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The experimental determination of low energy pi K scattering phase shifts would assist in determining scattering lengths as well as low energy constants of chiral perturbation theory for which sum rules have been constructed. The FOCUS…

High Energy Physics - Phenomenology · Physics 2016-09-06 B. Ananthanarayan , K. Shivaraj

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…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. V. Anisovich , H. Leutwyler

We use both old and new theoretical developments in QCD dispersion relation constraints on the scalar form factor in the decay K --> \pi l \nu_l to obtain constraints on the strange quark mass. The perturbative QCD side of the calculation…

High Energy Physics - Phenomenology · Physics 2014-11-17 Richard F. Lebed , Karl Schilcher

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…

High Energy Physics - Phenomenology · Physics 2012-01-23 Martin Zdrahal

We show that, independently of the size of the quark condensate, chiral symmetry correlates the two S-wave \pi\pi scattering lengths. In view of this constraint, the new precision data on K_{e_4} decay allow a remarkably accurate…

High Energy Physics - Phenomenology · Physics 2009-07-09 G. Colangelo , J. Gasser , H. Leutwyler

We calculate the ratios R_{e/mu}^{(P)} = Gamma(P -> e nu)/Gamma (P -> mu nu) (P=pi,K) in Chiral Perturbation Theory to order e^2 p^4. We complement the one- and two-loop effective theory results with a matching calculation of the local…

High Energy Physics - Phenomenology · Physics 2009-02-18 Vincenzo Cirigliano , Ignasi Rosell

$K_{\ell4}$ are for several reasons an especially interesting decay channel of $K$ mesons: $K_{\ell4}$ decays allow an accurate measurement of a combination of $S$-wave $\pi\pi$ scattering lengths, one form factor of the decay is connected…

High Energy Physics - Phenomenology · Physics 2017-08-23 Gilberto Colangelo , Emilie Passemar , Peter Stoffer

$K_{\ell4}$ decays offer several reasons of interest: they allow an accurate measurement of $\pi\pi$-scattering lengths; they provide the best source for the determination of some low-energy constants of ChPT; one form factor is directly…

High Energy Physics - Phenomenology · Physics 2015-09-09 Gilberto Colangelo , Emilie Passemar , Peter Stoffer

The cusp effect in K \to 3\pi and data on K_e4 decays allow one to extract experimental information on the elastic \pi\pi scattering amplitude near threshold, and to confront the outcome of the analyses with predictions made in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Gasser

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…

High Energy Physics - Phenomenology · Physics 2011-12-21 Karol Kampf , Marc Knecht , Jiří Novotný , Martin Zdráhal

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…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. Borasoy , Ulf-G. Meißner , R. Nißler

The NA48/2 experiment at the CERN SPS collected in 2003 and 2004 large samples of the decays K+- -> pi+ pi- e+- nu (Ke4+-), K+- -> pi0 pi0 e+- nu (Ke400) and K+- -> pi0 pi0 pi+-. From the Ke4+- form factors and from the cusp in the M00^2…

High Energy Physics - Experiment · Physics 2017-08-23 L. Masetti

The NA48/2 experiment at CERN reports the first observation of the $K^{\pm} \rightarrow \pi^{0} \pi^{0} \mu^{\pm} \nu$ decay based on a sample of 2437 candidates with 15% background contamination collected in 2003--2004. The decay branching…

