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APL Quantum

Ebers–Moll model inspired equivalent circuit for quantum thermal transistors

Anuradhi Rajapaksha, Sarath D. Gunapala, Malin Premaratne

Published May 13, 2025• 4 citations
Publisher

Abstract

The widespread success of electronic transistors is partly due to their ability to be modeled using equivalent circuits, which not only enables detailed analysis and efficient design but also provides greater insight for designers, facilitating the development of complex electronic systems. The Ebers–Moll model, for example, is a widely used large-signal equivalent circuit that replicates the operational characteristics of bipolar junction transistors. Similar to electronic transistors, research on quantum thermal transistors has gained considerable attention in recent years; however, minimal focus has been placed on developing equivalent circuit representations. Drawing inspiration from equivalent models of electronic transistors, our study proposes an equivalent model for a quantum thermal transistor built on a strongly coupled qubit–qutrit–qubit architecture. This configuration allows replication of its transistor behavior using a diode-based equivalent model, leveraging its property of splitting the qutrit into two individual qubits. The proposed quantum thermal diode-based equivalent model closely mirrors the diode-based representation of an electronic transistor. Using frameworks of open quantum systems and the quantum Markovian master equation, along with the Born approximation and rotating wave approximation, we conduct a comprehensive analysis and comparison of our quantum thermal diode-based equivalent model with an established quantum thermal transistor model. Furthermore, we discuss the intrinsic internal coupling between the two diodes and determine the optimum coupling strength necessary for efficient heat amplification. This equivalent model provides greater insight into the analysis of quantum thermal transistors and significantly contributes to the advancement of nanoscale thermal circuit designs.

