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Related papers: Scalar Mesons and Chiral States

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We study the formation of resonances in terms of the chiral SU(3) Lagrangian. At leading order parameter-free predictions are obtained for the scattering of Goldstone bosons off any hadron once we insist on approximate crossing symmetry of…

Nuclear Theory · Physics 2007-05-23 M. F. M. Lutz , E. E. Kolomeitsev

We construct an extended version of the linear sigma model in such a way as to describe spin-$1$ hadrons as well as spin-$0$ hadrons in two-color QCD (QC$_2$D) by respecting the Pauli-G\"{u}rsey $SU(4)$ symmetry. Within a mean-field…

High Energy Physics - Phenomenology · Physics 2023-12-29 Daiki Suenaga , Kotaro Murakami , Etsuko Itou , Kei Iida

We discuss the formation of s- and d-wave baryon resonances as predicted by the chiral SU(3) symmetry of QCD. Based on the leading order term of the chiral Lagrangian a rich spectrum of molecules is generated, owing to final-state…

High Energy Physics - Phenomenology · Physics 2010-12-16 M. F. M. Lutz , E. E. Kolomeitsev

After giving a short introduction to the Nambu-Jona-Lasinio model with an anomaly term, we show the importance of the scalar-scalar correlation in the low-energy hadron dynamics, which correlation may be summarized by a scalar-isoscalar…

High Energy Physics - Phenomenology · Physics 2016-09-01 Teiji Kunihiro

We discuss a holographic soft-wall model developed for the description of mesons and baryons with adjustable quantum numbers n, J, L, S. This approach is based on an action which describes hadrons with broken conformal invariance and which…

High Energy Physics - Phenomenology · Physics 2012-04-24 Thomas Gutsche , Valery E. Lyubovitskij , Ivan Schmidt , Alfredo Vega

Ground-state scalar isoscalar mesons and a scalar glueball are described in a U(3)xU(3) chiral quark model of the Nambu--Jona-Lasinio (NJL) type with 't Hooft interaction. The latter interaction produces singlet-octet mixing in the scalar…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Ebert , M. Nagy , M. K. Volkov , V. L. Yudichev

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 point out that meson spectrum indicates the existence of a degenerate chiral nonet in the energy region around 1.4 GeV with a slightly inverted spectrum with respect to a qq nonet. Based on this observation, the approximately linear…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mauro Napsuciale , Simon Rodriguez

We discuss the predictions of the bilepton model which is an extension of the standard model in which the group $SU(2) \times U(1)$ is changed to $SU(3)\times U(1)$ and the fermion families are treated non-sequentially with the third…

General Physics · Physics 2022-09-13 Paul H. Frampton

By comparing SU(3)-breaking scales of linear mass formulae, it is shown that the lowest vector, axial-vector, and scalar mesons all have a $\bar{q}q$ configuration, while the ground-state octet and decuplet baryons are $qqq$. Also, the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. D. Scadron , G. Rupp , E. van Beveren , F. Kleefeld

We employ the chiral quark-soliton model and the heavy quark symmetry to describe spectra of charm and beauty baryons. Heavy baryons can be classified according to the SU(3) representations of the light sector. We argue that recently…

High Energy Physics - Phenomenology · Physics 2022-05-09 Maxim V. Polyakov , Michal Praszalowicz

A well pronounced spin--grouping of baryon resonances to O(4) partial waves is found in baryon spectra and shown to be well interpreted in terms of Lorentz group representations of the type (1/2 +l', 1/2 +l')* [(1/2, 0)+(0,1/2)] with l'…

High Energy Physics - Phenomenology · Physics 2011-04-15 M. Kirchbach

The scalar form factors for the pions and kaons are calculated in SU(3) Chiral Perturbation Theory at order $p^6$, in the isospin limit $m_u=m_d=\hat{m}$. We find in general sizable corrections of $\mathcal{O}(p^6)$. We use our results to…

High Energy Physics - Phenomenology · Physics 2009-11-10 Johan Bijnens , Pierre Dhonte

The highlights of studies of mixing among scalar mesons below and above 1 GeV within a nonlinear chiral Lagrangian framework is briefly presented. Two scalar meson nonets are introduced to explore the mass spectrum and decay properties of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amir H. Fariborz

A chiral Lagrangian containing, besides the usual meson fields, their first radial excitations is constructed. The Lagrangian is derived by bosonization of a Nambu--Jona-Lasinio (NJL) type quark model with separable nonlocal interactions.…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. K. Volkov , V. L. Yudichev

A recent D-brane model designed to accommodate a phenomenologically acceptable fourth generation of chiral fermions was noted to produce an unexpected additional unbroken nonanomalous U(1) gauge group at the string scale. We show that the…

High Energy Physics - Phenomenology · Physics 2011-10-27 Richard F. Lebed , Van E. Mayes

The chiral symmetry of QCD requires energy-dependent pionic strong interactions at low energies. This constraint, however, is not fulfilled by the usual Breit--Wigner parameterization of pionic resonances, leading to masses larger than the…

High Energy Physics - Phenomenology · Physics 2019-06-12 Meng-Lin Du , Feng-Kun Guo , Ulf-G. Meißner

There exists a unique class of local Higher Spin Gravities with propagating massless fields in $4d$ - Chiral Higher Spin Gravity. Originally, it was formulated in the light-cone gauge. We construct a covariant form of this theory as a Free…

High Energy Physics - Theory · Physics 2022-08-17 Evgeny Skvortsov , Richard Van Dongen

We generalize the linear sigma model in order to develop a chiral-invariant model of nuclear structure. The model is natural, and contains not only the usual sigma meson which is the chiral partner of the pion but also a new chiral-singlet…

Nuclear Theory · Physics 2010-02-17 K. Saito , H. Kouno , K. Tsushima , A. W. Thomas

We study chiral symmetry aspects of the positive and negative parity baryons by identifying them with linear representations of the chiral group $SU(N_{f}) \otimes SU(N_{f})$. It is shown that there are two distinctive schemes: naive and…

High Energy Physics - Phenomenology · Physics 2011-07-19 Daisuke Jido , Makoto Oka , Atsushi Hosaka