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Related papers: Experimental results on $K_L$ decays

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The rare decays $\mathrm{K}^+\to \pi^+ \nu \bar{\nu}$ and $\mathrm{K_L}\to \pi^0 \nu \bar{\nu}$ are extremely attractive processes to study flavor physics because they are both exceptionally clean from a theoretical point of view. These…

High Energy Physics - Experiment · Physics 2019-06-21 Michal Zamkovsky

We have previously analysed the chiral predictions for the decay K_L -> pi0 gamma e+ e- and discussed how experimental measurements of this process can help our understanding of chiral theories and of CP tests. Motivated by the possibility…

High Energy Physics - Phenomenology · Physics 2009-10-31 John F. Donoghue , Fabrizio Gabbiani

This letter is the first report of the KL -> pi+- e-+ nu e+ e- decay. Based on 19208+-144 events, we determine the branching fraction, B(KL -> pi+- e-+ nu e+ e-; Mee > 5 MeV/c^2, E*ee > 30 MeV) = (1.285+-0.041)x10^-5, and Gamma(Ke3ee; Mee…

High Energy Physics - Experiment · Physics 2012-08-27 KTeV Collaboration

Precise measurements of the branching ratios for the flavor-changing neutral current decays $K\to\pi\nu\bar{\nu}$ can provide unique constraints on CKM unitarity and, potentially, evidence for new physics. It is important to measure both…

High Energy Physics - Experiment · Physics 2020-08-26 Matthew Moulson

We analyze $K_L$ lepton pair decays of $K_L \to l^+\l^-\gamma$ and $K_L \to l^+l^-l'^+l'^-$ $(l, l'=e, \mu)$ within the framework of the light-front QCD approach (LFQA). With the $K_L \to \gamma^* \gamma^*$ form factors evaluated in a model…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. Q. Geng , C. W. Hwang

We analyse the $\overline B_s^0\to K^+l^-\bar \nu$ and $\overline B_s^0\to K^{*+}(\to K\pi) \ell^-\bar \nu$ decays that are valuable for extracting the CKM matrix element $|V_{ub}|$. We calculate the differential and integrated partial…

High Energy Physics - Phenomenology · Physics 2014-08-06 Ulf-G. Meißner , Wei Wang

Based on 3.26 fb$^{-1}$ data sample collected at CLEO III, we study the decay $\tau^-\to K^+K^-\pi^-\nu_\tau$, and improve the measurement of the branching ratio ${\cal B}(\tau^-\to K^+K^-\pi^-\nu_\tau)= (1.59\pm0.06\pm0.13)\times10^{-3}$,…

High Energy Physics - Experiment · Physics 2019-08-16 Feng Liu

We present new results on the related rare KL decay modes KL -> pi+ pi- gamma and KL -> pi+ pi- e+ e-. KTeV has performed the first direct measurement of the form factor for the "direct emission" component of KL -> pi+ pi- gamma decays, a…

High Energy Physics - Experiment · Physics 2007-05-23 John Belz

The first dedicated search for the rare neutral-kaon decay $K_L^0\to\pi^0\nu\bar{\nu}$ has been carried out in the E391a experiment at the KEK 12-GeV proton synchrotron. The final upper limit of 2.6 $\times 10^{-8}$ at the 90% confidence…

High Energy Physics - Experiment · Physics 2015-03-13 The E391a Collaboration , J. K. Ahn

The NA62 experiment will begin taking data in 2015. Its primary purpose is a 10% measurement of the branching ratio of the ultrarare kaon decay $K^+ \to \pi^+ \nu \bar{ \nu }$, using the decay in flight of kaons in an unseparated beam with…

