Results 161 to 170 of about 6,172 (209)
Modeling Strong Light-Matter Coupling in Correlated Systems: State-Averaged Cavity Quantum Electrodynamics Complete Active Space Self-Consistent Field Theory. [PDF]
Vu N +5 more
europepmc +1 more source
A note on spontaneous symmetry breaking in the mean-field Bose gas. [PDF]
Deuchert A, Nam PT, Napiórkowski M.
europepmc +1 more source
Selected Configuration Interaction Using Time-Evolved Population Statistics. [PDF]
Weaving T +3 more
europepmc +1 more source
Some of the next articles are maybe not open access.
Related searches:
Related searches:
Toeplitz Operators on the Fock Space
Integral Equations and Operator Theory, 2010For positive parameter \(\alpha\), consider the measure \( d \lambda_{\alpha}(z)=\frac{\alpha}{\pi}e^{-\alpha|z|^{2}}dA(z) \) on the complex plane \(\mathbb C\), where \(dA(z)\) is the ordinary area measure. The Fock space \(F_{\alpha}^{2}\) is the subspace (with inherited norm) of all entire functions in \(L^{2}({\mathbb C},d\lambda_{\alpha})\).
Kehe Zhu, Josh Isralowitz, Zhu Kehe
exaly +2 more sources
HANKEL MEASURES FOR FOCK SPACE
Bulletin of the Australian Mathematical Society, 2022AbstractInspired by Xiao’s work on Hankel measures for Hardy and Bergman spaces [‘Pseudo-Carleson measures for weighted Bergman spaces’. Michigan Math. J.47 (2000), 447–452], we introduce Hankel measures for Fock space $F^p_\alpha $ . Given $p\ge 1$ , we obtain several equivalent descriptions for such measures on $F^p_\alpha $ .
openaire +2 more sources
1993
The preceding chapters dealt with the non-commutative analogues of discrete r.v.’s, then of real valued r.v.’s, and we now begin to discuss stochastic processes. We start with the description of Fock space (symmetric and antisymmetric) as it is usually given in physics books.
openaire +1 more source
The preceding chapters dealt with the non-commutative analogues of discrete r.v.’s, then of real valued r.v.’s, and we now begin to discuss stochastic processes. We start with the description of Fock space (symmetric and antisymmetric) as it is usually given in physics books.
openaire +1 more source
1984
We describe a Monte-Carlo algorithm to solve exactly the ground-state problem for a system of up to four nucleons interacting via a scalar neutral meson field. The mesonic degrees of freedom are treated exactly without recourse to the potential approximation.
L. Szybisz, John G. Zabolitzky
openaire +1 more source
We describe a Monte-Carlo algorithm to solve exactly the ground-state problem for a system of up to four nucleons interacting via a scalar neutral meson field. The mesonic degrees of freedom are treated exactly without recourse to the potential approximation.
L. Szybisz, John G. Zabolitzky
openaire +1 more source
FRACTIONAL FOCK–SOBOLEV SPACES
Nagoya Mathematical Journal, 2018Let $s\in \mathbb{R}$ and $0<p\leqslant \infty$. The fractional Fock–Sobolev spaces $F_{\mathscr{R}}^{s,p}$ are introduced through the fractional radial derivatives $\mathscr{R}^{s/2}$. We describe explicitly the reproducing kernels for the fractional Fock–Sobolev spaces $F_{\mathscr{R}}^{s,2}$ and then get the pointwise size estimate of the ...
Cho, Hong Rae, Park, Soohyun
openaire +2 more sources
Linear Operators on Fock Spaces
Integral Equations and Operator Theory, 2017The aim of this paper is to extend several results about properties of some linear operators on the Fock space \(F_\alpha^2\) to linear operators on Fock spaces \(F_\alpha^p\) for ...
Lou, Zengjian, Zhu, Kehe, Zhu, Senhua
openaire +1 more source
Fock Space and the Poisson Process
Proceedings of the London Mathematical Society, 2004The authors show that for any regular self-adjoint quantum semimartingale \((J_t)_{0\leq t\leq1}\) the essentially self-adjoint quantum semimartingale \((\hat M_t+J_t)_{0\leq t\leq1}\) satisfies the quantum Itô formula. Here \(\hat M_t\) is the operator corresponding to multiplication by the integral of a real, bounded, predictable process with respect
Pathmanathan, S., Vincent-Smith, G. F.
openaire +2 more sources

