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Related papers: Pion Decay Constant at Finite Temperature in the N…

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We have studied radiative pion decays Pi+ -> e+ nu gamma in three broad kinematic regions using the PIBETA detector and a stopped pion beam. Based on Dalitz distributions of 42,209 events we have evaluated absolute Pi -> e nu gamma…

We describe the design, construction and performance of the PIBETA detector built for the precise measurement of the branching ratio of pion beta decay, pi+ -> pi0 e+ nu, at the Paul Scherrer Institute. The central part of the detector is a…

We investigate the critical behaviour at theta=pi of the two-dimensional O(3) nonlinear sigma model with topological term on the lattice. Our method is based on numerical simulations at imaginary values of theta, and on scaling…

High Energy Physics - Lattice · Physics 2013-05-30 Vicente Azcoiti , Giuseppe Di Carlo , Eduardo Follana , Matteo Giordano

The chiral phase transition of the finite temperature QCD is discussed in the ladder approximated Exact (Wilson's) Renormalization Group (ERG). The gluon thermal mass is incorporated by the Hard Thermal Loop (HTL) approximation. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dai Shimizube , Jun-Ichi Sumi

We present an improved Standard-Model (SM) prediction for the dilepton decay of the neutral pion. The loop amplitude is determined by the pion transition form factor for $\pi^0\to\gamma^*\gamma^*$, for which we employ a dispersive…

High Energy Physics - Phenomenology · Physics 2022-05-02 Martin Hoferichter , Bai-Long Hoid , Bastian Kubis , Jan Lüdtke

The pion decay constants of the lowest orbitally excited states of the nucleon and the $\Delta(1232)$ along with the corresponding axial transition form factors are calculated with Poincar\'e covariant constituent-quark models with instant,…

Nuclear Theory · Physics 2009-11-10 B. Julia-Diaz , D. O. Riska , F. Coester

A new version of the so-called optimized perturbation (OPT), implementing consistently renormalization group properties, is used to calculate the nonperturbative ratio $F_\pi/\overline\Lambda$ of the pion decay constant and the basic QCD…

High Energy Physics - Phenomenology · Physics 2013-10-25 J-L. Kneur , A. Neveu

As increased statistics and new ensembles with light pions have become available within the CLS effort, we complete previous work by inspecting the chiral behaviour of the pion decay constant. We discuss the validity of Chiral Perturbation…

High Energy Physics - Lattice · Physics 2013-11-26 Stefano Lottini

A Finite Energy QCD sum rule at non-zero temperature is used to determine the $q^2$- and the T-dependence of the $\rho \pi \pi$ vertex function in the space-like region. A comparison with an independent QCD determination of the…

High Energy Physics - Phenomenology · Physics 2009-10-30 C. A. Dominguez , M. S. Fetea , M. Loewe

The weak decay of the kaon to two pions is studied within the NJL Model. Using the standard effective weak Hamiltonian, both the decay amplitude arising from an intermediate state \sigma-meson and the direct decay amplitude are calculated.…

High Energy Physics - Phenomenology · Physics 2015-02-02 Zhan-Wei Liu , Manuel E. Carrillo-Serrano , Anthony W. Thomas

We summarize recent work in determining the transition form factor (TFF) of the neutral pion ($\pi^0 \to \gamma^*\gamma^*$), by solving the non-perturbative Dyson-Schwinger and Bethe-Salpeter equations. We first study the transition form…

High Energy Physics - Phenomenology · Physics 2018-07-04 Esther Weil , Gernot Eichmann , Christian S. Fischer , Richard Williams

We start by studying the Goldberger-Treiman discrepancy (GTd) $\Delta = (2.259\pm 0.591)%$. Then we look at the $\pi N$ $\sigma$ term, with the dimensionless ratio $\sigma_N/2m_N=3.35%$. Finally we return to predicting (via the quark model)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Miroslav Nagy , Michael D. Scadron , Gerald E. Hite

In this work, we review how the mass and the width of the $f_{0}(500)$ pole behave in a regime where temperature is below the critical chiral transition value. This is attained by considering a large-$N$ $O(N + 1)/O(N)$ invariant Non-Linear…

High Energy Physics - Phenomenology · Physics 2016-09-29 Santiago Cortes , Angel Gomez Nicola , John Morales

Using a non-perturbative method based on the selfconsistent Quasi-particle Random-Phase Approximation (QRPA) we describe the properties of the pion in the linear $\sigma$-model. It is found that the pion is massless in the chiral limit,…

Nuclear Theory · Physics 2009-10-30 Z. Aouissat , G. Chanfray , P. Schuck , J. Wambach

In the present work, the temperature dependence of the scalar mesons parameters is investigated in the framework of thermal QCD sum rules. We calculate sigma-pole and the non-resonant two-pion continuum contributions to the spectral…

High Energy Physics - Phenomenology · Physics 2008-11-26 Elsen Veli Veliev , Takhmassib M. Aliev

We investigate the applicability of finite temperature random phase approximation (RPA) using a solvable Lipkin model. We show that the finite temperature RPA reproduces reasonably well the temperature dependence of total strength, both for…

Nuclear Theory · Physics 2009-11-06 K. Hagino , F. Minato

We compute the large $N$ effective action of the $O(N+1)/O(N)$ non-linear sigma model including the effect of the pion mass to order $m^2_{\pi}/f_{\pi}^2$. This action is more complex than the one corresponding to the chiral limit not only…

High Energy Physics - Phenomenology · Physics 2019-08-17 A. Dobado , J. Morales

We present a new determination of the parity of the neutral pion via the double Dalitz decay pi^0 -> e+ e- e+ e-. Our sample, which consists of 30511 candidate decays, was collected from K_L -> pi0 pi0 pi0 decays in flight at the KTeV-E799…

We investigate the possibility to determine the value of the pion-nucleon sigma term $\sigma_{\pi N}$ precisely by the experimental observables of the deeply bound pionic atoms. We discuss the sensitivity of the observables to $\sigma_{\pi…

This paper is devoted to the evaluation of the pionic scalar density at finite temperature and baryonic density. We express the latter effect in terms of the nuclear response evaluated in the random phase approxima- tion. We discuss the…

Nuclear Theory · Physics 2015-06-26 G. Chanfray , D. Davesne , J. Delorme , M. Ericson , J. Marteau
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