High Energy Physics - Experiment · Physics 2024-03-26 2 Collaboration , J. R. Batley , G. Kalmus , C. Lazzeroni , D. J. Munday , M. W. Slater , S. A. Wotton , R. Arcidiacono , A. Ceccucci , G. Bocquet , N. Cabibbo , D. Cundy , V. Falaleev , L. Gatignon , M. Fidecaro , A. Gonidec , W. Kubischta , A. Maier , A. Norton , M. Patel , A. Peters , S. Balev , P. L. Frabetti , E. Gersabeck , E. Goudzovski , P. Hristov , V. Kekelidze , D. Madigozhin , N. Molokanova , I. Polenkevich , Yu. Potrebenikov , A. Korotkova , S. Stoynev , A. Zinchenko , V. Kozhuharov , L. Litov , E. Monnier , E. Swallow , R. Winston , P. Rubin , A. Walker , W. Baldini , A. Cotta Ramusino , P. Dalpiaz , C. Damiani , M. Fiorini , A. Gianoli , M. Martini , F. Petrucci , M. Savrié , M. Scarpa , H. Wahl , A. Bizzeti , M. Veltri , M. Calvetti , E. Celeghini , E. Iacopini , M. Lenti , G. Ruggiero , M. Behler , K. Eppard , M. Hita-Hochgesand , K. Kleinknecht , P. Marouelli , L. Masetti , U. Moosbrugger , C. Morales Morales , B. Renk , M. Wache , A. Winhart , R. Wanke , D. Coward , A. Dabrowski , T. Fonseca Martin , M. Shieh , M. Szleper , M. Velasco , M. D. Wood , P. Cenci , M. Pepe , M. C. Petrucci , G. Anzivino , E. Imbergamo , A. Nappi , M. Piccini , M. Raggi , M. Valdata-Nappi , C. Cerri , R. Fantechi , G. Collazuol , L. Di Lella , G. Lamanna , I. Mannelli , A. Michetti , F. Costantini , N. Doble , L. Fiorini , S. Giudici , G. Pierazzini , M. Sozzi , S. Venditti , B. Bloch-Devaux , B. Peyaud , C. Cheshkov , J. B. Chèze , M. De Beer , J. Derré , G. Marel , E. Mazzucato , B. Vallage , M. Holder , M. Ziolkowski , C. Biino , N. Cartiglia , F. Marchetto , S. Bifani , M. Clemencic , S. Goy Lopez , H. Dibon , M. Jeitler , M. Markytan , I. Mikulec , G. Neuhofer , L. Widhalm

We derive the decay rate of $\pi\mu$ atom formation in $K_{\mu 4}$ decay. Using the obtained expressions we calculate the decay rate of atom formation and point out that considered decay can give a noticeable contribution as a background to…

High Energy Physics - Phenomenology · Physics 2010-05-07 S. R. Gevorkyan , A. V. Tarasov , O. O. Voskresenskaya

The NA48/2 experiment at the CERN SPS collected in 2003 and 2004 large samples of the decays K+- -> pi+ pi- e+- nu (Ke4+-), K+- -> pi0 pi0 e+- nu (Ke400) and K+- -> pi0 pi0 pi+-. From the Ke4+- form factors and from the cusp in the M00^2…

High Energy Physics - Experiment · Physics 2008-11-26 L. Masetti

The decays tau -> 3 pi + nu(tau) are analyzed at one loop order in the framework of Generalized Chiral Perturbation Theory, in order to test the sensitivity to the size of spontaneous chiral symmetry breaking parameters, contained in the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Luca Girlanda , Jan Stern

The infinite mass effective theory, when a heavy quark mass tends to infinity, and Chiral perturbation theory at the quark level, based on the extended Nambu -- Jona -- Lasinio model with linear realization of chiral $U(3)\times U(3)$…

High Energy Physics - Phenomenology · Physics 2016-09-01 F. Hussain , A. N. Ivanov , N. I. Troitskaya

High statistics Dalitz-plot distribution of $\eta \to \pi^+\pi^-\pi^0$ decay obtained recently by KLOE collaboration \cite{kloe} is fitted to the results of corresponding theoretical calculations in Chiral Perturbation Theory (ChPT) with…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. V. Martemyanov , V. S. Sopov

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…

High Energy Physics - Phenomenology · Physics 2018-11-20 Gilberto Colangelo , Stefan Lanz , Heinrich Leutwyler , Emilie Passemar

The branching ratio of the \eta->3\pi decay is an important source of information on the value of the quark mass ratio 1/R=(m_d-m_u)/(m_s-\hat m). Furthermore, isospin breaking effects in the decays K->3\pi provide information on the pion…

High Energy Physics - Phenomenology · Physics 2011-03-07 M. Zdrahal , K. Kampf , M. Knecht , J. Novotny
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