We present a complete derivation of the semiclassical limit of the coherent-state propagator in one dimension, starting from path integrals in phase space. We show that the arbitrariness in the path integral representation, which follows from the overcompleteness of the coherent states, results in many different semiclassical limits. We explicitly derive two possible semiclassical formulae for the propagator, we suggest a third one, and we discuss their relationships. We also derive an initial-value representation for the semiclassical propagator, based on an initial Gaussian wavepacket. It turns out to be related to, but different from, Heller's thawed Gaussian approximation. It is very different from the Herman-Kluk formula, which is not ...
We propose a conjugate application of the Bargmann representation of quantum mechanics. Applying the...
We derive the semiclassical limit of the coherent state propagator for systems with two degrees of f...
We determine the semiclassical coherent-state propagator for a particle going through one-dimensiona...
The semiclassical formula for the quantum propagator in the coherent state representation is not fr...
In this work, we derived a semiclassical approximation for the matrix elements of a quantum propagat...
We compute the semiclassical coherent-state propagator for a particle moving in a one-dimensional bo...
We construct a representation of the coherent state path integral using the Weyl symbol of the Hamil...
A semiclassical formula for the coherent-state propagator requires the determination of specific cla...
AbstractThe semiclassical formula for the coherent-state propagator is written in terms of complex c...
The semiclassical limit of the coherent state propagator involves complex classical trajectories of...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
By returning to the underlying discrete time formalism, we relate spurious results in coherent state...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
We derive the semiclassical limit of the coherent state propagator for systems with two degrees of f...
We propose a conjugate application of the Bargmann representation of quantum mechanics. Applying the...
We propose a conjugate application of the Bargmann representation of quantum mechanics. Applying the...
We derive the semiclassical limit of the coherent state propagator for systems with two degrees of f...
We determine the semiclassical coherent-state propagator for a particle going through one-dimensiona...
The semiclassical formula for the quantum propagator in the coherent state representation is not fr...
In this work, we derived a semiclassical approximation for the matrix elements of a quantum propagat...
We compute the semiclassical coherent-state propagator for a particle moving in a one-dimensional bo...
We construct a representation of the coherent state path integral using the Weyl symbol of the Hamil...
A semiclassical formula for the coherent-state propagator requires the determination of specific cla...
AbstractThe semiclassical formula for the coherent-state propagator is written in terms of complex c...
The semiclassical limit of the coherent state propagator involves complex classical trajectories of...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
By returning to the underlying discrete time formalism, we relate spurious results in coherent state...
The overcompleteness of the coherent states basis leads to a multiplicity of representations of Feyn...
We derive the semiclassical limit of the coherent state propagator for systems with two degrees of f...
We propose a conjugate application of the Bargmann representation of quantum mechanics. Applying the...
We propose a conjugate application of the Bargmann representation of quantum mechanics. Applying the...
We derive the semiclassical limit of the coherent state propagator for systems with two degrees of f...
We determine the semiclassical coherent-state propagator for a particle going through one-dimensiona...