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Related papers: QED(1+1) by Dirac Quantization

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We report the implementation of effective QED potentials for all-electron 4-component relativistic molecular calculations using the DIRAC code. The potentials are also available for 2-component calculations, proper picture-change being…

Chemical Physics · Physics 2022-11-09 Ayaki Sunaga , Maen Salman , Trond Saue

We extend Panella and Roy's [13] work on one-dimensional heterostructure for massless Dirac particles with position-dependent (PD) velocity. We consider Dirac particles where both the mass and velocity are position-dependent. Bound states…

Mathematical Physics · Physics 2018-02-14 Omar Mustafa

We determine the minimal bi-degree(s) of an irreducible filling curve over $\mathbb{F}_q$ for $\mathbb{P}^1\times \mathbb{P}^1$. It is $(q+1, q+1)$ if $q\neq 2$, and they are $(4,3)$ and $(3,4)$ if $q=2$.

Algebraic Geometry · Mathematics 2022-03-23 Masaaki Homma , Seon Jeong Kim

We present the correct solution of the Dirac equation in 1+1 dimensions with the Lorentz scalar potential V(x)=g|x|.

Quantum Physics · Physics 2009-11-07 R. M. Cavalcanti

Estimate (3.39) which appears in the proof of Proposition 3.4 in [Ann. Probab. 27 (1999) 1414--1467, doi:10.1214/aop/1022677454] is wrong. We present below a corrected proof which introduces an extra factor 2 in equations (3.34) and (3.35).…

Probability · Mathematics 2007-05-23 Marzio Cassandro , Enza Orlandi , Pierre Picco

We present results for the equation of state in (2+1)-flavor QCD using the highly improved staggered quark action and lattices with temporal extent $N_{\tau}=6,~8,~10$, and $12$. We show that these data can be reliably extrapolated to the…

Low-temperature expansion of the effective Lagrangian of the QED$_{3+1}$ with a uniform magnetic field and a finite chemical potential is performed. Temperature corrections, as well as zero-temperature expression for the effective…

High Energy Physics - Phenomenology · Physics 2007-05-23 Vadim Zeitlin

The $O(1/m_Q)$ corrections to masses of excited heavy mesons are studied with sum rules in the heavy quark effective theory. Numerical results for the matrix elements of the heavy quark kinetic energy operator K and chromomagnetic…

High Energy Physics - Phenomenology · Physics 2009-10-30 Yuan-ben Dai , Chao-shang Huang , Ming-qiu Huang

The $q$-analogue of an integer $m$ is given by $[m]_q=(1-q^m)/(1-q)$. Let $a$ be an integer, and let $n$ be a positive odd integer. Via discrete Fourier transforms, we establish the following two identities:…

Combinatorics · Mathematics 2026-05-19 Zhi-Wei Sun

We perform an analytic semi-classical quantization of the straight QCD string with one end fixed and a massless quark on the other, in the limits of orbital and radial dominant motion. We compare our results to the exact numerical…

High Energy Physics - Phenomenology · Physics 2014-11-17 Theodore J. Allen , Charles Goebel , M. G. Olsson , Sinisa Veseli

We calculated QED corrections to the $E1$ transition amplitudes in Ne-like iron and nickel. For the $2p \to 3d$ transitions the dominant effect came from the many-electron mixing, or electronic correlations. For the $2p \to 3s$ transitions…

Atomic Physics · Physics 2024-12-30 M. G. Kozlov , V. A. Yerokhin , M. Y. Kaygorodov. , E. V. Tryapitsyna

We present a calculation of the renormalized heavy-light and heavy-heavy currents in HQET at order O(1/m_Q^2).

High Energy Physics - Phenomenology · Physics 2009-10-30 Christopher Balzereit , Thorsten Ohl

I calculate the QED coupling, alpha, directly in the MS-bar scheme using an unsubtracted dispersion relation for the three light quarks, and perturbative QCD for charm and bottom quarks. Compact analytical expressions are presented, making…

High Energy Physics - Phenomenology · Physics 2010-04-06 Jens Erler

There are several mathematical and physical reasons why Dirac's quantization must hold. How far one can go without it remains an open problem. The present work outlines a few steps in this direction.

High Energy Physics - Theory · Physics 2007-05-23 A. I. Nesterov , F. Aceves de la Cruz

QCD equation of state is calculated in (2+1) flavor QCD at temperatures corresponding fermion action on lattices with temporal extent $N_{\tau}=8$. The results are compared with previous calculations performed at twice larger values of the…

High Energy Physics - Lattice · Physics 2010-11-05 P. Petreczky

Based on a simple example, quantization of some 3-spaces is explained.

Mathematical Physics · Physics 2015-05-13 E. Paal , J. Virkepu

We present recent results on the QCD equation of state with 2+1+1 flavors of highly improved staggered quarks (HISQ). We focus on three sets of ensembles with temporal extent 6, 8 and 10, that reach up to temperatures of 967, 725 and 580…

We study the computational complexity of certain integrable quantum theories in 1+1 dimensions. We formalize a model of quantum computation based on these theories. In this model, distinguishable particles start out with known momenta and…

Quantum Physics · Physics 2016-01-01 Saeed Mehraban

Eq.(19) is added and related issues are further clarified. Also some typos and signs a re corrected.

High Energy Physics - Phenomenology · Physics 2009-10-22 HoSeong La

A substantial enhancement is found of the $b \to c\,{\overline c}\, s$ decay rate due to the QCD interaction within the $\overline c s$ pair, which enhancement may amount to 30\%, or more. Some general features of calculation of the QCD…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. B. Voloshin
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