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Quantum Mpemba Effect: Controlling Thermalization via Initial State Symmetry

Original: "Tuning the Quantum Mpemba Effect in Isolated System by Initial State Engineering"
arXiv:2505.02040v2 · 2025-05-04 · CC BY · ⏱ 3 min · Quantum Physics
By controlling the charge distribution in a quantum thermal bath, physicists have learned to speed up or slow down the system's approach to equilibrium.
Abstract

The quantum Mpemba effect was investigated in isolated non-integrable quantum systems, where relaxation dynamics depend on the structure of initial states. Analysis of initial state distributions across symmetry subspaces reveals a tunable mechanism responsible for the effect: some states, initially further from equilibrium, relax faster. An experimentally realizable quantum scheme without complex control, suitable for quantum simulators, is proposed to verify theoretical predictions. The results establish symmetry-resolved state engineering as a practical tool for managing non-equilibrium quantum dynamics.

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Context

Why does water seemingly defy intuition by freezing faster from a hot state? This paradox, known as the Mpemba effect, was recently extended to the quantum world, where nonequilibrium systems sometimes relax faster the further they are from equilibrium. Understanding such processes is critical for quantum information technologies, where uncontrolled thermalization destroys quantum states. However, the mechanisms allowing control over quantum relaxation rates remained unclear.

Methods

The researchers considered an isolated chain of 15 spins, split into a small open system (3 spins) and a thermal bath (12 spins). The Hamiltonian with long-range interactions and a non-uniform field was chosen to be nonintegrable, so that the only conserved quantity was total spin along the z-axis—analogous to electric charge. Using entanglement of spin pairs, they parameterized the bath's initial state by varying charge variance without changing its mean. Relaxation was tracked via measurement of entanglement asymmetry—a measure of restored-symmetry deviation in the density matrix, introduced in the spirit of von Neumann. The design was verified with a quantum circuit suitable for implementation on quantum simulators, as envisioned by Richard Feynman.

Results

Numerical simulations showed that the decay rate of off-diagonal density matrix elements of the open system directly depends on the width of the energy spectrum in the occupied symmetry sectors of the bath. When the bath's initial state had small charge variance—corresponding to a narrow superposition distribution—relaxation accelerated. Conversely, large variance slowed thermalization. For instance, with a fixed system initial state, varying the bath parameter θb from π/2 to π reduced the characteristic time t0 by about 30%. Moreover, by simultaneously tuning system and bath states, they could switch on and off the quantum Mpemba effect itself: in one regime the asymmetry curves crossed, in another they did not. Interestingly, averaging over random thermalization times was unnecessary—fluctuations did not disrupt control.

Implications

The work establishes a direct link between entropy at the microlevel and macroscopic irreversibility. A denser energy spectrum—akin to the rapid entropy growth in Boltzmann's formula S = k log W—acts as a lubricant for dynamics, facilitating exploration of phase space. This not only deepens the understanding of thermalization in quantum chaotic systems but also provides a practical tool: by manipulating the initial symmetries of the bath, one can program the 'heat death tempo' of a quantum device.

Future development

The next challenge is to account for additional symmetries and interactions of multiple conserved charges. Even finer relaxation tuning might emerge, potentially halting thermalization completely in certain subspaces—a phenomenon already observed in many-body localization.

Impact

The results will influence the design of quantum processors, where controlling decoherence time is crucial, as well as quantum thermodynamics, offering new methods to manage heat and information flows.

Next steps

Experimental verification on platforms like ion traps or superconducting qubits, as well as studying the role of quantum chaos in operator growth.

Key open problems

The study links the Mpemba effect to the fundamental problem of quantum thermalization and the eigenstate thermalization hypothesis, as well as to the arrow of time—why irreversibility is so universal when microscopic laws are time-symmetric.

🎯 The classical Mpemba effect was noticed by Aristotle and rediscovered by Tanzanian schoolboy Erasto Mpemba in 1963 while making ice cream.

🎬 The idea of controlling thermalization rates echoes the concept of 'entropy slowdown' in Greg Egan's novel 'Permutation City'.

S = k_B \ln \Omega
Entropy is proportional to the logarithm of the number of accessible microstates; a higher density of energy levels means faster entropy growth and, consequently, accelerated relaxation.
\Delta S_A = \mathrm{tr}\left[ \rho ( \log\rho - \log\rho_Q ) \right]
A quantum-information measure of symmetry restoration: ρ is the subsystem density matrix, ρ_Q its fully charge-symmetrized version.
\mathrm{Var}(\omega) = \mathrm{Var}\left( E_{n_1}^{m+q_1} \right) + \mathrm{Var}\left( E_{n_2}^{m+q_2} \right)
The width of the spectral function that determines the relaxation rate of off-diagonal elements; the larger the variance, the faster the decay.

Key numbers

  • number of qubits in thermal bath: 12
  • number of qubits in open system: 3
  • total spin chain length: 15
  • exchange interaction constant J: 1.0
  • magnetic field amplitude h: 0.2
Scientists
Erwin SchrödingerHugh Everett IIINiels BohrPascual JordanWerner HeisenbergStephen Hawking
Tags
quantum information entropy quantum decoherence quantum computer quantum entanglement superposition quantum measurement Water
Laws
second law of thermodynamicsSchrödinger equationHeisenberg uncertainty principleHawking radiationBekenstein-Hawking entropyBoltzmann distribution
Original: arXiv:2505.02040v2 · CC BY · bridge42worlds