DOI
10.1063/5.0270456

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The widespread success of electronic transistors is partly due to their ability to be modeled using equivalent circuits, which not only enables detailed analysis and efficient design but also provides greater insight for designers, facilitating the development of complex electronic systems. The Ebers–Moll model, for example, is a widely used large-signal equivalent circuit that replicates the operational characteristics of bipolar junction transistors. Similar to electronic transistors, research on quantum thermal transistors has gained considerable attention in recent years; however, minimal focus has been placed on developing equivalent circuit representations. Drawing inspiration from equivalent models of electronic transistors, our study proposes an equivalent model for a quantum thermal transistor built on a strongly coupled qubit–qutrit–qubit architecture. This configuration allows replication of its transistor behavior using a diode-based equivalent model, leveraging its property of splitting the qutrit into two individual qubits. The proposed quantum thermal diode-based equivalent model closely mirrors the diode-based representation of an electronic transistor. Using frameworks of open quantum systems and the quantum Markovian master equation, along with the Born approximation and rotating wave approximation, we conduct a comprehensive analysis and comparison of our quantum thermal diode-based equivalent model with an established quantum thermal transistor model. Furthermore, we discuss the intrinsic internal coupling between the two diodes and determine the optimum coupling strength necessary for efficient heat amplification. This equivalent model provides greater insight into the analysis of quantum thermal transistors and significantly contributes to the advancement of nanoscale thermal circuit designs.
We present a quantum thermal diode model based on a coupled qutrit–qubit system designed to control heat flow between two thermal baths with unprecedented efficiency. This differs from previous models in terms of the asymmetry introduced by spin particles and their interaction. By exploiting the interactions between degenerate states within the coupled qutrit–qubit system, our model demonstrates diode-like behavior that is both robust and energy-efficient. Utilizing the frameworks of open quantum systems and the quantum Markovian master equation, with the Born and rotating wave approximations, we comprehensively analyze the system’s behavior. Numerical simulations reveal significant thermal rectification across a wide temperature range, positioning our model as a groundbreaking solution for nanoscale heat management. In addition, we employ state transition diagrams to elucidate the transition rate characteristics that underpin the diode behavior. Finally, we explore the potential for physical implementation using superconducting circuits, highlighting the practical relevance of our design.
Abstract We investigate the performance of a three-qubits quantum thermal transistor using coarse-graining, global, and local master equations, respectively. Special attention is paid to the validity of the three methods in different internal coupling strengths. The effects of system and bath parameters on the amplification effect are studied. It is found that small middle qubit frequency, weak internal coupling, and symmetric configuration of system-bath coupling lead to large amplification factor. The heat current amplification mechanism is discussed and quantum coherence does not contribute to amplification. Besides, the thermal transistor is realized by tuning the temperature of the middle bath, the temperature of the left bath, or the internal coupling strength.
A quantum thermal transistor is designed by the strong coupling between one qubit and one qutrit which are in contact with three heat baths with different temperatures. The thermal behavior is analyzed based on the master equation by both the numerical and the approximately analytic methods. It is shown that the thermal transistor, as a three-terminal device, allows a weak modulation heat current (at the modulation terminal) to switch on and off and effectively modulate the heat current between the other two terminals. In particular, the weak modulation heat current can induce the strong heat current between the other two terminals with the multiple-region amplification of heat current. Furthermore, the heat currents are quite robust to the temperature (current) fluctuation at the lower-temperature terminal within a certain range of temperature, and so it can behave as a heat current stabilizer.
Quantum heat transport governs energy exchange processes and statistical laws in non-equilibrium quantum systems, and plays a pivotal role in quantum thermodynamics. We investigate the steady-state thermal transport of a noncommuting coupled spin system. We employ the quantum dressed master equation approach within the framework of open quantum system theory to accurately analyze the non-equilibrium dynamics, ensuring the validity of transport results in the strong coupling regime. Our results demonstrate that noncommuting spin coupling serves as a significant resource for modulating the nonlinearity of the heat current. Specifically, in the weak spin-coupling regime, the system exhibits robust negative differential thermal conductance (NDTC) across various spin numbers. By deriving analytical expressions for the heat current in both the single-spin and large-spin limits, we reveal that this NDTC behavior is governed by microscopic cycle fluxes. Physically, this arises because spin excitation channels induced by the cold reservoir are suppressed under a large temperature bias, thereby blocking energy exchange cycles. Conversely, in the strong spin-coupling and large temperature bias regime, the quantum system demonstrates pronounced thermal rectification. This high rectification efficiency originates from the unidirectional saturation of the heat current, rendering the system a promising candidate for high-performance thermal diodes. Furthermore, we extend the model to a three-terminal configuration to construct a quantum thermal transistor. By manipulating the temperature of the gate reservoir, we achieve efficient modulation and amplification of heat flow between the source and drain. The heat amplification factor is shown to far exceed unity in specific operating regions, confirming significant thermal amplification.
Precisely controlling heat transfer in a quantum mechanical system is particularly significant for designing quantum thermodynamical devices. With the technology of experiment advances, circuit quantum electrodynamics (circuit QED) has become a promising system due to controllable light-matter interactions as well as flexible coupling strengths. In this paper, we design a thermal diode in terms of the two-photon Rabi model of the circuit QED system. We find that the thermal diode can not only be realized in the resonant coupling but also achieve better performance, especially for the detuned qubit-photon ultrastrong coupling. We also study the photonic detection rates and their nonreciprocity, which indicate similar behaviors with the nonreciprocal heat transport. This provides the potential to understand thermal diode behavior from the quantum optical perspective and could shed new insight into the relevant research on thermodynamical devices.
In recent years, integrating quantum feedback mechanisms into thermal machines has gained attention due to its benefits in manipulating the system states and energy flows. This is particularly advantageous for quantum thermal transistors in preserving their inherent quantum properties as they lose the purity of the system states due to decoherence and relaxation from interactions with thermal baths, within the subsystems, and monitoring. In the literature, studies have demonstrated that preserving quantum coherence can enhance the performance of quantum thermal machines, improving their efficiency. In our paper, we present a model that proposes engineering baths to be equipped with detectors and a controller to enable feedback in a quantum thermal transistor that emulates a role played by a feedback resistor in an electronic transistor. We use the framework of quantum feedback control via weak monitoring. We modify the system evolution trajectories by using a weak monitoring record from a detector. By taking the ensemble average of these trajectories, we unveil the evolution of the system density matrix that corresponds to the Markovian dynamics of the transistor. This type of feedback introduces minimal perturbation to the system and, once tuned, enhances the system coherence that would otherwise degrade due to bath interactions. Furthermore, there will be no change in the relaxation times. The probabilities of population terms remain unchanged. We treat this an enhancement in the operational characteristics of the quantum thermal transistor as it maintains its quantum features with an added benefit of improved amplification capabilities.