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Related papers: Weak Nonleptonic Omega Decay in Chiral Perturbatio…

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We first review the current algebra - PCAC approach to nonleptonic octet baryon 14 weak decay B (\to) (B^{\prime})(\pi) amplitudes. The needed four parameters are independently determined by (\Omega \to \Xi \pi),(\Lambda K) and (\Xi ^{-}\to…

High Energy Physics - Phenomenology · Physics 2016-08-15 M. D. Scadron , D. Tadić

We study the |Delta I|=3/2 amplitudes of the octet-hyperon decays B -> B' + pion and of the decays Omega^- -> Cascade + pion in the context of heavy-baryon chiral perturbation theory. For the octet-hyperon decays, we investigate the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jusak Tandean

The non-leptonic hyperon decays are analyzed up to one-loop order including all counterterms in the framework of heavy baryon chiral perturbation theory. We use the exchange of the spin-3/2 decuplet resonances as an indication of which…

High Energy Physics - Phenomenology · Physics 2011-09-13 B. Borasoy , B. R. Holstein

Motivated by recent experimental advances in the corresponding measurements, non-leptonic hyperon decays are calculated, for the first time in a relativistic manner, in Chiral Perturbation Theory at next-to-leading order (NLO). On the one…

High Energy Physics - Phenomenology · Physics 2026-04-16 Nora Salone , Fernando Alvarado , Stefan Leupold , Andrzej Kupsc

In the framework of the heavy baryon chiral perturbation theory (HBChPT), we calculate the radiative decay amplitudes of the singly heavy baryons up to the next-to-next-to-leading order (NNLO). In the numerical analysis, we adopt the heavy…

High Energy Physics - Phenomenology · Physics 2019-02-27 Guang-Juan Wang , Lu Meng , Shi-Lin Zhu

Hyperon non-leptonic weak decay amplitudes are studied in the chiral perturbation theory. The weak interaction vertices caused by the four quark operators are substituted by the products of the hadronic currents and by the…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Takayama , M. Oka

We present an analysis of the octet baryon masses and the $\pi N$ and $KN$ $\sigma$--terms in the framework of heavy baryon chiral perturbation theory. At next-to-leading order, ${\cal O}(q^3)$, knowledge of the baryon masses and…

High Energy Physics - Phenomenology · Physics 2016-08-14 Véronique Bernard , Norbert Kaiser , Ulf-G. Meißner

Hyperon non-leptonic weak decay amplitudes are studied in the chiral perturbation theory. We employ the low energy effective weak Hamiltonian which contains the perturbative QCD correction. To include the non-perturbative QCD effect, quark…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Takayama , M. Oka

The complete renormalization of the weak Lagrangian to chiral order q^2 in heavy baryon chiral perturbation theory is performed using heat kernel techniques. The results are compared with divergences appearing in the calculation of Feynman…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Borasoy , G. Muller

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

The development of chiral perturbation theory in hyperon phenomenology has been troubled due to power-counting subtleties and to a possible slow convergence. Furthermore, the presence of baryon-resonances, e.g. the lowest-lying decuplet,…

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

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

$\Omega_b \rightarrow \Omega_c^{(*)}$ semi-leptonic decays are studied in details. Relevant helicity amplitudes are written down. Both unpolarized and polarized $\Omega_b$ cases are considered. Decay angular distributions, asymmetry…

High Energy Physics - Phenomenology · Physics 2015-05-28 Ming-Kai Du , Chun Liu

We study the decay Omega^- -> Xi^- pi^+ pi^- in heavy-baryon chiral perturbation theory. At leading order, the decay is completely dominated by the Xi^{*0}(1530) intermediate state, and the predicted rate and Xi^-pi^+ mass distribution are…

High Energy Physics - Phenomenology · Physics 2008-11-26 Oleg Antipin , Jusak Tandean , G. Valencia

We examine the importance of J^P = 1/2^+, 1/2^- resonances for weak nonleptonic Omega^- decays within the framework of chiral perturbation theory. The spin-1/2 resonances are included into an effective theory and tree contributions to the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Bugra Borasoy , Barry R. Holstein

We use one-loop chiral perturbation theory (ChPT) to compare lattice results for the K+ to pi+ pi0 decay amplitude with the experimental value. Three systematic effects: quenching, finite-volume effects, and the use of unphysical values of…

High Energy Physics - Lattice · Physics 2009-10-30 Maarten Golterman , Ka Chun Leung

Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose couplings ("low-energy constants") encode all non-perturbative QCD physics. It has recently been suggested that these low-energy constants…

High Energy Physics - Lattice · Physics 2010-02-03 P. Hernandez , M. Laine

The mass spectrum of the lowest lying octet baryons is calculated to next-to-next-to-leading order in heavy baryon chiral perturbation theory and partially quenched heavy baryon chiral perturbation theory. We work in the isospin limit and…

High Energy Physics - Lattice · Physics 2009-11-10 Andre Walker-Loud

We investigate the nonleptonic two-body weak decays of the single bottom baryon $\Omega_{b}^{*}$ into $\Omega_{c}^{*}P(V)$ final states within the factorization framework. Employing this framework and incorporating the contributions from…

High Energy Physics - Phenomenology · Physics 2025-12-23 A. Amiri , K. Azizi

We compute the octet baryon charge radii to O(1/Heavy^3) in heavy baryon chiral perturbation theory. We examine the effect of including the decuplet of spin-3/2 baryons explicitly. We find that it does no t improve the level of agreement…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. J. Puglia , M. J. Ramsey-Musolf , Shi-Lin Zhu
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