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Related papers: Low Energy Constants from Kl4 Form-Factors

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K^0 \to pi^- e^+ nu_e e^+ e^- decay is studied up to the next-to-leading order O^4 in chiral perturbation theory. It is found that the O^4 terms appreciably modifiy the shape of the invariant mass distribution of the leptons and the energy…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. Tsuji , T. Sato

A sum rule analysis of the hadronic tau-decay data can be used to determine the low-energy constants L10(mu) and C87(mu). These constants are QCD chiral-order parameters, which appear at order p^4 and p^6, respectively, in the chiral…

High Energy Physics - Phenomenology · Physics 2009-08-03 M. Gonzalez-Alonso , A. Pich , J. Prades

This paper describes the calculation of the electromagnetic form factor of the K0 meson at order p^6 of chiral perturbation theory which is the next-to-leading order correction to the well-known p^4 result achieved by Gasser and Leutwyler.…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. Post , K. Schilcher

We derive all the O(p^6) Chiral Perturbation Theory low-energy constants from a class of gravity dual models of QCD described by the Yang-Mills and Chern-Simons Lagrangian terms, with the chiral symmetry broken through boundary conditions…

High Energy Physics - Phenomenology · Physics 2015-06-05 P. Colangelo , J. J. Sanz-Cillero , F. Zuo

Chiral symmetry breaking may exhibit significantly different patterns in two chiral limits: N_f=2 massless flavours (m_u=m_d=0, m_s physical) and N_f=3 massless flavours (m_u=m_d=0=m_s=0). Such a difference may arise due to vacuum…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Descotes-Genon

In the presence of photons, the neutral $K_{\ell 4}$ decay, $K^0\to\pi^0\pi^-\ell^+\nu_\ell$, can be parameterized in terms of three vectorial, one anomalous, and one tensorial form factors. We present here analytic expressions of two…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Nehme

We present an improved calculation of all B -> light pseudoscalar formfactors from light-cone sum rules, including one-loop radiative corrections to twist-2 and twist-3 contributions, and leading order twist-4 corrections. The total…

High Energy Physics - Phenomenology · Physics 2017-08-23 Patricia Ball , Roman Zwicky

We develop a unitarity approach to consider the final state interaction corrections to the tree level graphs calculated from Chiral Perturbation Theory ($\chi PT$) allowing the inclusion of explicit resonance fields. The method is discussed…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. A. Oller , E. Oset , J. E. Palomar

A calculation for the one-loop pion vector form-factor in Resonance Chiral Theory is provided in this talk. The amplitude is computed up to next-to-leading order in 1/Nc and, by means of high-energy constraints, we are able to produce a…

High Energy Physics - Phenomenology · Physics 2011-02-01 J. J. Sanz-Cillero

The theoretical and experimental status of the isovector axial-vector current form factors G_A(q^2) and G_P(q^2) of the nucleon is reviewed. We also describe a new calculation of these form factors in manifestly Lorentz-invariant chiral…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. R. Schindler , S. Scherer

At order ${\mathcal O}(\alpha G_{\mathrm F})$, the amplitudes for the decays $K\to\pi \ell^+\ell^-$ involve a form factor given by the matrix element of the time-ordered product of the electromagnetic current with the four-quark operators…

High Energy Physics - Phenomenology · Physics 2019-09-20 Giancarlo D'Ambrosio , David Greynat , Marc Knecht

We properly define off-shell $K\to\pi$ transition amplitudes and use them to extract information for on-shell $K\to\pi\pi$ amplitudes within Chiral Perturbation Theory. At order $p^2$ in the chiral expansion all three parameters of weak…

High Energy Physics - Phenomenology · Physics 2009-10-31 Johan Bijnens , Elisabetta Pallante , Joaquim Prades

The NA48/2 Collaboration at CERN has accumulated unprecedented statistics of rare kaon decays in the Ke4 modes: Ke4(+-) ($K^\pm \to \pi^+ \pi^- e^\pm \nu$) and Ke4(00) ($K^\pm \to \pi^0 \pi^0 e^\pm \nu$) with nearly one percent background…

