2021
DOI: 10.1007/s11128-021-03019-x
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Coupled two-qubit engine and refrigerator in Heisenberg model

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Cited by 13 publications
(9 citation statements)
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“…Here we consider a system consisting of two interacting qubits a and b as the working material a four- level quantum Otto engine, which is described by XY Hamiltonian considering the spin-orbit interaction and magnetic field 35 : where denotes the Pauli operators that affect the qubits , and are the strength of the antiferromagnetic couplings, B is the intensity of the magnetic field, and D is the spin-orbit interaction factor. We set and assume that the dynamics of the working matter density operator have the Markovian property, and can be stated by Lindblad master equation as follows 36 : Accordingly, and is the jump operator that describes the operation of the baths, and is the dissipation rate associated with the Lindblad term in the above equation.…”
Section: Model System: the Quantum Otto Enginementioning
confidence: 99%
“…Here we consider a system consisting of two interacting qubits a and b as the working material a four- level quantum Otto engine, which is described by XY Hamiltonian considering the spin-orbit interaction and magnetic field 35 : where denotes the Pauli operators that affect the qubits , and are the strength of the antiferromagnetic couplings, B is the intensity of the magnetic field, and D is the spin-orbit interaction factor. We set and assume that the dynamics of the working matter density operator have the Markovian property, and can be stated by Lindblad master equation as follows 36 : Accordingly, and is the jump operator that describes the operation of the baths, and is the dissipation rate associated with the Lindblad term in the above equation.…”
Section: Model System: the Quantum Otto Enginementioning
confidence: 99%
“…Here we consider a system consisting of two interacting qubits a and b as the working material a four-level quantum Otto engine, which is described by XY Hamiltonian considering the spin-orbit interaction and magnetic field [37]:…”
Section: Model System: the Quantum Otto Enginementioning
confidence: 99%
“…[50][51][52] when a thermal bath being replaced by a quantum measurement as a new source of heat, in Ref. [53][54][55] the role of Dzyaloshinski-Moriya interaction, in Ref. [56] the authors examine the performance of a two-coupled spins of arbitrary magnitudes (where majorization [57] has been used to find the upper bound of efficiency, which was an open question to be answered), and last but not least, the role of non-adiabaticity (i.e., when the unitary strokes are done in finite time) for one spin and two coupled spin-1/2 particles [58][59][60][61][62].…”
Section: Introductionmentioning
confidence: 99%
“…We show that they shift the advantage in COP to large values of Γ z . When the system is working as a refrigerator, it has been studied in [55,72], but in contrast to them, we explore the role of idel levels as well as the role of increasing the number of interacting spins on the COP, two situations that have not been explored there. Moreover, taking advantage of this model, we point out a flaw in [47], by showing that it is not necessary to change both the external magnetic field and the coupling parameters to break the extensive property of the global extractable work.…”
Section: Introductionmentioning
confidence: 99%