scholarly journals A PATH INTEGRAL FOR CLASSICAL DYNAMICS, ENTANGLEMENT, AND JAYNES-CUMMINGS MODEL AT THE QUANTUM-CLASSICAL DIVIDE

2011 ◽  
Vol 09 (supp01) ◽  
pp. 203-224 ◽  
Author(s):  
HANS-THOMAS ELZE ◽  
GIOVANNI GAMBAROTTA ◽  
FABIO VALLONE

The Liouville equation differs from the von Neumann equation "only" by a characteristic superoperator. We demonstrate this for Hamiltonian dynamics, in general, and for the Jaynes-Cummings model, in particular. Employing superspace (instead of Hilbert space), we describe time evolution of density matrices in terms of path integrals, which are formally identical for quantum and classical mechanics. They only differ by the interaction contributing to the action. This allows us to import tools developed for Feynman path integrals, in order to deal with superoperators instead of quantum mechanical commutators in real time evolution. Perturbation theory is derived. Besides applications in classical statistical physics, the "classical path integral" and the parallel study of classical and quantum evolution indicate new aspects of (dynamically assisted) entanglement (generation). Our findings suggest to distinguish intra- from inter-space entanglement.

2020 ◽  
Vol 75 (2) ◽  
pp. 131-141 ◽  
Author(s):  
Bhavya Bhatt ◽  
Manish Ram Chander ◽  
Raj Patil ◽  
Ruchira Mishra ◽  
Shlok Nahar ◽  
...  

AbstractThe measurement problem and the absence of macroscopic superposition are two foundational problems of quantum mechanics today. One possible solution is to consider the Ghirardi–Rimini–Weber (GRW) model of spontaneous localisation. Here, we describe how spontaneous localisation modifies the path integral formulation of density matrix evolution in quantum mechanics. We provide two new pedagogical derivations of the GRW propagator. We then show how the von Neumann equation and the Liouville equation for the density matrix arise in the quantum and classical limit, respectively, from the GRW path integral.


2000 ◽  
Vol 14 (03) ◽  
pp. 73-78 ◽  
Author(s):  
LUIZ C. L. BOTELHO

We show that Nelson's stochastic mechanics suitably formulated as a Hamilton–Jacobi first-order equation leads straightforwardly to the Feynman path integral formulation of quantum mechanics.


2019 ◽  
Vol 32 (01) ◽  
pp. 2050003 ◽  
Author(s):  
Wataru Ichinose

The Feynman path integrals for the magnetic Schrödinger equations are defined mathematically, in particular, with polynomially growing potentials in the spatial direction. For example, we can handle electromagnetic potentials [Formula: see text] such that [Formula: see text] “a polynomial of degree [Formula: see text] in [Formula: see text]” [Formula: see text] and [Formula: see text] are polynomials of degree [Formula: see text] in [Formula: see text]. The Feynman path integrals are defined as [Formula: see text]-valued continuous functions with respect to the time variable.


2001 ◽  
Vol 15 (15) ◽  
pp. 2107-2113 ◽  
Author(s):  
MICHAEL STONE

I consider the time evolution of generalized coherent states based on non-standard fiducial vectors, and show that only for a restricted class of such vectors does the associated classical motion determine the quantum evolution of the states. I discuss some consequences of this for path integral representations.


1992 ◽  
Vol 07 (supp01a) ◽  
pp. 377-390 ◽  
Author(s):  
Takashi HASHIMOTO ◽  
Kazunori OGURA ◽  
Kiyosato OKAMOTO ◽  
Ryuichi SAWAE

Path integrals with Hamiltonians on coadjoint orbits of SU(2) and SU(1,1) are explicitly calculated, taking the operator ordering into account. The path integral gives the kernel function of the unitary operator of the representation which is constructed by the method of Kirillov-Kostant theory.


1976 ◽  
Vol 28 (3) ◽  
pp. 793-805 ◽  
Author(s):  
V. P. Maslov ◽  
A. M. Chebotarev

2011 ◽  
Vol 42 (2) ◽  
pp. 319-339 ◽  
Author(s):  
Domagoj Kuić ◽  
Paško Županović ◽  
Davor Juretić

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