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arXiv:2610.32610

Optimizing Quantum Battery via Counterdiabatic driving

F. Ahmadi, S. Salimi

quant-phSubmitted Oct 23, 2026• Announced Oct 26, 2026• 0 citations
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Abstract

We analyze the energy charging of a quantum battery within an open quantum framework, where the interaction between the battery element and an external power source is mediated by an ancilla system acting as a controllable switch. Specifically, we investigate the charging and discharging dynamics of a cavity-based quantum battery coupled to a driven qubit functioning as the charger. To ensure lossless power transfer, we utilize an adiabatic evolution protocol. Furthermore, we implement counterdiabatic driving, achieved by applying an auxiliary control field to the original Hamiltonian, to suppress undesired transitions and realize fast adiabatic dynamics. This scheme significantly accelerates the charging process. We demonstrate that the charging efficiency under adiabatic evolution is enhanced and exhibits stable, non-oscillatory behavior, and we determine the optimal duration for the operation. Finally, we show that counterdiabatic driving minimizes the path length between the initial and final states, inducing the shortest possible evolution distance.

AI Summary

The paper studies whether counterdiabatic (CD) control can accelerate charging of a lossy cavity quantum battery while retaining the smooth trajectory of slow driving. Its circuit-QED model comprises a classical microwave source, a dispersively coupled qubit mediator, and a storage cavity. Eliminating the qubit gives a linearly driven harmonic oscillator with zero-temperature photon loss at rate $\kappa$. Starting from vacuum, the reduced model remains in a pure coherent state. Charging therefore reduces to solving a linear equation for its amplitude, with stored energy and ergotropy both equal to $\hbar\omega_a|\alpha|^2$. Analytical solutions compare constant driving, a smooth $\sin^2$ ramp, and a CD-assisted ramp. The auxiliary complex envelope $\Omega_{\rm cd}=\dot\Omega/(i\omega_{\rm eff}+\kappa/2)$ enforces exact tracking of the instantaneous steady-state amplitude, suppressing transient oscillations at finite charging times. Using integrated squared drive amplitude as a control-cost metric, the paper obtains reference and auxiliary costs proportional to $t_f$ and $1/t_f$, respectively. Their sum is minimized at $t_f^{\rm opt}=\pi/(\sqrt{3}|i\omega_{\rm eff}+\kappa/2|)$, approximately $1.21$ ns for one parameter choice. It also reports near-unit geometric efficiency for CD trajectories. After switch-off, energy and ergotropy decay as $e^{-\kappa(t-t_f)}$; CD control does not improve retention lifetime. The analysis assumes dispersive qubit elimination, negligible thermal occupation, and Markovian cavity loss. Arbitrarily fast tracking requires diverging auxiliary-field fluence, limiting practical speed; the geometric and charging comparisons are established within this effective oscillator model.

Likely largely AI-generatedOverclaimsIncrementalMissing comparisonPossible error

Central claim may not hold: The CD trajectory minimizes length within the coherent-state manifold but does not attain the paper's full-state-space geodesic distance or establish quantum-speed-limit saturation, and Hamiltonian variance alone is not the speed of its dissipative trajectory. The displayed explicit CD ramp pulse omits the finite-damping correction required by the paper's exact tracking formula and is valid only approximately in the weak-damping regime. The quoted optimal-duration example uses parameters different from the circuit-QED table, whose values instead predict approximately 0.579 ns. The total fluence omits a finite-damping interference contribution of kappa Omega_0^2/(2|gamma_eff|^2), affecting the reported cost and efficiency but not the unconstrained minimizing duration. The abstract's lossless-transfer assertion contradicts the positive charging losses in the dissipative model; full extractability of the remaining energy does not imply lossless transfer.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
9 pages, 6 figures

