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相关论文: Light quark mass ratio from Dalitz plot of $\eta \…

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The $\eta \to 3 \pi$ amplitude is sensitive to the quark mass difference $m_u-m_d$ and offers a unique way to determine the quark mass ratio $Q^2 \equiv (m_s^2-m_{ud}^2)/(m_d^2-m_u^2)$ from experiment. We calculate the amplitude…

高能物理 - 唯象学 · 物理学 2017-01-23 Gilberto Colangelo , Stefan Lanz , Heinrich Leutwyler , Emilie Passemar

The dispersive analysis of the decay $\eta\to3\pi$ is reviewed and thoroughly updated with the aim of determining the quark mass ratio ~$Q^2=(m_s^2-m_{ud}^2)/(m_d^2-m_u^2)$. With the number of subtractions we are using, the effects…

高能物理 - 唯象学 · 物理学 2018-11-20 Gilberto Colangelo , Stefan Lanz , Heinrich Leutwyler , Emilie Passemar

The decay $\eta \to 3 \pi$ proceeds exclusively through isospin violating operators and is therefore an excellent probe to examine the strength of isospin breaking in the strong interaction. The latter can be expressed through the quark…

高能物理 - 唯象学 · 物理学 2018-09-27 Stefan Lanz

We propose a novel approach for extracting symmetry breaking effects from symmetry conserving three-body decays. The method is based on mapping the Dalitz plot to a unit disk, and the difference of the disk distributions of two related…

高能物理 - 唯象学 · 物理学 2026-05-26 Adolfo Guevara , Feng-Kun Guo , Hao-Jie Jing

For a precise determination of the m_u and m_d quark masses, it is useful to combine isospin symmetric results of lattice or sum rules QCD techniques with some isospin breaking study performed in chiral perturbation theory (ChPT). The most…

高能物理 - 唯象学 · 物理学 2012-01-23 Martin Zdrahal

Because of their small electromagnetic corrections, the isospin-breaking decays $\eta\to3\pi$ seem to be good candidates for extracting isospin-breaking parameters $ (m_d-m_u)$. This task is unfortunately complicated by large chiral…

高能物理 - 唯象学 · 物理学 2011-12-21 Karol Kampf , Marc Knecht , Jiří Novotný , Martin Zdráhal

In recent years, the decay eta --> 3 pi has received considerable attention from experimental and theoretical side. It is of particular theoretical interest because it allows for the determination of (m_u - m_d). In addition, for many years…

高能物理 - 唯象学 · 物理学 2013-08-26 Stefan Lanz

In view of the recent high-statistic KLOE data for the $\eta \to \pi^+ \pi^- \pi^0$ decay, a new determination of the quark mass double ratio has been done. Our approach relies on a dispersive model that takes into account rescattering…

高能物理 - 唯象学 · 物理学 2017-06-14 P. Guo , I. V. Danilkin , C. Fernández-Ramírez , V. Mathieu , A. P. Szczepaniak

We demonstrate that the decay eta -> 3 pi represents a sensitive probe for the breaking of chiral symmetry by the quark masses. The transition amplitude is proportional to the mass ratio (m_d^2-m_u^2)/(m_s^2-m^2). The factor of…

高能物理 - 唯象学 · 物理学 2008-11-26 A. V. Anisovich , H. Leutwyler

We have studied, with the KLOE detector at the DA$\Phi$NE $\Phi$-Factory, the dynamics of the decay $\eta\to\pi^+\pi^-\pi^0$ using data from the radiative $\phi\to\eta\gamma$ decay for an integrated luminosity $L = 450 \textrm{pb^{-1}}$.…

The isospin-breaking decay eta {\to} 3pi is an ideal tool to extract information on light quark mass ratios from experiment. For a precise determination, however, a detailed description of the Dalitz plot distribution is necessary. In that…

高能物理 - 唯象学 · 物理学 2011-02-17 Sebastian P. Schneider , Bastian Kubis , Christoph Ditsche

We present a new dispersive analysis of the isospin breaking decay eta --> 3 pi. The resulting representation of the decay amplitude allows us to determine the quark mass double ratio Q and we find as a preliminary result Q = 22.3 +/- 0.4.…

高能物理 - 唯象学 · 物理学 2014-11-20 Gilberto Colangelo , Stefan Lanz , Emilie Passemar

Light quark masses are important fundamental parameters of the Standard Model. The decays psi'-->J/psi pi^0 (eta) were widely used in determining the light quark mass ratio m_u/m_d. However, there is a large discrepancy between the…

高能物理 - 唯象学 · 物理学 2010-04-06 Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

The claim that the light quark mass ratio (m_d - m_u)/m_s can be extracted from the decay width ratio Gamma(eta' -> pi^0 pi^+ pi^-)/Gamma(eta' -> eta pi^+ pi^-) is critically investigated within a U(3) chiral unitary framework. The…

高能物理 - 唯象学 · 物理学 2008-11-26 B. Borasoy , Ulf-G. Meißner , R. Nißler

We provide a model-independent determination of the quantity B_0(m_d-m_u). Our approach rests only on chiral symmetry and data from the decay of the eta into three neutral pions. Since the low-energy prediction at next-to-leading order…

高能物理 - 唯象学 · 物理学 2008-11-26 A. Deandrea , A. Nehme , P. Talavera

The branching fraction of the decay $\eta' \to \pi\rho$ is calculated in the chiral quark NJL model. The decay exists due to the mass difference between $u$- and $d$-quarks leading to $\pi^{0}-\eta^{'}$ mixing. Two different approaches are…

高能物理 - 唯象学 · 物理学 2022-11-29 M. K. Volkov , A. A. Pivovarov , K. Nurlan

We study the light quark mass dependence of the $D$ and $D_s$ meson decay constants, $f_D$ and $f_{D_s}$, using a covariant formulation of chiral perturbation theory ($\chi$PT) at next-to-next-to-leading order (NNLO). Using the HPQCD…

高能物理 - 唯象学 · 物理学 2011-02-03 L. S. Geng , M. Altenbuchinger , W. Weise

The chiral effective Lagrangian for pseudoscalar nonet is constructed in consideration of isospin breaking. And the difference of quark condensates is taken accounted. The SU(3) singlet eta0 is not taken as Goldstone-boson. The mixing with…

高能物理 - 唯象学 · 物理学 2009-11-13 Xiaoya Li , Xiaofu Lv

We perform a Dalitz plot analysis of the decay Ds to K+K-pi+ with the CLEO-c data set of 586/pb of e+e- collisions accumulated at sqrt(s) = 4.17 GeV. This corresponds to about 0.57 million D_s+D_s(*)- pairs from which we select 14400…

高能物理 - 实验 · 物理学 2010-04-08 The CLEO Collaboration , R. E. Mitchell

We calculate the decay $\eta\to3\pi$ at next-to-next-to-leading order or order $p^6$ in Chiral Perturbation Theory. The corrections are somewhat larger than was indicated by dispersive estimates. We present numerical results for the Dalitz…

高能物理 - 唯象学 · 物理学 2009-01-06 Johan Bijnens , Karim Ghorbani
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