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arXiv:2512.00820 · Physics Letters A

Particle creation, adiabaticity, and irreversibility in the TDHO

Salvador J. Robles-Perez, Salvador Castillo-Rivera

quant-phSubmitted Nov 30, 2025• Announced Dec 2, 2025• 0 citations
v1 · Nov 30, 2025v2 · Feb 19, 2026v3 · Sep 3, 2026
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Abstract

We present an exact description of the dynamics and the thermodynamics of a time dependent harmonic oscillator (TDHO) that follows a unitary evolution. In that context, we study the relationship between particle creation, adiabaticity and irreversibility in terms of three different representations: the initial, the diagonal and the invariant representations of the TDHO. We provide analytical results that are valid for any functional value of the frequency and along the whole evolution of the TDHO, which allows us to monitor the behavior of the thermodynamical magnitudes in regions that are not fully considered in previous works, i.e. the transition and the non quasi-static regions. We supplement the analytical results with numerical calculations and graphs. They both show how the largest modes of the non invariant representations may undergo a process of reversible thermalization, where the concept of temperature naturally arises from the unitary evolution of the oscillator with no relation to any external concept of temperature. It would allow us to monitor an unexpected classical-to-quantum transition, which might entail a violation of the third principle of classical thermodynamics. We also provide adaptations of the customary definitions of the quantum heat and work that account for the particle creation of the TDHO. They thus depend on the representation and their evolution is different for the three representations analyzed in this paper, which might have important consequences in the development of quantum thermal machines. Finally, we study the relationship between the creation of particles and the diagonal entropy, which is derived from the von Neumann entropy in the diagonalization limit. The condition of no production of entropy under unitary evolution suggests the definition of a mode temperature that would correspond to the thermal temperature is some appropriate limit.

DOI
10.1016/j.physleta.2026.132089
Comments
25 pages, 35 figures

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We present an exact description of the dynamics and the thermodynamics of a time dependent harmonic oscillator (TDHO) that follows a unitary evolution. In that context, we study the relationship between particle creation, adiabaticity and irreversibility in terms of three different representations: the initial, the diagonal and the invariant representations of the TDHO. We provide analytical results that are valid for any functional value of the frequency and along the whole evolution of the TDHO, which allows us to monitor the behavior of the thermodynamical magnitudes in regions that are not fully considered in previous works, i.e. the transition and the non quasi-static regions. We supplement the analytical results with numerical calculations and graphs.
They both show how the largest modes of the non invariant representations may undergo a process of reversible thermalization, where the concept of temperature naturally arises from the unitary evolution of the oscillator with no relation to any external concept of temperature. It would allow us to monitor an unexpected classical-to-quantum transition, which might entail a violation of the third principle of classical thermodynamics. We also provide adaptations of the customary definitions of the quantum heat and work that account for the particle creation of the TDHO. They thus depend on the representation and their evolution is different for the three representations analyzed in this paper, which might have important consequences in the development of quantum thermal machines. Finally, we study the relationship between the creation of particles and the diagonal entropy, which is derived from the von Neumann entropy in the diagonalization limit. The condition of no production of entropy under unitary evolution suggests the definition of a mode temperature that would correspond to the thermal temperature is some appropriate limit.
We show a finite-time Otto-like quantum thermodynamic cycle that preserves the adiabatic population structure of a time-dependent harmonic oscillator in the non-quasi-static regime. In the conventional energy representation, finite-rate driving induces non-adiabatic population redistribution and leaves residual excitations after the Hamiltonian has returned to its initial value. We show that this difficulty can be avoided by formulating the dynamics in the Lewis-Riesenfeld invariant representation, without modifying the physical Hamiltonian through auxiliary counterdiabatic driving. For a parametric Mathieu protocol, quantum inertia produces a mismatch between the spatial width of the working mode and its transient dressed energy scale. We propose an experimental implementation of this scheme in a trapped-ion Paul trap using stimulated Raman interactions, with independent control of the laser detuning and beam intersection angle. This provides a finite-time implementation in which the invariant population structure is preserved while the physical trap frequency evolves non-quasi-statically. Our results establish a clear distinction between adiabatic operation and quasi-static driving, providing a route toward finite-time quantum thermal cycles that retain the adiabatic energy structure without requiring the quasi-static limit.
We study the first law of thermodynamics utilizing a frequency modulated quantum harmonic oscillator. For an adiabatic change in frequency, the temperature of the oscillator is proportional to the frequency. Then, we present a number representing the non-adiabaticity determined by the relation between Ermakov-Lewis-Riesenfeld invariant and hamiltonian. We write the first law of thermodynamics for the oscillator's quantum state having non-adiabaticity and then find the temperature. The temperature gains a non-negative non-adiabaticity correction to the adiabatic temperature. We describe the thermalization process for the oscillator as a differential equation. The equation deals with the evolution of the exponent of the density operator. Finally, we write the first law of thermodynamics for thermalization for the harmonic oscillator.
We study a time-dependent harmonic oscillator based on the dynamics of instantaneous phonons, which have obvious physical meaning and direct experimental relevance. We find simple analytic solutions for an important class of evolution and identify two parameter-changing-rate regimes with qualitatively different oscillator behaviors. We show that rapid adiabatic processes are possible if the frequency and the mass of the oscillator change in opposite directions. The state vector in the Schrödinger picture is handily achieved by use of the eigenstates of the instantaneous phonon operators that are analytically known for arbitrary frequency and mass values.
We investigate the dynamic evolution and thermodynamic process of a driven quantum system immersed in a finite-temperature heat bath. A Born-Markovian quantum master equation is formally derived for the time-dependent system with discrete energy levels. This quantum master equation can be applied to situations with a broad range of driving speeds and bath temperatures and thus be used to study the finite-time quantum thermodynamics even when nonadiabatic transition and dissipation coexist. The dissipative Landau-Zener model is analyzed as an example. The population evolution and transition probability of the model reveal the importance of the competition between driving and dissipation beyond the adiabatic regime. Moreover, local maxima of irreversible entropy production occur at intermediate sweep velocity and finite temperature, which the low-dissipation model cannot describe.
The unavoidable irreversible losses of power in a heat engine are found to be of quantum origin. Following thermodynamic tradition a model quantum heat engine operating by the Otto cycle is analyzed. The working medium of the model is composed of an ensemble of harmonic oscillators. A link is established between the quantum observables and thermodynamical variables based on the concept of canonical invariance. These quantum variables are sufficient to determine the state of the system and with it all thermodynamical variables. Conditions for optimal work, power and entropy production show that maximum power is a compromise between the quasistatic limit of adiabatic following on the compression and expansion branches and a sudden limit of very short time allocation to these branches. At high temperatures and quasistatic operating conditions the efficiency at maximum power coincides with the endoreversible result. The optimal compression ratio varies from the square root of the temperature ratio in the quasistatic limit where their reversibility is dominated by heat conductance to the temperature ratio to the power of 1/4 in the sudden limit when the irreversibility is dominated by friction. When the engine deviates from adiabatic conditions the performance is subject to friction. The origin of this friction can be traced to the noncommutability of the kinetic and potential energy of the working medium.
We study a quantum harmonic oscillator undergoing thermalization. To describe the thermalization process, we generalize the Ermakov-Lewis-Riesenfeld (ELR) invariant method for the oscillator. After imposing appropriate conditions on the thermalization process, we introduce an ansatz equation that describes the time evolution effectively. We write down the first law for thermalization in the same form as that for ordinary thermodynamics. Here, the thermalization effect appears through a change of the ELR frequency. Finally, we obtain the oscillator's energy undergoing thermalization as a function of entropy and its time derivative.