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Microscopic theory of Mpemba effects and a no-Mpemba theorem for monotone many-body systems
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Mpemba effects (MPEs), where a hotter system cools faster than a colder one, present intriguing anomalies in relaxation processes. Despite their universal observation and significant fundamental and practical implications, a comprehensive theoretical understanding based on microscopic properties remains elusive. In this Letter, we introduce two universal frameworks for classical systems to address this gap. Firstly, we reveal that MPEs, traditionally defined by macroscopic temperature comparisons, can be understood through microstate comparisons. This insight offers a straightforward and universal microscopic perspective on MPEs, relevant for experiments and numerical simulations to identify their microscopic origins. Secondly, we establish a "no-Mpemba theorem," a rigorous sufficient condition for the absence of MPEs, thereby identifying specific classes of systems devoid of these effects. Our findings are exemplified using ferromagnetic Ising models and one-dimensional multiparticle systems, demonstrating the practical applicability of our theoretical advancements.
Forward citations
Cited by 3 Pith papers
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Quantum tunneling Mpemba effect
Non-monotonic a2(Ti) from Sturm-Liouville nodal alignment drives a size-independent quantum tunneling Mpemba effect under boundary absorption when over-barrier decay vastly outpaces the tunneling doublet.
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Predicting the conditions for observing the Mpemba effect
In 1D overdamped relaxation, hard or soft walls—not well count or metastability—determine whether the Mpemba effect appears.
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The Mpemba effect likes to hit a wall
The one-dimensional classical Mpemba effect in an asymmetric double-well is driven solely by a hard wall, not by metastability, and vanishes for infinite systems.
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