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Within a chiral quark sigma model in which quarks interact via the exchange of sigma and pi-mesons, hadron properties are investigated. This model of the nucleon and delta is based on the idea that strong QCD forces on very short distances…

General Physics · Physics 2011-10-20 M. Rashdan , T. Ali , S. El-Kholy , M. Abu-Shady

A Roy equation analysis of the available $\pi\pi$ phase shift data is performed with the $I=0$ S- wave scattering length $a^0_0$ in the range predicted by the one-loop standard chiral perturbation theory. A suitable dispersive framework is…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Ananthanarayan , P. Büttiker

The coupling constants g_{\pi \Lambda \Sigma} and g_{K \Sigma \Xi} are calculated in the QCD sum rule approach using the three-point function method and taking into account the SU(3) symmetry breaking effects. The pattern of SU(3) breaking…

Nuclear Theory · Physics 2008-11-26 Seungho Choe

We compute the strong coupling constant $G_{B^{**} B \pi} \; (G_{D^{**} D \pi})$, where $B^{**}$ ($D^{**}$) is the $0^+$ $P-$wave $b \bar q \; (c \bar q)$ state, by QCD sum rules and by light-cone sum rules. The two methods give compatible…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Colangelo , F. De Fazio , N. Di Bartolomeo , R. Gatto , G. Nardulli

We propose a new approach to the determination of hadronic observables in which the essential features of chiral symmetry are combined with conventional constituent quark models. To illustrate the approach, we consider the simple quark…

High Energy Physics - Phenomenology · Physics 2010-02-17 I. C. Cloet , D. B. Leinweber , A. W. Thomas

The B* B pi coupling is a fundamental parameter of chiral effective Lagrangian with heavy-light mesons and can constrain the B->pi l nu form factor in the soft pion limit which will be useful for precise determination of |Vub|. We compute…

High Energy Physics - Lattice · Physics 2009-04-14 Hiroshi Ohki , Hideo Matsufuru , Tetsuya Onogi

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

According to the Coleman-Glashow null theorem if all the symmetry breaking effects belong to the same regular representation (octet in the case of SU(3) and {\bf 15} in the case of SU(4)) and are generated in a tadpole type mechanism, the…

High Energy Physics - Phenomenology · Physics 2016-09-01 R. C. Verma , M. P. Khanna

The $B^* B\pi$ coupling is a fundamental parameter of chiral effective Lagrangian with heavy-light mesons and can constrain the chiral behavior of $f_B$, $B_B$ and the $B\to \pi l \nu$ form factor in the soft pion limit. We compute the $B^*…

High Energy Physics - Lattice · Physics 2008-11-26 Hiroshi Ohki , Hideo Matsufuru , Tetsuya Onogi

We consider a quark-lepton symmetry model of unification of the strong and electromagnetic interactions. The model has the gauge group $SU(4)\times U(1)_{Y}$ and the minimal Higgs structure consisting of one complex quartet of scalar…

High Energy Physics - Phenomenology · Physics 2009-04-09 E. K. Loginov

The form factors for the $B-->\pi$ transition are evaluated in the entire momentum transfer range by using the constraints obtained in the framework combining the heavy quark expansion and chiral symmetry for light quarks and the quark…

High Energy Physics - Phenomenology · Physics 2009-10-31 Riazuddin , T. A. Al-Aithan , Amjad Hussain Shah Gilani

Using QCD sum rules, we compute the diagonal meson-baryon couplings, $\pi NN$, $\eta NN$, $\pi \Xi\Xi$, $\eta \Xi\Xi$, $\pi \Sigma \Sigma$ and $\eta \Sigma \Sigma$, from the baryon-baryon correlation function with a meson, $i\int d^4x…

Nuclear Theory · Physics 2009-11-06 Hungchong Kim , Takumi Doi , Makoto Oka , Su Houng Lee

Properties of b-baryon decay matrix elements (amplitudes) have been derived in a nonsymmetric quark model without any use of SU(6), SU(3), or SU(2) (isotopic spin) groups. Equalities between pairs of amplitudes are derived, and…

High Energy Physics - Phenomenology · Physics 2021-12-16 Jerrold Franklin

We suggest an effective quark model for low-lying baryon octet and decuplet motivated by QCD with a linearly rising confinement potential incorporating the extended Nambu-Jona-Lasinio (ENJL) model with linear realization of chiral U(3)XU(3)…

High Energy Physics - Phenomenology · Physics 2008-11-26 A . N. Ivanov , M. Nagy , N. I. Troitskaya

Chiral symmetry breaking parameters are calculated in quenched SU(2) gauge theory and with Abelian gauge fields projected in maximal Abelian gauge and in field strength gauge. Maximal Abelian gauge projected fields lead to chiral condensate…

High Energy Physics - Lattice · Physics 2016-08-31 R. M. Woloshyn

A flavor SU(2) effective model for pions and quarks is derived by considering polarization effects departing from the usual quark-quark effective interaction induced by dressed gluon exchange, i.e. a global color model for QCD. For that,…

High Energy Physics - Phenomenology · Physics 2016-05-30 Fabio L. Braghin

We evaluate the $\pi N!N$, $\pi\Sigma\Sigma$, $\pi\Lambda\Sigma$, $K\Lambda N$ and $K \Sigma N $ coupling constants and the corresponding monopole masses in lattice QCD with two flavors of dynamical quarks. The parameters representing the…

High Energy Physics - Lattice · Physics 2009-07-10 G. Erkol , M. Oka , T. T. Takahashi

The external-field QCD Sum Rules method is used to evaluate the coupling constants of the light-isoscalar scalar meson (``\sigma'' or \epsilon) to the \Lambda, \Sigma, and \Xi baryons. It is shown that these coupling constants as calculated…

Nuclear Theory · Physics 2008-11-26 G. Erkol , M. Oka , Th. A. Rijken , R. G. E. Timmermans

We close a gap in previous studies of nonsupersymmetric ${\cal N}=0$ quiver gauge theories from a phenomenological point of view aimed at acquiring specific proposals for models beyond the Standard Model (BSM). Because $SU(3)$ is the gauge…

High Energy Physics - Phenomenology · Physics 2017-04-12 Claudio Coriano , Paul H. Frampton

We construct the full axial current of the constituent quarks by a summation of the infinite number of diagrams describing constituent-quark soft interactions. By requiring that the conservation of this current is violated only by terms of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wolfgang Lucha , Dmitri Melikhov , Silvano Simula