleation of the martensitic phase is initiated at much lower T through the de-arrest of the glasslike arrested state contrasted with the respective first-order transformation (through supercooling at much higher T), the long-time relaxation rate scales with the nonequilibrium phase fraction but has a very weak dependence on T. This is explained on the basis of the H-T path dependent size of the critical radii of the nuclei and the subsequent growth of the equilibrium phase through the motion of the interface.
UR - http://www.scopus.com/inward/record.url?scp=84855310196&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84855310196&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.84.214420
DO - 10.1103/PhysRevB.84.214420
M3 - Article
AN - SCOPUS:84855310196
SN - 1098-0121
VL - 84
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 21
M1 - 214420
ER -