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Related papers: Baryon magnetic moments in chiral perturbation the…

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The baryon magnetic and transition magnetic moments are computed in heavy baryon chiral perturbation theory in the large-N_c limit, where N_c is the number of colors. One-loop nonanalytic corrections of orders m_q^{1/2} and m_q ln m_q are…

High Energy Physics - Phenomenology · Physics 2010-01-18 Ruben Flores-Mendieta

Baryon magnetic moments are computed in baryon chiral perturbation theory in the large-$N_c$ limit at one-loop order, where $N_c$ is the number of color charges. Orders $\mathcal{O}(m_q^{1/2})$ and $\mathcal{O}(m_q \ln m_q)$ corrections are…

High Energy Physics - Phenomenology · Physics 2022-01-05 Ruben Flores-Mendieta , Carlos Isaac Garcia , Johann Hernandez , Maria Anabel Trejo

First non-trivial chiral corrections to the magnetic moments of triplet (T) and sextet (S^(*)) heavy baryons are calculated using Heavy Hadron Chiral Perturbation Theory. Since magnetic moments of the T-hadrons vanish in the limit of…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. C. Banuls , I. Scimemi , J. Bernabeu , V. Gimenez , A. Pich

We extend an earlier study of the baryon magnetic moments in chiral perturbation theory by the explicit inclusion of the spin-3/2 decuplet resonances. We find that the corrections induced by these heavier degrees of freedom are relatively…

High Energy Physics - Phenomenology · Physics 2014-11-18 L. S. Geng , J. Martin Camalich , M. J. Vicente Vacas

We report a calculation of the baryon magnetic moments using covariant chiral perturbation theory within the extended-on-mass-shell renormalization scheme including intermediate octet and decuplet contributions. By fitting the two available…

High Energy Physics - Phenomenology · Physics 2011-02-09 J. Martin Camalich , L. Alvarez-Ruso , L. S. Geng , M. J. Vicente Vacas

We reexamine critically the chiral expansion for the baryon magnetic moments including the contributions from loops which involve intermediate octet and decuplet baryons. We find that, contrary to some claims, the nonanalytic loop…

High Energy Physics - Phenomenology · Physics 2009-10-30 Loyal Durand , Phuoc Ha

We analyze the baryon mass differences up to second order in chiral perturbation theory, including the effects of decuplet intermediate states. We show that the Coleman--Glashow relation has computable corrections of order $(m_d - m_u)…

High Energy Physics - Phenomenology · Physics 2009-10-28 Richard F. Lebed , Markus A. Luty

We consider the baryon octet and decuplet magnetic moments in a simultaneous expansion in $m_s$ and $1/N$ taking $N_F / N \sim 1$, where $N$ is the number of QCD colors and $N_F$ is the number of light quark flavors. At leading order in…

High Energy Physics - Phenomenology · Physics 2009-09-25 Markus A. Luty , John March-Russell , Martin White

Nonanalytic $m_q^{1/2}$ and $m_q\ln m_q$ chiral corrections to the baryon magnetic moments are computed. The calculation includes contributions from both intermediate octet and decuplet baryon states. Unlike the one-loop contributions to…

High Energy Physics - Phenomenology · Physics 2010-04-06 Elizabeth Jenkins , Michael Luke , Aneesh V. Manohar , M. J. Savage

Baryon octet magnetic moments when calculated within the chiral quark model, incorporating the orbital angular momentum as well as the quark sea contribution through the Cheng-Li mechanism, not only show improvement over the non…

High Energy Physics - Phenomenology · Physics 2009-11-07 Harleen Dahiya , Manmohan Gupta

We compute the magnetic moments of the octet baryons up to two orders in quenched chiral perturbation theory. In addition to the $\sim\sqrt{m_q}$ contributions that arise in QCD, there are lower-order contributions of the form $M_0^2\log…

Nuclear Theory · Physics 2009-11-07 Martin J. Savage

We calculate the octet baryon magnetic moments in covariant baryon chiral perturbation theory with the extended-on-mass-shell renormalization scheme up to next-to-next-to-leading order. At this order, there are nine low-energy constants,…

High Energy Physics - Phenomenology · Physics 2018-06-25 Yang Xiao , Xiu-Lei Ren , Jun-Xu Lu , Li-Sheng Geng , Ulf-G. Meißner

We have systematically investigated the decuplet (T) to octet (B) baryon ($T\rightarrow B\gamma$) transition magnetic moments to the next-to-next-to-leading order and electric quadruple moments to the next-to-leading order in the framework…

High Energy Physics - Phenomenology · Physics 2017-06-22 Hao-Song Li , Zhan-Wei Liu , Xiao-Lin Chen , Wei-Zhen Deng , Shi-Lin Zhu

We show that the magnetic moments of the octet baryons can be fitted to an accuracy of 1.5 percent by a phenomenological Lagrangian in which SU(3) breaking corrections appear only linearly. This is in contrast to conventional chiral…

High Energy Physics - Phenomenology · Physics 2008-02-03 J. W. Bos , D. Chang , S. C. Lee , Y. C. Lin , H. H. Shih

Octet and decuplet baryon magnetic moments have been formulated within the \chiQM with configuration mixing incorporating the sea quark polarizations and their orbital angular momentum through the generalization of the Cheng-Li mechanism.…

High Energy Physics - Phenomenology · Physics 2009-03-02 Harleen Dahiya , Manmohan Gupta

We study the decuplet baryon magnetic moments in a QCD-based quark model beyond quenched approximation. Our approach for unquenching the theory is based on the heavy baryon perturbation theory in which the axial couplings for baryon - meson…

High Energy Physics - Phenomenology · Physics 2009-10-31 Phuoc Ha

We present in this talk a recent analysis for the magnetic moments of the baryon antidecuplet within the framework of the chiral quark-soliton model with linear $m_s$ corrections considered. We take into account the mixing of higher…

High Energy Physics - Phenomenology · Physics 2017-08-23 Hyun-Chul Kim , Ghil-Seok Yang , Michal Praszalowicz , Klaus Goeke

First non-trivial chiral corrections to the magnetic moments of triplet (T) and sextet ($S^{(*)}$) heavy baryons are presented using Heavy Hadron Chiral Perturbation Theory. The contributions are calculated up to order ${\cal O}(1/(m_Q…

High Energy Physics - Phenomenology · Physics 2007-05-23 I. Scimemi

The Coleman-Glashow sum-rule for magnetic moments is always fulfilled in the chiral quark model, independently of SU(3) symmetry breaking. This is due to the structure of the wave functions, coming from the non-relativistic quark model.…

High Energy Physics - Phenomenology · Physics 2009-10-30 Johan Linde , Tommy Ohlsson , Hakan Snellman

In this work, we investigate the chiral corrections to the magnetic moments of the spin-$3\over 2$ doubly charmed baryons systematically up to next-to-next-to-leading order with the heavy baryon chiral perturbation theory. The numerical…

High Energy Physics - Phenomenology · Physics 2018-06-08 Lu Meng , Hao-Song Li , Zhan-Wei Liu , Shi-Lin Zhu
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