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Related papers: Suppression of PiNN* Coupling and Chiral Symmetry

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Meson-baryon couplings between positive and negative parity nucleons are investigated using two point correlation functions in the soft meson and the chiral limit. We find that the pi NN* coupling vanishes due to chiral symmetry, while the…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Jido , Y. Nemoto , M. Oka , A. Hosaka

Jido, Oka and Hosaka have shown that the p-slash gamma_5 piece of the pion-to-vacuum correlator of two baryon interpolating fields vanishes in the soft-pion limit, as a consequence of chiral transformation properties of those fields. This…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael C. Birse

The \pi NN^* and \eta NN^* coupling constants are studied based on the two point functions between the vacuum and a one meson state in the soft meson limit. In terms of a suitably constructed interpolating field for the nucleon and…

High Energy Physics - Phenomenology · Physics 2008-02-03 D. Jido , M. Oka , A. Hosaka

Chiral properties of positive and negative parity nucleons, N and N*$, are studied from the viewpoint of chiral symmetry. Two possible ways to assign chiral transformations to the negative parity nucleon are considered. Using linear sigma…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Jido , Y. Nemoto , M. Oka , A. Hosaka

Using a chiral unitary model in which the negative parity nucleon resonance $N^\ast \equiv N^\ast(1535)$ is generated dynamically by means of the Bethe Salpeter equation with coupled meson baryon channels in the $S = 0$ sector, we have…

Nuclear Theory · Physics 2009-10-31 J. C. Nacher , A. Parreno , E. Oset , A. Ramos , A. Hosaka , M. Oka

The \pi NN^* and \eta NN^* coupling constants are studied in the QCD sum rule ($N^* \equiv N(1535)). We investigate the two point functions between the vacuum and a one meson state in the soft meson limit. The operator product expansion is…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Hosaka , D. Jido , M. Oka

If a baryon field belongs to a certain linear representation of chiral symmetry of $SU(2) \otimes SU(2)$, the axial coupling constant $g_{A}$ can be determined algebraically from the commutation relations derived from the superconvergence…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. Hosaka , D. Jido , M. Oka

Baryon resonances with even and odd parity are collectively investigated from the viewpoint of chiral symmetry(ChS). We propose a quartet scheme where Delta's and N^*'s with even and odd parity form a chiral multiplet. This scheme gives…

High Energy Physics - Phenomenology · Physics 2011-07-19 D. Jido , T. Hatsuda , T. Kunihiro

The strong coupling constants of the $\pi$ and $K$ mesons with negative parity octet baryons are estimated within the light cone QCD sum rules. It is observed that all strong coupling constants, similar to the case for the positive parity…

High Energy Physics - Phenomenology · Physics 2016-12-21 T. M. Aliev , M. Savcı

Chiral symmetry of the 2-dimensional chiral Gross-Neveu model is broken explicitly by a bare mass term as well as a splitting of scalar and pseudo-scalar coupling constants. The vacuum and light hadrons - mesons and baryons which become…

High Energy Physics - Theory · Physics 2014-11-20 Christian Boehmer , Michael Thies

We present a chiral-invariant meson-baryon Lagrangian which describes the interactions of the baryon octet with the lowest-mass meson nonets. The nonlinear realization of the chiral symmetry generates pair-meson interaction vertices. The…

Nuclear Theory · Physics 2016-09-08 V. G. J. Stoks , Th. A. Rijken

Masses and couplings of the negative parity excited baryons are studied in the QCD sum rule. Separation of the negative-parity spectrum is proposed and is applied to the flavor octet and singlet baryons. We find that the quark condensate is…

High Energy Physics - Phenomenology · Physics 2015-06-25 M. Oka , D. Jido , A. Hosaka

The strong coupling constants of negative parity heavy baryons belonging to a sextet and antitriplet representations of $SU_f(3)$ with light $\pi$ and $K$ mesons are estimated within the light cone QCD sum rules. It is observed that each…

High Energy Physics - Phenomenology · Physics 2017-12-06 T. M. Aliev , S. Bilmis , M. Savci

It is generally thought that pion masses vanish when bare light quark masses $m_q$ vanish. The pions are Nambu-Goldstone bosons of chiral $SU_{A}(2)$ symmetry. We discuss a possibility that even when $m_q=0$, the chiral symmetry is…

High Energy Physics - Phenomenology · Physics 2019-04-22 Aiichi Iwazaki

We construct an $SU(3)_L \times SU(3)_R$ symmetric chiral effective model which includes parity pair baryon fields. It is assumed that the positive and negative parity baryons in the parity pair have opposite chiral transformation…

High Energy Physics - Phenomenology · Physics 2009-10-30 Y. Nemoto , D. Jido , M. Oka , A. Hosaka

The N*(1440) -> N pi pi decay is studied by making use of the chiral reduction formula. This formula suggests a scalar-isoscalar pion-baryon contact interaction which is absent in the recent study of Hern{\'a}ndez et al. The contact…

Nuclear Theory · Physics 2009-11-10 H. Kamano , M. Morishita , M. Arima

The coupling constants of K and pi mesons with the octet baryons are studied in light cone QCD sum rules taking into account SU(3)f flavor symmetry breaking effects, but keeping the SU(2) isospin symmetry intact. It is shown that, in the…

High Energy Physics - Phenomenology · Physics 2009-11-11 T. M. Aliev , A. Ozpineci , S. B. Yakovlev , V. Zamiralov

The effective restoration of the chiral U(A)(1) symmetry in strong interactions is studied using the linear chiral SU(3)xSU(3) model at finite temperatures. We find that the disappearance of the chiral anomaly causes a considerable change…

High Energy Physics - Phenomenology · Physics 2011-07-19 J. Schaffner-Bielich

From an SU(2)$\otimes $SU(2) chiral quark potential model incorporating spontaneous chiral symmetry breaking the asymptotic $\pi $ and $\sigma $ exchange pieces of the $NN$ potential are generated. From them the $\pi NN$ and $\sigma NN$…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. T. Fernandez-Carames , P. Gonzalez , A. Valcarce

In this two part series a chiral confining model of baryons is used to describe low--lying negative parity resonances $N^*$, $\Delta^*$, $\Lambda^*$ and $\Sigma^*$ in the mean field approximation. A physical baryon in this model consists of…

Nuclear Theory · Physics 2007-05-23 Y. Umino , M. K. Banerjee
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