2013
DOI: 10.1002/chir.22155
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A Langevin Canonical Approach to the Dynamics of Chiral Systems: Populations and Coherences

Abstract: A canonical framework for chiral two-level systems coupled to a bath of harmonic oscillators is developed to extract, from a stochastic dynamics, the thermodynamic equilibrium values of both the population difference and coherences. The incoherent and coherent tunneling regimes are analyzed for an Ohmic environment in terms of a critical temperature defined by the maximum of the heat capacity. The corresponding numerical results issued from solving a non-linear coupled system of equations are fitted to approxi… Show more

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Cited by 10 publications
(40 citation statements)
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“…In these cases, the time evolution of each individual trajectory is not possible, and a previous stability analysis is mandatory. However, in the stable case, a satisfactory description of population differences and coherences, average energies, and heat capacity have been achieved by running up to 10 4 trajectories (as previously used) [21,22]. The friction coefficient used is finally γ = 0.1 (dimensionless rate), and a canonical (Maxwell-Boltzmann) distribution is assumed, only classical noise being considered.…”
Section: Resultsmentioning
confidence: 99%
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“…In these cases, the time evolution of each individual trajectory is not possible, and a previous stability analysis is mandatory. However, in the stable case, a satisfactory description of population differences and coherences, average energies, and heat capacity have been achieved by running up to 10 4 trajectories (as previously used) [21,22]. The friction coefficient used is finally γ = 0.1 (dimensionless rate), and a canonical (Maxwell-Boltzmann) distribution is assumed, only classical noise being considered.…”
Section: Resultsmentioning
confidence: 99%
“…The average energy in the normalized |Ψ(t) state is given by Ψ|Ĥ|Ψ = −2δ √ 1 − z 2 cos Φ + 2 z ≡ H 0 , where H 0 represents a Hamiltonian function. Furthermore, the Heisenberg equations of motion can be easily derived fromż = −∂H 0 /∂Φ andΦ = ∂H 0 /∂z, leading to the following non-linear coupled equations for an isolated chiral TLS [19][20][21][22]…”
Section: Isolated (Closed) Dynamicsmentioning
confidence: 99%
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“…This work can be considered as a step forward (as a follow‐up of a previous work) into a more complete stochastic dynamical analysis of this open quantum system by focusing on different thermodynamic quantities such as average energies, phase differences, and heat capacities. We are not going to consider here a very important topic about anomalies of the heat capacity and refer the reader to some pertinent works .…”
Section: Introductionmentioning
confidence: 99%