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Related papers: Rare Kaon Decays Revisited

200 papers

We carry out a detailed study of the branching fractions and lepton pair invariant-mass spectrum of \tau^- ->\pi^- \nu_\tau l^+l^- decays (l=e,\mu). In addition to the model-independent (QED) contributions, we include the…

High Energy Physics - Phenomenology · Physics 2013-09-03 P. Roig , A. Guevara , G. López Castro

The rare decay $K^\pm\to\pi^\pm\gamma\gamma$ has been recently measured from data samples collected by the NA48/2 and NA62 experiments at CERN. These measurements are presented, including model-independent spectrum measurements and fits to…

High Energy Physics - Experiment · Physics 2019-08-14 Evgueni Goudzovski

We analyse the rare kaon decays $K_S \to \gamma\gamma$ and $K_S \to \gamma\ell^+\ell^-$ $(\ell = e \mbox{ or } \mu)$ in a dispersive framework in which the weak Hamiltonian carries momentum. Our analysis extends predictions from lowest…

High Energy Physics - Phenomenology · Physics 2016-11-14 Gilberto Colangelo , Ramon Stucki , Lewis C. Tunstall

The interplay between short- and long-distance contributions to the K_L-->mu+ mu- decay amplitude is analyzed. The long-distance piece is estimated using chiral perturbation theory techniques and large-N_C considerations, leading to a…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Gomez Dumm , A. Pich

The decay K_L -> pi0 gamma e+ e- occurs at a it higher rate than the nonradiative process K_L -> pi0 e+ e-, and hence can be a background to CP violation studies using the latter reaction. It also has an interest in its own right in the…

High Energy Physics - Phenomenology · Physics 2009-10-30 John F. Donoghue , Fabrizio Gabbiani

The neutral Kaon decays Ks->gamma gamma and Kl->pi0 gamma gamma are very sensitive to higher order loop effects of Chiral Perturbation Theory (ChPT). New measurements of the NA48 experiment show that ChPT contributions of O(p^6) cannot be…

High Energy Physics - Experiment · Physics 2007-05-23 Rainer Wanke

In Ref [1] we have presented the results of an exploratory lattice QCD computation of the long-distance contribution to the $K^+\to\pi^+\nu\bar{\nu}$ decay amplitude. In the present paper we describe the details of this calculation, which…

High Energy Physics - Lattice · Physics 2018-10-24 Ziyuan Bai , Norman H. Christ , Xu Feng , Andrew Lawson , Antonin Portelli , Christopher T. Sachrajda

The rare kaon decays $K\to\pi\nu\bar{\nu}$ are strongly suppressed in the standard model and widely regarded as processes in which new phenomena, not predicted by the standard model, may be observed. Recognizing such new phenomena requires…

High Energy Physics - Lattice · Physics 2016-07-06 Norman H. Christ , Xu Feng , Antonin Portelli , Christopher T. Sachrajda

The following proceedings contain a theory perspective on rare Kaon decays. I review rare kaon decays in the LHC era: we discuss interplay with B-anomalies and possible New Physics in direct CP violation in $K\to 2\pi$: very rare kaon…

High Energy Physics - Phenomenology · Physics 2019-07-15 Giancarlo D'Ambrosio

We update the Standard Model predictions for the rare decays $K^+\to\pi^+\nu\bar\nu$ and $K_L\to\pi^0\nu\bar\nu$. In view of improved limits on $B_s$--$\bar B_s$ mixing we derive a stringent and theoretically clean Standard Model upper…

High Energy Physics - Phenomenology · Physics 2009-10-09 Gerhard Buchalla , Andrzej J. Buras

The estimation of rare K decay matrix-elements from Kl3 experimental data is extended beyond LO in Chiral Perturbation Theory. Isospin-breaking effects at NLO (and partially NNLO) in the ChPT expansion, as well as QED radiative corrections…

High Energy Physics - Phenomenology · Physics 2008-11-26 Federico Mescia , Christopher Smith

The decay K_L -> pi0 e+ e- is being searched for as a signal of direct Delta S = 1 CP violation. We provide a thorough updating of the analysis of the three components of the decay: 1) Direct CP violation, 2) CP violation through the mass…

High Energy Physics - Phenomenology · Physics 2010-11-01 John F. Donoghue , Fabrizio Gabbiani

We evaluate the rare radiative kaon decays K_{L,S} -> 3 gamma. Applying the requirements of gauge invariance and Bose symmetry, we derive a general form of the decay amplitude, including both parity-conserving and parity-violating…

High Energy Physics - Phenomenology · Physics 2010-12-24 Shu-Yu Ho , Jusak Tandean

Most of the analytic approaches which are used at present to understand Kaon decays, get their inspiration from QCD in the limit of a large number of colours $N_c$. After a general overview, we illustrate this with a recent application to…

High Energy Physics - Phenomenology · Physics 2007-05-23 David Greynat , Eduardo de Rafael

We report a first, complete lattice QCD calculation of the long-distance contribution to the $K^+\to\pi^+\nu\bar{\nu}$ decay within the standard model. This is a second-order weak process involving two four-Fermi operators that is highly…

High Energy Physics - Lattice · Physics 2017-06-28 Ziyuan Bai , Norman H. Christ , Xu Feng , Andrew Lawson , Antonin Portelli , Christopher T. Sachrajda

In this paper I will describe the search for rare kaon decay processes $K^+\to \pi^+ \nu \bar\nu$ and $K^0_L \to \pi^0 \nu \bar\nu$. The small decay rate for these processes is considered a key prediction of the standard model. We searched…

High Energy Physics - Experiment · Physics 2007-05-23 Milind V Diwan

We analyze rare kaon decays in models in which the dominant new effect is an enhanced $\bar s d Z$ vertex $Z_{ds}$. We point out that in spite of large theoretical uncertainties the CP-violating ratio $\epsilon^\prime/\epsilon$ provides at…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andrzej J. Buras , Luca Silvestrini

Starting from the Chiral Perturbation Theory Lagrangian, but keeping different masses for the charged and neutral mesons, and using a previously developed non-perturbative unitary scheme that generates the lightest meson-meson resonances,…

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

Meson decays offer a good opportunity to probe new physics. The rare kaon decay $K^+ \rightarrow \pi^+ \nu\bar{\nu}$ is one of the cleanest of them and, for this reason, is rather sensitive to new physics, in particular, vector mediators.…

High Energy Physics - Phenomenology · Physics 2021-06-09 Téssio B. de Melo , Sergey Kovalenko , Farinaldo S. Queiroz , C. Siqueira , Yoxara S. Villamizar

The NA48/2 Collaboration at CERN has accumulated and analysed unprecedented statistics of rare kaon decays in the $K_{e4}$ modes: $K_{e4}(+-)$ ($K^\pm \to \pi^+ \pi^- e^\pm \nu$) and $K_{e4}(00)$ ($K^\pm \to \pi^0 \pi^0 e^\pm \nu$) with…

High Energy Physics - Experiment · Physics 2014-08-05 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. Cheze , 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. Derre , 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. Retiere , P. Riedler , A. Romano , P. Rubin , G. Ruggiero , A. Salamon , G. Saracino , M. Savrie , 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