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In previous work, a lattice scalar propagator was rigorously defined in $d=1$ flat space and shown to equal the known Klein-Gordon propagator of QFT. This work generalizes this lattice propagator to manifolds whose universal cover is the…

Mathematical Physics · Physics 2023-11-30 Rory O'Dwyer

The method of dimensional recurrences proposed by one of the authors [1,2] is applied to the evaluation of the pentagon-type scalar integral with on-shell external legs and massless internal lines. For the first time, an analytic result…

High Energy Physics - Theory · Physics 2015-05-18 Bernd A. Kniehl , Oleg V. Tarasov

We deal with the asymptotic behaviour for $\lambda\to+\infty$ of the counting function $N_P(\lambda)$ of certain positive selfadjoint operators $P$ with double order $(m,\mu)$, $m,\mu>0$, $m\not=\mu$, defined on a manifold with ends $M$.…

Functional Analysis · Mathematics 2014-06-27 Sandro Coriasco , Lidia Maniccia

We study the structure of the gauge propagators of a 3d version of the electroweak interaction in terms of the Higgs vacuum expectation value nu, of the non-Abelian gauge coupling g, and of the Abelian gauge coupling g', when…

High Energy Physics - Theory · Physics 2013-10-10 M. A. L. Capri , D. Dudal , M. S. Guimaraes , I. F. Justo , S. P. Sorella , D. Vercauteren

We consider the operator $ L = - (d/dx)^2 + x^2 y + w(x) y , y \in L^2(\mathbb{R}) $, where $ w(x) = s [ \delta(x - b) - \delta(x + b)], b \neq 0,$ real, $s \in \mathbb{C}$. This operator has a discrete spectrum: eventually the eigenvalues…

Spectral Theory · Mathematics 2015-06-22 Boris Mityagin

We perform a Wigner analysis of Fourier integral operators (FIOs), whose main examples are Schr\"odinger propagators arising from quadratic Hamiltonians with bounded perturbations. The perturbation is given by a pseudodifferential operator…

Analysis of PDEs · Mathematics 2025-03-04 Elena Cordero , Gianluca Giacchi , Luigi Rodino

We determine the spectrum of Kostant's cubic Dirac operator $D^{1/3}$ on locally symmetric Lorentzian manifolds of the form $\Gamma\backslash {\rm Osc}_1$, where ${\rm Osc}_1$ is the four-dimensional oscillator group and $\Gamma\subset {\rm…

Differential Geometry · Mathematics 2023-07-06 Ines Kath , Margarita Kraus

In a spacetime with no global timelike Killing vector, we do not have a natural choice for the vacuum state of matter fields, leading to an ambiguity in defining the Feynman propagators. In this paper, taking the vacuum state to be the…

High Energy Physics - Theory · Physics 2013-07-24 Masafumi Fukuma , Yuho Sakatani , Sotaro Sugishita

This paper deals with the massive three-dimensional Dirac operator coupled with a Lorentz scalar shell interaction supported on a compact smooth surface. The rigorous definition of the operator involves suitable transmission conditions…

Spectral Theory · Mathematics 2018-06-01 Markus Holzmann , Thomas Ourmières-Bonafos , Konstantin Pankrashkin

In this work we extend a previous work about the Weyl asymptotics of the distribution of eigenvalues of non-self-adjoint differential operators with small multiplicative random perturbations, by treating the case of operators on compact…

Spectral Theory · Mathematics 2008-09-25 Johannes Sjoestrand

This paper presents an application of white noise functional approach to derive the quantum propagator and the evolution of the reduced density matrix for an open quantum system consisting of coupled harmonic oscillators which are coupled…

Quantum Physics · Physics 2016-07-08 Bienvenido M. Butanas , Roland Cristopher F. Caballar

Darboux transformations of the singular harmonic oscillator are considered. Analytical expressions for the propagators are obtained, using the image method applied to formal singular propagators. Two-well and three-well families of…

Quantum Physics · Physics 2025-12-19 Andrey M. Pupasov-Maksimov , Marcelo Silva Oliveira

Consider a compact manifold with boundary $M$ with a scattering metric $g$ or, equivalently, an asymptotically conic manifold $(M^\circ, g)$. (Euclidean $\mathbb{R}^n$, with a compactly supported metric perturbation, is an example of such a…

Analysis of PDEs · Mathematics 2007-05-23 Andrew Hassell , Jared Wunsch

Applying domain decomposition to the lattice Dirac operator and the associated quark propagator, we arrive at expressions which, with the proper insertion of random sources therein, can provide improvement to the estimation of the…

High Energy Physics - Lattice · Physics 2009-11-11 Tommy Burch , Christian Hagen

We present a classical optics simulation of the one-dimensional Dirac equation for a free particle. Positive and negative energy components are represented by orthogonal polarizations of a free propagating beam, while the spatial profile…

We show that the mode corresponding to the point of essential spectrum of the electromagnetic scattering operator is a vector-valued distribution representing the square root of the three-dimensional Dirac's delta function. An explicit…

Classical Physics · Physics 2007-05-23 Neil V. Budko , Alexander B. Samokhin

Deformation quantization for any Grassmann scalar free field is described via the Weyl-Wigner-Moyal formalism. The Stratonovich-Weyl quantizer, the Moyal $\star$-product and the Wigner functional are obtained by extending the formalism…

High Energy Physics - Theory · Physics 2011-07-19 I. Galaviz , H. Garcia-Compean , M. Przanowski , F. J. Turrubiates

Let $(M,g)$ be a complete non-compact Riemannian surface. We consider operators of the form $\Delta + aK + W$, where $\Delta$ is the non-negative Laplacian, $K$ the Gaussian curvature, $W$ a locally integrable function, and $a$ a positive…

Differential Geometry · Mathematics 2019-10-07 Pierre Bérard , Philippe Castillon

We develop a method to obtain $\epsilon$-expansions of massless two-point integrals in position space, based on the constraints implied by symmetries of the asymptotic expansion of conformal four-point integrals. Together with parametric…

High Energy Physics - Theory · Physics 2018-02-05 Alessandro Georgoudis , Vasco Gonçalves , Erik Panzer , Raul Pereira

We construct, using simple geometrical arguments, a Wigner function defined on a discrete phase space of arbitrary integer Hilbert-space dimension that is free of redundancies. ``Ghost images'' plaguing other Wigner functions for discrete…

Quantum Physics · Physics 2009-11-11 Arturo Argüelles , Thomas Dittrich
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