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Related papers: Bi-local baryon interpolating fields with two flav…

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We study the chiral transformation properties of all possible local (non-derivative) interpolating field operators for baryons consisting of three quarks with two flavors, assuming good isospin symmetry. We derive and use the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Keitaro Nagata , Atsushi Hosaka , V. Dmitrašinovi\' c

Fierz identities follow from permutations of quark indices and thus determine which chiral multiplets of baryon fields are Pauli-allowed, and which are not. In a previous paper we have investigated the Fierz identities of baryon fields with…

High Energy Physics - Phenomenology · Physics 2013-09-03 Hua-Xing Chen , V. Dmitrasinovic

We systematically investigate tri-local (non-local) three-quark baryon fields with U_L(2)*U_R(2) chiral symmetry, according to their Lorentz and isospin (flavor) group representations. We note that they can also be called as "nucleon wave…

High Energy Physics - Phenomenology · Physics 2012-10-03 Hua-Xing Chen

Large sets of baryon interpolating field operators are developed for use in lattice QCD studies of baryons with zero momentum. Operators are classified according to the double-valued irreducible representations of the octahedral group. At…

We investigate chiral properties of local (non-derivative) fields of baryons consisting of three quarks with flavor SU(3) symmetry. We construct explicitly independent local three-quark fields belonging to definite Lorentz and flavor…

High Energy Physics - Phenomenology · Physics 2008-12-18 Hua-Xing Chen , V. Dmitrasinovic , Atsushi Hosaka , Keitaro Nagata , Shi-Lin Zhu

We have analyzed the chiral expansion of the baryon masses to second order in the quark masses, including strong isospin violation. The calculations are performed in Lorentz-invariant baryon chiral perturbation theory. Chiral extrapolation…

High Energy Physics - Lattice · Physics 2007-05-23 Matthias Frink , Ulf-G. Meißner

Three-quark nucleon interpolating fields in QCD have well-defined SU_L(3)*SU_R(3) and U_A(1) chiral transformation properties, viz. [(6,3)+(3,6)], [(3,3_bar)+(3_bar,3)], [(8,1)+(1,8)] and their "mirror" images, Ref.[9]. It has been shown…

High Energy Physics - Phenomenology · Physics 2011-01-24 Hua-Xing Chen , V. Dmitrasinovic , Atsushi Hosaka

We study baryons on the lattice with a special focus on excited states. For that purpose we construct several interpolators which differ in their Dirac structure. These interpolators are built from Jacobi smeared quarks with different…

High Energy Physics - Lattice · Physics 2007-05-23 Tommy Burch , Christof Gattringer , Leonid Ya. Glozman , Christian Hagen , Dieter Hierl , C. B. Lang , Andreas Schaefer

We study the most general Fierz identities for a pair of non-contracted Dirac matrices both in the standard basis and for chiral spinors. These identities are useful in building independent effective operators of fermions that involve…

High Energy Physics - Phenomenology · Physics 2012-06-25 Yi Liao , Ji-Yuan Liu

Chiral effective field theory is a framework to derive systematic nuclear interactions. It is based on the symmetries of quantum chromodynamics and includes long-range pion physics explicitly, while shorter-range physics is expanded in a…

Nuclear Theory · Physics 2017-12-05 L. Huth , I. Tews , J. E. Lynn , A. Schwenk

Short-range parts of the baryon-baryon ($BB$) interactions are analyzed from the spin-flavor $SU(6)_{sf}\supset SU(3)_f \times SU(2)_s$ symmetry viewpoint. Due to the Pauli principle of quarks, the symmetry structure of the wave functions…

Nuclear Theory · Physics 2023-01-18 Makoto Oka

Minimally doubled fermions realize one pair of Dirac fermions on the lattice. Similarities to Kogut-Susskind fermions exist, namely, spin and taste degrees of freedom become intertwined, and a peculiar non-singlet chiral symmetry and…

High Energy Physics - Lattice · Physics 2025-08-12 Johannes Heinrich Weber

We match the non-relativistic quark model, with both flavor dependent and flavor independent effective quark-quark interactions, to the spin-flavor operator basis of the 1/Nc expansion for the L=1 non-strange baryons. We obtain analytic…

Nuclear Theory · Physics 2016-02-10 Cintia Willemyns , Carlos Schat

The spectrum of the doubly heavy baryons is estimated with respect to the new observation from the LHCb collaboration [Aaij:2017ueg] by using the chiral partner structure and heavy quark spin-flavor symmetry. The effects of heavy quark…

High Energy Physics - Phenomenology · Physics 2018-08-01 Yong-Liang Ma , Masayasu Harada

The basis of leading operators which are not invariant under baryon number is constructed within the Higgs Effective Field Theory. This list contains 12 dimension six operators, which preserve the combination B-L, to be compared to only 6…

High Energy Physics - Phenomenology · Physics 2017-04-26 Luca Merlo , Sara Saa , Mario Sacristan-Barbero

Using bi-spinor fields we write the pseudo-scalar and bi-spinor fields that are characterized by the field functions of coordinates of several particles, namely multi-particle fields. By applying the quantization procedure to these…

A calculational scheme is developed to evaluate chiral corrections to properties of composite baryons with composite pions. The composite baryons and pions are bound states derived from a microscopic chiral quark model. The model is…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. J. A. Bicudo , G. Krein , J. E. F. T. Ribeiro

We develop a systematic effective field theory framework for studying $|\Delta B|=2$ interactions across energy scales. Using chiral symmetry, we construct the complete and non-redundant set of operators governing these interactions at low…

High Energy Physics - Phenomenology · Physics 2026-04-30 Arnau Bas i Beneito , Ajdin Palavrić , Andrea Sainaghi

Energies for excited light baryons are computed in quenched QCD with a pion mass of 490 MeV. Operators used in the simulations include local operators and the simplest nonlocal operators that have nontrivial orbital structures. All…

We have previously calculated the pion-nucleon $\Sigma_{\pi N}$ term in the chiral mixing approach with $u,d$ flavors only, and found the lower bound $\Sigma_{\pi N} \geq \left(1 + \frac{16}{3} \sin^2 \theta \right){3 \over 2}…

High Energy Physics - Phenomenology · Physics 2018-12-11 V. Dmitrasinovic , Hua-Xing Chen , Atsushi Hosaka
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