Diffusion Process Representations for a Scalar-Field Schrödinger Equation Solution in Rotating Coordinates

Author(s):  
William M. McEneaney ◽  
Ruobing Zhao
1998 ◽  
Vol 503 (1) ◽  
pp. 446-449 ◽  
Author(s):  
G. P. Malik ◽  
Raman Kumar Jha ◽  
Vijaya S. Varma

2012 ◽  
Vol 12 (2) ◽  
Author(s):  
Gilles Evéquoz ◽  
Tobias Weth

AbstractWe consider the stationary semilinear Schrödinger equation−Δu + a(x)u = f (x, u), u ∈ Hwhere a and f are continuous functions converging to some limits a


2019 ◽  
Vol 16 (02) ◽  
pp. 1950017 ◽  
Author(s):  
I. V. Kanatchikov

The functional Schrödinger representation of a scalar field on an [Formula: see text]-dimensional static space-time background is argued to be a singular limiting case of the hypercomplex quantum theory of the same system obtained by the precanonical quantization based on the space-time symmetric De Donder–Weyl Hamiltonian theory. The functional Schrödinger representation emerges from the precanonical quantization when the ultraviolet parameter [Formula: see text] introduced by precanonical quantization is replaced by [Formula: see text], where [Formula: see text] is the time-like tangent space Dirac matrix and [Formula: see text] is an invariant spatial [Formula: see text]-dimensional Dirac’s delta function whose regularized value at [Formula: see text] is identified with the cutoff of the volume of the momentum space. In this limiting case, the Schrödinger wave functional is expressed as the trace of the product integral of Clifford-algebra-valued precanonical wave functions restricted to a certain field configuration and the canonical functional derivative Schrödinger equation is derived from the manifestly covariant Dirac-like precanonical Schrödinger equation which is independent of a choice of a codimension-one foliation.


1999 ◽  
Vol 82 (20) ◽  
pp. 3976-3979 ◽  
Author(s):  
D. R. Schultz ◽  
M. R. Strayer ◽  
J. C. Wells

1995 ◽  
Vol 10 (15) ◽  
pp. 2231-2240 ◽  
Author(s):  
ABHIK KUMAR SANYAL

Semiclassical approximation to the Wheeler-DeWitt equation which corresponds to gravity with a nonminimally coupled scalar field is carried out. To the leading order, the vacuum Einstein equation, along with the functional Schrödinger equation for the matter field propagating in the background of classical curved space, is obtained. The Schrödinger equation is solved for a quartic potential. It is observed that the wave functional admits the wormhole boundary condition even for large negative values of the coupling constant ∊. For conformal coupling, ∊=1/6, the Hawking-Page wormhole solution is recovered.


Symmetry ◽  
2020 ◽  
Vol 12 (6) ◽  
pp. 943
Author(s):  
Philip Broadbridge ◽  
Kathryn Deutscher

For a scalar field in an exponentially expanding universe, constituent modes of elementary excitation become unstable consecutively at shorter wavelength. After canonical quantization, a Bogoliubov transformation reduces the minimally coupled scalar field to independent 1D modes of two inequivalent types, leading eventually to a cosmological partitioning of energy. Due to accelerated expansion of the coupled space-time, each underlying mode transits from an attractive oscillator with discrete energy spectrum to a repulsive unit with continuous unbounded energy spectrum. The underlying non-autonomous Schrödinger equation is solved here as the wave function evolves through the attraction-repulsion transition and ceases to oscillate.


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