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We explore the magnetic properties of Nd₂Zr₂O₇ and Pr₂Zr₂O₇ single crystals subjected to pulsed magnetic fields up to 60 T using magnetization and magnetocaloric-effect (MCE) measurements, with initial temperatures ranging from 2 to 31K. The MCE data exhibit pronounced and unconventional hysteresis loops, in which the sample temperature increases during both the up-sweep and down-sweep of the field. In Nd₂Zr₂O₇, the MCE further displays a striking plateau as a function of time, followed by a rapid temperature rise that begins at the maximum applied field, across pulses with differing peak-field strengths. Our magnetization measurements reveal an inferred temperature of the magnetic subsystem that differs significantly from the directly measured sample temperature and exhibits opposite hysteresis: the temperature is higher on the up-sweep than the down-sweep, unlike the direct measurements. These observations indicate a breakdown of thermal equilibrium between magnetic and lattice degrees of freedom on the timescale of the pulse (~ 10⁻¹s). We interpret the results using a phenomenological model involving two thermally coupled subsystems - the magnetic ions and phonons, and a thermal reservoir, which accounts well for the behavior of Pr₂Zr₂O₇. However, it fails to reproduce the plateau seen in Nd₂Zr₂O₇. Agreement with Nd₂Zr₂O₇ data is improved substantially if we allow the thermal coupling between the magnetic and the lattice subsystems to depend on the product HdH/dt. Our results reveal anomalously slow heat transfer between magnetic and lattice subsystems and point toward a novel mechanism for dynamically controlling the heat flow in Nd₂Zr₂O₇ via the rate of magnetic field variation.
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Benton et al. (2026) studied this question.
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