The irreversibility of the martensite transition in magnetic shape memory alloys (MSMAs) with respect to the external magnetic field is one of the biggest challenges that limits their application as giant caloric materials. This transition is a magnetostructural transition that is accompanied with a steep drop in magnetization (i.e.,$\mathrm{\Delta }M$) around the martensite start temperature $\left({\mathrm{M}}_{\mathrm{s}}\right)$ due to the lower magnetization of the martensite phase. In this Rapid Communication, we show that $\mathrm{\Delta }M$ around ${\mathrm{M}}_{\mathrm{s}}$ in Mn-rich Ni-Mn-based MSMAs gets suppressed by two orders of magnitude in crushed powders due to the stabilization of the martensite phase at temperatures well above ${\mathrm{M}}_{\mathrm{s}}$ and the austenite finish $\left({\mathrm{A}}_{\mathrm{f}}\right)$ temperatures due to residual stresses. Analysis of the intensities and the FWHM of the x-ray powder-diffraction patterns reveals stabilized martensite phase fractions as $97\%, 75\%$, and $90\%$ with corresponding residual microstrains as $5.4\%, 5.6\%$, and $3\%$ in crushed powders of the three different Mn-rich Ni-Mn alloys, namely, $\mathrm{M}{\mathrm{n}}_{1.8}\mathrm{N}{\mathrm{i}}_{1.8}\mathrm{I}{\mathrm{n}}_{0.4}, \mathrm{M}{\mathrm{n}}_{1.75}\mathrm{N}{\mathrm{i}}_{1.25}\mathrm{Ga}$, and $\mathrm{M}{\mathrm{n}}_{1.9}\mathrm{N}{\mathrm{i}}_{1.1}\mathrm{Ga}$, respectively. Even after annealing at 773 K, the residual stress stabilized martensite phase does not fully revert to the equilibrium cubic austenite phase as the magnetostructural transition is only partially restored with a reduced value of $\mathrm{\Delta }M$. Our results have a very significant bearing on the application of such alloys as inverse magnetocaloric and barocaloric materials.

• Received 1 June 2015

DOI:https://doi.org/10.1103/PhysRevB.92.020105