Abstract:The utility of classical mechanics to compute the dynamics of decoherence in continuous variable systems, as defined by the time dependence of the system purity, is examined. Its accuracy, in the semiclassical domain, is shown to depend on the nature of the coupling potentials and, less so, on the initial conditions. For a large range of cases, agreement between quantum and classical computations in small systems is shown to be excellent.
We analyze the dynamical generation of entanglement in systems of two interacting spins initially prepared in a product of spin coherent states. For arbitrary time-independent Hamiltonians, we derive a semiclassical expression for the purity of the reduced density matrix as function of time. The final formula, subsidiary to the linear entropy, shows that the short-time dynamics of entanglement depends exclusively on the stability of trajectories governed by the underlying classical Hamiltonian. Also, this semiclassical measure is shown to reproduce the general properties of its quantum counterpart and give the expected result in the large spin limit. The accuracy of the semiclassical formula is further illustrated in a problem of phase exchange for two particles of spin j.
We analyze the dynamical generation of entanglement in systems of two interacting spins initially prepared in a product of spin coherent states. For arbitrary time-independent Hamiltonians, we derive a semiclassical expression for the purity of the reduced density matrix as function of time. The final formula, subsidiary to the linear entropy, shows that the short-time dynamics of entanglement depends exclusively on the stability of trajectories governed by the underlying classical Hamiltonian. Also, this semiclassical measure is shown to reproduce the general properties of its quantum counterpart and give the expected result in the large spin limit. The accuracy of the semiclassical formula is further illustrated in a problem of phase exchange for two particles of spin j.
“…It is through this principle that we are able to establish a connection between the quantum and classical subdivision of observables [Eqs. (15) and (35)], and to define classical analogs of quantum interference contributions. If this principle does not hold then it is possible that quantum and classical interference terms do not correspond to the same physical phenomenon.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…Further, the resulting classical analogues, if they exist, offer alternative perspectives on well established coherent control schemes. Lastly, decoherence effects on laser control could be analyzed from a completely classical perspective [15] and may well offer insight into novel ways to combat it.…”
“…With the breakdown in the statistical independence of the trajectories, this method can capture the quantum effect of the system . Entanglement dynamics in the semiclassical regime has been widely studied, for its importance has been recognized in the context of from the explanation of the quantum‐classical transition and its implications to the measurement problem to the understanding of the nonlocal aspects permeating the Einstein–Podolsky–Rosen debate …”
Section: Introductionmentioning
confidence: 99%
“…With the breakdown in the statistical independence of the trajectories, this method can capture the quantum effect of the system. [11][12][13][14][15][16][17][18][19] Entanglement dynamics in the semiclassical regime has been widely studied, [20][21][22][23] for its importance has been recognized in the context of from the explanation of the quantum-classical transition [24] and its implications to the measurement problem to the understanding of the nonlocal aspects permeating the Einstein-Podolsky-Rosen debate. [3,25] In this article, we investigate quantum tunneling effect in entanglement dynamics in a closed system starting from separable Gauss state using ETMD method.…”
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