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Like the axial vector charges, defined from the forward nucleon matrix element of the axial vector current on the light cone, the nucleon tensor charge, defined from the corresponding matrix element of the tensor current, is essential for…

High Energy Physics - Phenomenology · Physics 2007-05-23 Leonard Gamberg , Gary R. Goldstein

The axial vector and tensor charge, defined as the first moments of the forward nucleon matrix elements of corresponding quark currents, are essential for characterizing the spin structure of the nucleon. However, the transversity…

High Energy Physics - Phenomenology · Physics 2009-11-07 Leonard Gamberg , Gary R. Goldstein

We point out that the new interaction of spinning particles with the torsion tensor, discussed recently, is odd under charge conjugation and time reversal. This explains rather unexpected symmetry properties of the induced effective…

High Energy Physics - Theory · Physics 2009-11-11 I. B. Khriplovich , A. A. Pomeransky

We calculate the tensor and axial charges of the quark in the Schwinger-Dyson formalism of Landau gauge QCD. It is found that the dressed tensor and isovector axial charges of the quark are suppressed against the bare quark contribution,…

High Energy Physics - Phenomenology · Physics 2014-01-30 Nodoka Yamanaka , Takahiro M. Doi , Shotaro Imai , Hideo Suganuma

The difference in angular distributions between top quarks and antiquarks, commonly referred to as the charge asymmetry, is measured in pp collisions at the LHC with the CMS experiment. The data sample corresponds to an integrated…

High Energy Physics - Experiment · Physics 2012-08-27 CMS Collaboration

Charge correlations in lattice gauge calculations suggest that up, down and strange charges move independently in the QGP (quark-gluon plasma), and that the density of such charges is similar to what is expected from simple thermal…

Nuclear Theory · Physics 2015-06-04 Scott Pratt

The regularities at large distances of complete gauge invariance in QCD are shown to bear nontrivial consequences for the selection among inequivalent representations of canonical commutation (anticommutation) rules for gauge boson (quark)…

High Energy Physics - Theory · Physics 2012-02-17 Peter Minkowski

We constrain generic nonstandard neutrino interactions with existing experimental data on neutrino transition magnetic moments and derive strong bounds on tensorial couplings of neutrinos to charged fermions. We also discuss how some of…

High Energy Physics - Phenomenology · Physics 2014-04-24 Kristopher J. Healey , Alexey A. Petrov , Dmitry Zhuridov

We propose to measure the $HZ\gamma$ and $H\gamma\gamma$ anomalous couplings in the process of $e^{+}e^{-}\rightarrow H\gamma$ with the sequential decay of $H\to b{\bar b}$. The discovery potential of observing the anomalous couplings are…

High Energy Physics - Phenomenology · Physics 2015-12-09 Qing-Hong Cao , Hao-Ran Wang , Ya Zhang

Within the context of the Standard Model, quarks are placed in a $(\mathbf{3},\mathbf{2})\oplus (\mathbf{3},\bar{\mathbf{2}})$ matter field representation of $U_{EW}(2)$. Although the quarks carry unit intrinsic electric charge in this…

High Energy Physics - Phenomenology · Physics 2015-01-27 J. LaChapelle

A topological approach to quark fractional charges, based on charge constraints unexplained by the Standard Model of particle physics, is discussed. Charge fractionalization is related to a tunneling process occurring in time between pure…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernesto A. Matute

For gauge theories with direct product internal symmetry groups, the relationship between internal quantum numbers (charges) and coupling strengths is examined. In these types of theories, the Lagrangian density may contain non-trivial…

High Energy Physics - Phenomenology · Physics 2015-01-27 J. LaChapelle

With appropriate gauge transformations, field can replace electric charge in quarks. Classical quarks, in a necessary non-gauge invariant formulation, are used for illustration, bringing to the fore the limitations of the usual electric…

General Physics · Physics 2015-10-05 Harry Schiff

It is shown that the difference in the distributions of positive ($\mu^+$) and negative charged leptons ($\mu^-$) in reactions $\gamma \gamma \to \mu^+\mu^-+\nu\bar\nu$ and $\gamma \gamma \to W^\pm\mu^\mp +\nu(\bar\nu)$ at $\sqrt{s}>200$…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. A. Anipko , M. Cannoni , I. F. Ginzburg , O. Panella , A. V. Pak

The standard additive quark model and the ensuing counting rules are modified to take into account the quark-gluonic content of the Pomeron and of the secondary Reggeons. The result is that a much improved description of $pp, \pi p, \gamma…

High Energy Physics - Phenomenology · Physics 2011-09-13 P. Desgrolard , M. Giffon , E. Martynov , E. Predazzi

Using the multipole expansion of electromagnetic (EM) field, we present the angular magnetoelectric (AME) coupling in irreducible tensor form. We evaluate the matrix elements when the radiation source is described by electronic transitions…

Atomic Physics · Physics 2017-10-11 Rytis Jursenas

The Tevatron, where the top quark was discovered, and the currently functional Large Hadron Collider (LHC), with copiously produced top pairs, enable a detailed study of top-quark properties. In particular, they can be used to test the…

High Energy Physics - Phenomenology · Physics 2013-10-31 Sudhansu S. Biswal , Saurabh D. Rindani , Pankaj Sharma

We examine charge correlations and instabilities in the pseudogap phase of high-$T_c$ cuprates modeled by $d$-density wave ordering. The latter has a gap symmetry similar to the one observed in the $d$-wave superconductor. We use $t$-$J$…

Strongly Correlated Electrons · Physics 2023-10-17 Dheeraj Kumar Singh , Yunkyu Bang

Advances in research have sparked an increasing curiosity in understanding the plasmonic excitation properties of molecular-scale systems. Polycyclic aromatic hydrocarbons, as the fundamental building blocks of graphene, have been…

Mesoscale and Nanoscale Physics · Physics 2025-01-22 Haoran Liu , Nan Gao , Yurui Fang

We extend the quark-meson coupling (QMC) model to incorporate chiral symmetry. The relationship between the QMC model and chiral perturbation theory is also discussed. The nuclear central potential is modified by the effect of internal…

Nuclear Theory · Physics 2015-05-18 Koichi Saito