2019
DOI: 10.1088/1367-2630/ab54ac
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Local versus global master equation with common and separate baths: superiority of the global approach in partial secular approximation

Abstract: Open systems of coupled qubits are ubiquitous in quantum physics. Finding a suitable master equation to describe their dynamics is therefore a crucial task that must be addressed with utmost attention. In the recent past, many efforts have been made toward the possibility of employing local master equations, which compute the interaction with the environment neglecting the direct coupling between the qubits, and for this reason may be easier to solve. Here, we provide a detailed derivation of the Markovian mas… Show more

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Cited by 153 publications
(139 citation statements)
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References 97 publications
(231 reference statements)
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“…Assuming weak coupling between the machine and reservoirs and a rapid decay of the reservoirs correlation functions, a master equation in the Lindblad form [64] can be derived within the standard Born-Markov approximation [63]. Furthermore, as the coupling among the three qubits is assumed to be weak (g=E i ), a local approach can be taken such that the dissipative part of the master equation can be calculated neglecting the interqubit coupling, which would only enter in the coherent part of the evolution [65][66][67][68][69]. It is worth mentioning that even if it has been argued that the local approach may lead to violations of the second law in a specific configuration [70], these deviations are so small that fall below the order of magnitude employed to derive the master equation, and then should be simply neglected [71].…”
Section: Master Equation In the Local Approachmentioning
confidence: 99%
See 1 more Smart Citation
“…Assuming weak coupling between the machine and reservoirs and a rapid decay of the reservoirs correlation functions, a master equation in the Lindblad form [64] can be derived within the standard Born-Markov approximation [63]. Furthermore, as the coupling among the three qubits is assumed to be weak (g=E i ), a local approach can be taken such that the dissipative part of the master equation can be calculated neglecting the interqubit coupling, which would only enter in the coherent part of the evolution [65][66][67][68][69]. It is worth mentioning that even if it has been argued that the local approach may lead to violations of the second law in a specific configuration [70], these deviations are so small that fall below the order of magnitude employed to derive the master equation, and then should be simply neglected [71].…”
Section: Master Equation In the Local Approachmentioning
confidence: 99%
“…These assumptions imply that the three environments are not correlated to each other and lead to a Born-Markov master equation where the dissipative part is the sum of three separate contributions, each of them due to one of the three reservoirs. Furthermore, in the limit of g small with respect to the natural energies, a local approach to the master equation can be adopted, which allows one to compute the Lindbladian using local operators [65][66][67][68][69].…”
Section: Appendix a Derivation Of The Master Equationmentioning
confidence: 99%
“…First, it is essential to employ the so-called global approach 13,48,49 to the master equation (i.e., the explicit inclusion of the interaction term in the system Hamiltonian) in the present work because interaction parameters w can be an order of the detuning of single-electron energies. It is worthwhile to note that the crucial importance of using the global approach has recently been pointed out in a number of works especially in the context of its consistency with thermodynamics 13,48,49 . Second, while our estimation on the level spacing δ above holds true for most of the Fock states, it might break down if a part of Fock states exhibit the degeneracy as found in, e.g., the case of the highest-power machines.…”
Section: Methodsmentioning
confidence: 99%
“…More details can be found in Appendix A. With these prescriptions, the state of the two‐qubit system ρS obeys the following master equation under the partial secular approximation [ 54 ] ddtρSfalse(tfalse)=Lfalse[ρS(t)false]=ifalse[HS+HLS,ρS(t)false]+Dfalse[ρS(t)false]where HLS is the Lamb‐shift Hamiltonian which reads HLS=j,k=1,2false(sjkσk+σj+sjkσkσj+false)while scriptD is the dissipator defined as: truerightscriptDfalse[ρSfalse]=leftj,k=1,2γjk()σjρSσk+12false{ρS,σk+σjfalse}left+j,k=1,2γjk()σj+ρSσk12false{ρS,σkσj+false}…”
Section: Modelmentioning
confidence: 99%