High Energy Physics - Experiment · Physics 2016-08-10 NA48/2 , NA62 Collaborations , : , F. Ambrosino , A. Antonelli , G. Anzivino , R. Arcidiacono , W. Baldini , S. Balev , J. R. Batley , M. Behler , S. Bifani , C. Biino , A. Bizzeti , B. Bloch-Devaux , G. Bocquet , V. Bolotov , F. Bucci , N. Cabibbo , M. Calvetti , N. Cartiglia , A. Ceccucci , P. Cenci , C. Cerri , C. Cheshkov , J. B. Chèze , M. Clemencic , G. Collazuol , F. Costantini , A. Cotta Ramusino , D. Coward , D. Cundy , A. Dabrowski , G. D'Agostini , P. Dalpiaz , C. Damiani , H. Danielsson , M. De Beer , G. Dellacasa , J. Derré , H. Dibon , D. Di Filippo , L. DiLella , N. Doble , V. Duk , J. Engelfried , K. Eppard , V. Falaleev , R. Fantechi , M. Fidecaro , L. Fiorini , M. Fiorini , T. Fonseca Martin , P. L. Frabetti , A. Fucci , S. Gallorini , L. Gatignon , E. Gersabeck , A. Gianoli , S. Giudici , A. Gonidec , E. Goudzovski , S. Goy Lopez , E. Gushchin , B. Hallgren , M. Hita-Hochgesand , M. Holder , P. Hristov , E. Iacopini , E. Imbergamo , M. Jeitler , G. Kalmus , V. Kekelidze , K. Kleinknecht , V. Kozhuharov , W. Kubischta , V. Kurshetsov , G. Lamanna , C. Lazzeroni , M. Lenti , E. Leonardi , L. Litov , D. Madigozhin , A. Maier , I. Mannelli , F. Marchetto , G. Marel , M. Markytan , P. Marouelli , M. Martini , L. Masetti , P. Massarotti , E. Mazzucato , A. Michetti , I. Mikulec , M. Misheva , N. Molokanova , E. Monnier , U. Moosbrugger , C. Morales Morales , M. Moulson , S. Movchan , D. J. Munday , M. Napolitano , A. Nappi , G. Neuhofer , A. Norton , T. Numao , V. Obraztsov , V. Palladino , M. Patel , M. Pepe , A. Peters , F. Petrucci , M. C. Petrucci , B. Peyaud , R. Piandani , M. Piccini , G. Pierazzini , I. Polenkevich , I. Popov , Yu. Potrebenikov , M. Raggi , B. Renk , F. Retière , P. Riedler , A. Romano , P. Rubin , G. Ruggiero , A. Salamon , G. Saracino , M. Savrié , M. Scarpa , V. Semenov , A. Sergi , M. Serra , M. Shieh , S. Shkarovskiy , M. W. Slater , M. Sozzi , T. Spadaro , S. Stoynev , E. Swallow , M. Szleper , M. Valdata-Nappi , P. Valente , B. Vallage , M. Velasco , M. Veltri , S. Venditti , M. Wache , H. Wahl , A. Walker , R. Wanke , L. Widhalm , A. Winhart , R. Winston , M. D. Wood , S. A. Wotton , O. Yushchenko , A. Zinchenko , M. Ziolkowski

We merge heavy quark effective theory with staggered chiral perturbation theory to calculate heavy-light (B, D) meson quantities. We present results at NLO for the $B(D)$ meson decay constant in the partially quenched and full QCD cases,…

High Energy Physics - Lattice · Physics 2009-11-10 C. Aubin , C. Bernard

We present two-loop calculations on the axial-vector form factors $F_A$ of semileptonic radiative kaon and pion decays in chiral perturbation theory. The relevant dimension-6 terms of the lagrangian are evaluated from the resonance…

High Energy Physics - Phenomenology · Physics 2009-11-10 C. Q. Geng , I-Lin Ho , T. H. Wu

We present a comprehensive study of the electromagnetic form factor, the decay constant and the mass of the pion computed in lattice QCD with two degenerate O(a)-improved Wilson quarks at three different lattice spacings in the range…

High Energy Physics - Lattice · Physics 2015-06-16 Bastian B. Brandt , Andreas Juttner , Hartmut Wittig

The existing Chiral Perturbation Theory (ChPT) calculations at order $p^6$ are reviewed. The principles of ChPT and how they are used are introduced. The main part is a review of the two- and three-flavour full two-loop calculations and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Johan Bijnens

In a recent study [M.C.M. Rentmeester et al., Phys. Rev. C 67, 044001 (2003)], the Nijmegen group reports on the determination of the chiral low-energy constants (LEC), c_3 and c_4, involved in the 2-pi-exchange part of the NN amplitude at…

Nuclear Theory · Physics 2007-05-23 D. R. Entem , R. Machleidt

We perform a complete and systematic calculation of the octet-baryon form factors within the fully covariant approach of SU(3) chiral perturbation theory at O(p^3). We use the extended on-mass shell renormalization scheme, and include…

High Energy Physics - Phenomenology · Physics 2017-11-29 Astrid N. Hiller Blin

This paper summarizes the recent calculations of the masses and decay constants of the pseudoscalar mesons at the two-loop level, or NNLO, in Partially Quenched Chiral Perturbation Theory (PQxPT). Possible applications include chiral…

High Energy Physics - Lattice · Physics 2009-11-11 Timo A. Lahde , Johan Bijnens , Niclas Danielsson
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