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We analyze the energy charging of a quantum battery within an open quantum framework, where the interaction between the battery element and an external power source is mediated by an ancilla system acting as a controllable switch. Specifically, we investigate the charging and discharging dynamics of a cavity-based quantum battery coupled to a driven qubit functioning as the charger. To ensure lossless power transfer, we utilize an adiabatic evolution protocol. Furthermore, we implement counterdiabatic driving, achieved by applying an auxiliary control field to the original Hamiltonian, to suppress undesired transitions and realize fast adiabatic dynamics. This scheme significantly accelerates the charging process. We demonstrate that the charging efficiency under adiabatic evolution is enhanced and exhibits stable, non-oscillatory behavior, and we determine the optimal duration for the operation. Finally, we show that counterdiabatic driving minimizes the path length between the initial and final states, inducing the shortest possible evolution distance.
The paper studies whether counterdiabatic (CD) control can accelerate charging of a lossy cavity quantum battery while retaining the smooth trajectory of slow driving. Its circuit-QED model comprises a classical microwave source, a dispersively coupled qubit mediator, and a storage cavity. Eliminating the qubit gives a linearly driven harmonic oscillator with zero-temperature photon loss at rate κ\kappaκ.
Starting from vacuum, the reduced model remains in a pure coherent state. Charging therefore reduces to solving a linear equation for its amplitude, with stored energy and ergotropy both equal to ℏωa∣α∣2\hbar\omega_a|\alpha|^2ℏωa​∣α∣2. Analytical solutions compare constant driving, a smooth sin⁡2\sin^2sin2 ramp, and a CD-assisted ramp. The auxiliary complex envelope Ωcd=Ω˙/(iωeff+κ/2)\Omega_{\rm cd}=\dot\Omega/(i\omega_{\rm eff}+\kappa/2)Ωcd​=Ω˙/(iωeff​+κ/2) enforces exact tracking of the instantaneous steady-state amplitude, suppressing transient oscillations at finite charging times.
Using integrated squared drive amplitude as a control-cost metric, the paper obtains reference and auxiliary costs proportional to tft_ftf​ and 1/tf1/t_f1/tf​, respectively. Their sum is minimized at tfopt=π/(3∣iωeff+κ/2∣)t_f^{\rm opt}=\pi/(\sqrt{3}|i\omega_{\rm eff}+\kappa/2|)tfopt​=π/(3​∣iωeff​+κ/2∣), approximately 1.211.211.21 ns for one parameter choice. It also reports near-unit geometric efficiency for CD trajectories. After switch-off, energy and ergotropy decay as e−κ(t−tf)e^{-\kappa(t-t_f)}e−κ(t−tf​); CD control does not improve retention lifetime.
The analysis assumes dispersive qubit elimination, negligible thermal occupation, and Markovian cavity loss. Arbitrarily fast tracking requires diverging auxiliary-field fluence, limiting practical speed; the geometric and charging comparisons are established within this effective oscillator model.
Quantum batteries are energy storage devices that satisfy quantum mechanical principles. How to improve the battery’s performance such as stored energy and power is a crucial element in the quantum battery. Here, we investigate the charging and discharging dynamics of a three-level counterdiabatic stimulated Raman adiabatic passage quantum battery via shortcuts to adiabaticity, which can compensate for undesired transitions to realize a fast adiabatic evolution through the application of an additional control field to an initial Hamiltonian. The scheme can significantly speed up the charging and discharging processes of a three-level quantum battery and obtain more stored energy and higher power compared with the original stimulated Raman adiabatic passage. We explore the effect of both the amplitude and the delay time of driving fields on the performances of the quantum battery. Possible experimental implementation in superconducting circuit and nitrogen-vacancy center is also discussed.
Abstract Quantum control allows us to address the problem of engineering quantum dynamics for special purposes. While recently the field of quantum batteries has attracted much attention, optimization of their charging has not benefited from the quantum control methods. Here we fill this gap by using an optimization method. We apply for the first time the convergent iterative method for the control of the population of a bipartite quantum system in two cases, starting with a qubit-qubit case. The quantum charger-battery system is considered here, where the energy is pumped into the charger by an external classical electromagnetic field. Secondly, we systematically extend our investigation to a second case involving two harmonic oscillators in the Gaussian regime, presenting an original formulation of the method. In both cases, the charger is considered to be an open dissipative system, as its interaction with the drive may require a more pronounced exposure to general interaction with environment. A key consideration in our optimization strategy is the practical concern of turning the charging external field on and off. We find that optimizing the pulse shape yields a substantial enhancement in both the power and efficiency of the charging process compared to a sinusoidal drive. The harmonic oscillator configuration of quantum batteries is particularly intriguing, as the optimal driving pulse remains effective regardless of the environmental temperature. This study introduces a novel approach to quantum battery charging optimization, opening avenues for enhanced performance in real-world applications.
Although implementing shortcuts to adiabaticity (STA) in open quantum systems remains challenging due to the complex control schemes required for such systems, their powerful ability to rapidly steer the system toward target states and their widespread applicability in quantum technologies have motivated us to explore their potential in quantum energy storage. In this work, we employ STA techniques to charge an open quantum battery and demonstrate that the extractable work (Ergotropy) from such a battery can be significantly enhanced by several times compared to the case where the battery is charged using a time independent driving field. Our results pave the way for accelerating the dynamics of open quantum systems and suggest promising applications in the development of high-performance, stable quantum batteries.
We discuss a one-dimensional coupled qubit-array quantum battery model under Born-Karman boundary conditions and investigate both the charging and discharging processes. Applying the stored energy, charging power, and ergotropy as the essential physical indicators of quantum battery, it is observed that minimizing the hopping interaction between the nearest-neighbor qubits in the qubit-array and increasing the number of qubits during battery setup are crucial. Additionally, we employ a classical driving field to optimize battery performance and explore the optimal quantum battery performance by adjusting the driving strength of the classical field. Finally, we have discovered that the initial energy in the charger no longer needs to be higher than the energy in the battery in our protocol, the charger will continue to supply energy to the battery even when there is limited initial available energy in the charger. And the conventional approach of preparing the battery's initial state in its ground state, as observed in previous studies, may not necessarily be the optimal choice. By introducing a strong classical driving field, it is possible to enhance energy storage by allowing for an initial presence of some energy within the battery.
Charger-mediated quantum batteries offer promising opportunities for efficient energy transfer and storage at the quantum level, with potential advantages beyond their classical counterparts. Here, we theoretically demonstrate that nonlinear charger-battery interactions can substantially accelerate the charging of quantum batteries. In the weak-driving regime, sufficiently strong nonlinear coupling can dominate over the effect of dephasing and significantly reduce the charging time. In the strong- and optimal-driving regimes, where the optimal driving strength maximizes the steady-state ergotropy in the linear-coupling regime, nonlinear coupling gives rise to a new optimum in the charging time beyond that of the linear-coupling regime, accompanied by nearly critically damped dynamics. Remarkably, even in the absence of external driving, nonlinear coupling alone can substantially reduce the charging time, providing an alternative route toward fast battery charging. Our results establish nonlinear charger-battery coupling as an effective resource for accelerating quantum-battery charging and broaden the scope of interaction-enabled quantum advantages in energy transfer and storage.