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Related papers: Large N QCD

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Mesons in large-N QCD are analysed in light-front coordinates with a transverse lattice at strong coupling. In this limit, their properties can be expressed as simple renormalisations of the 't Hooft model results. The integral eigenvalue…

High Energy Physics - Lattice · Physics 2007-05-23 Apoorva Patel

After a brief historical review of the emergence of QCD as the quantum field theory of strong interactions, the basic notions of colour and gauge invariance are introduced leading to the QCD Lagrangian. The second lecture is devoted to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Gerhard Ecker

We continue analytical study of the meson mass spectrum in the large-$N_c$ two-dimensional QCD, known as the 't Hooft model, by addressing the most general case of quarks with unequal masses. Based on our previous work, we develop…

High Energy Physics - Theory · Physics 2025-04-17 Aleksandr Artemev , Alexey Litvinov , Pavel Meshcheriakov

We present a method for ordering two-nucleon interactions based upon their scaling with the number of QCD colors, $N_c$, in the limit that $N_c$ becomes large. Available data in the two-nucleon sector shows general agreement with this…

Nuclear Theory · Physics 2022-12-27 Thomas R. Richardson , Matthias R. Schindler , Roxanne P. Springer

Some mysterious features of the strong interactions become easily understood if our usual QCD with N=3 is `close to' SU(oo) and if the latter theory is confining. N=oo theories are theoretically simpler; in particular there has been much…

High Energy Physics - Lattice · Physics 2007-05-23 Michael Teper

The hyperfine mass splittings of baryons in large $N$ QCD are proved to be proportional to ${\bf J}^2$. Hyperfine mass splittings are first allowed at order $1/N$ in the $1/N$ expansion.

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Jenkins

We present the results of a systematic, first-principles study of the spectrum and decay constants of mesons for different numbers of color charges N, via lattice computations. We restrict our attention to states in the non-zero isospin…

High Energy Physics - Lattice · Physics 2013-06-25 Gunnar S. Bali , Francis Bursa , Luca Castagnini , Sara Collins , Luigi Del Debbio , Biagio Lucini , Marco Panero

By considering the scaling behaviour of various Feynman graphs at leading order in large $\Nf$ at the non-trivial fixed point of the $d$-dimensional $\beta$-function of QCD we deduce the critical exponents corresponding to the quark, gluon…

High Energy Physics - Theory · Physics 2009-10-22 J. A. Gracey

Following Weinberg's argument that narrow tetraquark mesons are not precluded in large N_c QCD, we explore the flow of N_c factors needed for the consistency of this picture, and show that they must arise in a novel way, not simply through…

High Energy Physics - Phenomenology · Physics 2013-10-30 Richard F. Lebed

We provide a brief introduction to the high density effective theory of QCD. As an application, we consider the instanton correction to the perturbatively generated gap in the color superconducting phase. We show that the instanton…

High Energy Physics - Phenomenology · Physics 2017-08-23 Thomas Schaefer

The masses of octet baryons are calculated by the method of QCD sum rules. Using generalized interpolating fields, three independent sets of QCD sum rules are derived which allow the extraction of low-lying N* states with spin-parity 1/2+,…

Nuclear Theory · Physics 2014-11-18 Frank X. Lee , Xinyu Liu

We consider diagonal and non-diagonal QCD sum rules for the ground state heavy baryons to leading order in $1/m_Q$ and at next-to-leading order in $\alpha_S$. In the non-diagonal case we evaluate the eight different two-loop diagrams which…

High Energy Physics - Phenomenology · Physics 2016-08-25 S. Groote , J. G. Körner , O. I. Yakovlev

Triggered by ongoing dark matter searches in the top quark sector at the Large Hadron Collider we report on the calculation of the next-to-leading order QCD corrections to the Standard Model process $pp\to t\bar{t}+ Z(\to \nu_\ell…

High Energy Physics - Phenomenology · Physics 2019-11-15 G. Bevilacqua , H. B. Hartanto , M. Kraus , T. Weber , M. Worek

An elementary, pedagogical introduction to the large-N limit of QCD and to its phenomenological implications is presented, and a survey of lattice results in the 't Hooft limit is briefly discussed.

High Energy Physics - Theory · Physics 2014-03-05 Biagio Lucini , Marco Panero

A systematic study of large N expansion in supersymmetric theories are given. Supersymmetric O(N) non-linear sigma model in two and three dimensions, massless and massive supersymmetric QCD with $N_{f}<N_{c}-1$ and supergravity models are…

High Energy Physics - Phenomenology · Physics 2008-02-03 Tomohiro Matsuda

In the framework of a specific scheme of the QCD sum rules for $S$-wave levels of the heavy quarkonium, one derives expressions, relating the leptonic constants, the energetic density of quarkonium states and universal characteristics in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kiselev V.

We construct the heavy baryonic currents by using the Bethe-Salpeter wave functions in the heavy quark limit. We discuss the one-loop renormalization of these heavy baryonic currents as well as their two-point correlators up to the order…

High Energy Physics - Phenomenology · Physics 2014-11-17 H. Y. Jin , J. G. Körner

We extend the recently developed treatment of baryon resonances in large N_c QCD to describe resonance multiplets collected according to the SU(3) flavor symmetry that includes strange quarks. As an illustration we enumerate the SU(3)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas D. Cohen , Richard F. Lebed

Based on a previous study of deriving the chiral Lagrangian (CL) from QCD, we illustrate the main feature of QCD predictions for the CL coefficients (CLC) in certain approximations. We first show that, in the large-N(c) limit, the anomaly…

High Energy Physics - Phenomenology · Physics 2014-11-17 qing wang , Yu-Ping Kuang , Hua Yang , Qin Lu

We show that excited baryons in large N_c QCD form multiplets, within which masses are first split at O(1/N_c). The dominant couplings of resonances to various mesons are highly constrained: The N(1535) decays at leading 1/N_c order…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas D. Cohen , Richard F. Lebed
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