High Energy Physics - Experiment · Physics 2014-11-04 G. Aglieri Rinella , R. Aliberti , F. Ambrosino , B. Angelucci , A. Antonelli , G. Anzivino , R. Arcidiacono , I. Azhinenko , S. Balev , J. Bendotti , A. Biagioni , C. Biino , A. Bizzeti , T. Blazek , A. Blik , B. Bloch-Devaux , V. Bolotov , V. Bonaiuto , M. Bragadireanu , D. Britton , G. Britvich , N. Brook , F. Bucci , V. Buescher , F. Butin , E. Capitolo , C. Capoccia , T. Capussela , V. Carassiti , N. Cartiglia , A. Cassese , A. Catinaccio , A. Cecchetti , A. Ceccucci , P. Cenci , V. Cerny , C. Cerri , O. Chikilev , R. Ciaranfi , G. Collazuol , P. Cooke , P. Cooper , G. Corradi , E. Cortina Gil , F. Costantini , A. Cotta Ramusino , D. Coward , G. D'Agostini , J. Dainton , P. Dalpiaz , H. Danielsson , J. Degrange , N. De Simone , D. Di Filippo , L. Di Lella , N. Dixon , N. Doble , V. Duk , V. Elsha , J. Engelfried , T. Enik , V. Falaleev , R. Fantechi , L. Federici , M. Fiorini , J. Fry , A. Fucci , L. Fulton , S. Gallorini , L. Gatignon , A. Gianoli , S. Giudici , L. Glonti , A. Goncalves Martins , F. Gonnella , E. Goudzovski , R. Guida , E. Gushchin , F. Hahn , B. Hallgren , H. Heath , F. Herman , D. Hutchcroft , E. Iacopini , O. Jamet , P. Jarron , K. Kampf , J. Kaplon , V. Karjavin , V. Kekelidze , S. Kholodenko , G. Khoriauli , A. Khudyakov , Yu. Kiryushin , K. Kleinknecht , A. Kluge , M. Koval , V. Kozhuharov , M. Krivda , Y. Kudenko , J. Kunze , G. Lamanna , C. Lazzeroni , R. Leitner , R. Lenci , M. Lenti , E. Leonardi , P. Lichard , R. Lietava , L. Litov , D. Lomidze , A. Lonardo , N. Lurkin , D. Madigozhin , G. Maire , A. Makarov , I. Mannelli , G. Mannocchi , A. Mapelli , F. Marchetto , P. Massarotti , K. Massri , P. Matak , G. Mazza , E. Menichetti , M. Mirra , M. Misheva , N. Molokanova , J. Morant , M. Morel , M. Moulson , S. Movchan , D. Munday , M. Napolitano , F. Newson , A. Norton , M. Noy , G. Nuessle , V. Obraztsov , S. Padolski , R. Page , V. Palladino , A. Pardons , E. Pedreschi , M. Pepe , F. Perez Gomez , M. Perrin-Terrin , P. Petrov , F. Petrucci , R. Piandani , M. Piccini , D. Pietreanu , J. Pinzino , M. Pivanti , I. Polenkevich , I. Popov , Yu. Potrebenikov , D. Protopopescu , F. Raffaelli , M. Raggi , P. Riedler , A. Romano , P. Rubin , G. Ruggiero , V. Russo , V. Ryjov , A. Salamon , G. Salina , V. Samsonov , E. Santovetti , G. Saracino , F. Sargeni , S. Schifano , V. Semenov , A. Sergi , M. Serra , S. Shkarovskiy , A. Sotnikov , V. Sougonyaev , M. Sozzi , T. Spadaro , F. Spinella , R. Staley , M. Statera , P. Sutcliffe , N. Szilasi , D. Tagnani , M. Valdata-Nappi , P. Valente , M. Vasile , V. Vassilieva , B. Velghe , M. Veltri , S. Venditti , M. Vormstein , H. Wahl , R. Wanke , P. Wertelaers , A. Winhart , R. Winston , B. Wrona , O. Yushchenko , M. Zamkovsky , A. Zinchenko

The decay $K^+ \to \pi^+\nu\bar{\nu}$ is highly suppressed in the Standard Model (SM), while its rate can be predicted with minimal theoretical uncertainty. The branching ratio (BR) for this decay is thus a sensitive probe of the flavor…

High Energy Physics - Experiment · Physics 2013-10-30 Matthew Moulson

Recent results a future prospects of the NA62 experiment at CERN SPS are presented. The NA62 experiment performed the most precise measurement of the ratio $R_K$ of the $K^+\rightarrow e^\pm\nu$ and K^+\rightarrow \mu^\pm\nu$ decay rates…

High Energy Physics - Experiment · Physics 2012-12-21 Giuseppe Ruggiero

The NA48/2 experiment at CERN collected a large sample of charged kaon decays into final states with multiple charged particles in 2003--2004. A new upper limit on the rate of the lepton number violating decay…

High Energy Physics - Experiment · Physics 2016-11-23 Karim Massri

The long-distance and non-local parts of the form factors describing the single-photon mediated $K_{S,L}\to\pi^0\gamma^*\to\pi^0\ell^+\ell^-$ ($\ell = e, \mu$) transitions in the standard model are addressed in QCD in the limit where the…

High Energy Physics - Phenomenology · Physics 2024-09-16 Giancarlo D'Ambrosio , Marc Knecht

We report on a study of the decay $K_L \to e^+e^-\gamma\gamma$ carried out as a part of the KTeV/E799 experiment at Fermilab. The 1997 data yielded a sample of 1543 events, including an expected background of $56 \pm 8$ events. An effective…

High Energy Physics - Experiment · Physics 2008-11-26 The KTeV Collaboration , A. Alavi-Harati

We calculate the momentum dependent form factors of $P \to \gamma^* \gamma^*$($P=\pi^{0}, \eta$) within the light-front quark model. Using the form factors, we examine the decays of $P \to l^+ l^-$, $P \to l^+ l^- \gamma$ and $P \to l^+ l^-…

High Energy Physics - Phenomenology · Physics 2011-04-20 Chong-Chung Lih

The ratio $R_K = \Gamma(K^{\pm}\to e^{\pm}\nu(\gamma)) / \Gamma(K^{\pm}\to\mu^{\pm}\nu(\gamma))$ provides a powerful probe of the structure of weak interactions. It is calculated with very high precision within the Standard Model, but…

High Energy Physics - Experiment · Physics 2008-04-30 Evgueni Goudzovski

We calculate the branching ratios of the $K^+ \to \pi^0 l^+ \nu_l\gamma (l = e, \mu)$ decays, and the T-odd triple momenta correlations $\xi=\vec{q}\cdot[\vec{p}_l \times \vec{p}_\pi]/M^3_K$, due to the electromagnetic final state…

High Energy Physics - Phenomenology · Physics 2015-05-20 I. B. Khriplovich , A. S. Rudenko

The CERN NA62 experiment uses a novel "kaon decay-in-flight" technique to observe $K^+ \to \pi^+ \nu \overline{\nu}$. The preliminary result based on the analysis of the full 2016 dataset will be presented. In agreement with the Standard…

High Energy Physics - Experiment · Physics 2018-10-17 Bob Velghe
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