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Related papers: $K\to\pi\nu\bar\nu$ spectra and NA62 interpretatio…

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The excellent experimental prospects to measure the invisible mass spectrum of the $K^+\to\pi^+\nu\bar\nu$ decay opens a new path to test generalised quark--neutrino interactions with flavour changing $s\to d$ transitions and as such to…

High Energy Physics - Phenomenology · Physics 2024-07-03 Martin Gorbahn , Ulserik Moldanazarova , Kai Henryk Sieja , Emmanuel Stamou , Mustafa Tabet

In this work we investigate the implication of $K\to \pi \nu \bar{\nu}$ from the recent KOTO and NA62 measurements for generic neutrino interactions and the new physics scale in effective field theories. The interactions between quarks and…

High Energy Physics - Phenomenology · Physics 2020-04-10 Tong Li , Xiao-Dong Ma , Michael A. Schmidt

Results from the study of the rare decays $K^+\to\pi^+\nu\bar{\nu}$, $K^{+}\rightarrow\pi^{+}\mu^{+}\mu^{-}$ and $K^{+}\rightarrow\pi^{+}\gamma\gamma$ at the NA62 experiment at CERN are interpreted in terms of improved limits for…

High Energy Physics - Experiment · Physics 2025-10-22 NA62 Collaboration

We obtain the complete and independent bases of effective operators at mass dimension 5, 6, 7, 8, 9 in both standard model effective field theory with light sterile right-handed neutrinos ($\nu$SMEFT) and low energy effective field theory…

High Energy Physics - Phenomenology · Physics 2021-11-24 Hao-Lin Li , Zhe Ren , Ming-Lei Xiao , Jiang-Hao Yu , Yu-Hui Zheng

We explore the constraints on new physics from the recent NA62 observation of the kaon decay $K^+\to\pi^+$+$\not{\!\!E}$ with missing energy $\not{\!\!E}$ in the context of a dark-matter (DM) scenario recently used to accommodate the Belle…

High Energy Physics - Phenomenology · Physics 2025-09-19 Xiao-Gang He , Xiao-Dong Ma , Jusak Tandean , German Valencia

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 2016-11-16 Matthew Moulson

We compute the contribution of the decays $K_L \rightarrow \pi^0 Q \bar Q$ and $K^+ \rightarrow \pi^+ Q \bar Q$, where $Q$ is a dark fermion of the dark sector, to the measured widths for the rare decays $K^+\rightarrow \pi^+ \nu \bar \nu$…

High Energy Physics - Phenomenology · Physics 2020-07-15 Marco Fabbrichesi , Emidio Gabrielli

The recently proposed "mini-seesaw mechanism" combines naturally suppressed Dirac and Majorana masses to achieve light Standard Model neutrinos via a low-scale seesaw. A key feature of this approach is the presence of multiple light (order…

High Energy Physics - Phenomenology · Physics 2011-11-15 Michael Duerr , Damien P. George , Kristian L. McDonald

$K\rightarrow \pi\nu \bar\nu$ is one of the theoretically cleanest meson decay where to look for indirect effects of new physics complementary to LHC searches. The NA62 experiment at CERN SPS is designed to measure the branching ratio of…

High Energy Physics - Experiment · Physics 2019-03-27 Silvia Martellotti

The Grossman-Nir bound concept is robust, but the common perception of $K_L \to \pi^0\nu\bar\nu < 1.4 \times 10^{-9}$ may be circumvented. Because of the blinding $K\pi2$(3) decay, $K^+$ decay experiments such as E787/E949 and the currently…

High Energy Physics - Phenomenology · Physics 2016-11-30 George W. S. Hou

The latest search for the rare kaon decay $K^+\to\pi^+\nu\bar\nu$ by the NA62 experiment has produced evidence for it with a branching fraction consistent with the prediction of the standard model. The new result implies that in this decay,…

High Energy Physics - Phenomenology · Physics 2020-12-23 Chao-Qiang Geng , Jusak Tandean

$K^{+}\rightarrow\pi^{+}\nu\overline{\nu}$ is one of the theoretically cleanest meson decay where to look for indirect effects of new physics complementary to LHC searches. The NA62 experiment at CERN SPS is designed to measure the…

High Energy Physics - Experiment · Physics 2019-08-12 NA62 Collaboration , G. Aglieri Rinella , R. Aliberti , F. Ambrosino , R. Ammendola , B. Angelucci , A. Antonelli , G. Anzivino , R. Arcidiacono , I. Azhinenko , S. Balev , M. Barbanera , J. Bendotti , A. Biagioni , L. Bician , C. Biino , A. Bizzeti , T. Blazek , A. Blik , B. Bloch-Devaux , V. Bolotov , V. Bonaiuto , M. Boretto , M. Bragadireanu , D. Britton , G. Britvich , M. B. Brunetti , D. Bryman , F. Bucci , F. Butin , J. Calvo , E. Capitolo , C. Capoccia , T. Capussela , A. Cassese , A. Catinaccio , A. Cecchetti , A. Ceccucci , P. Cenci , V. Cerny , C. Cerri , B. Checcucci , O. Chikilev , S. Chiozzi , R. Ciaranfi , G. Collazuol , A. Conovaloff , P. Cooke , P. Cooper , G. Corradi , E. Cortina Gil , F. Costantini , F. Cotorobai , 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 , S. Di Lorenzo , N. Dixon , N. Doble , B. Dobrich , V. Duk , V. Elsha , J. Engelfried , T. Enik , N. Estrada , V. Falaleev , R. Fantechi , V. Fascianelli , L. Federici , S. Fedotov , A. Filippi , M. Fiorini , J. Fry , J. Fu , A. Fucci , L. Fulton , S. Gallorini , S. Galeotti , E. Gamberini , L. Gatignon , G. Georgiev , S. Ghinescu , A. Gianoli , M. Giorgi , S. Giudici , L. Glonti , A. Goncalves Martins , F. Gonnella , E. Goudzovski , R. Guida , E. Gushchin , F. Hahn , B. Hallgren , H. Heath , F. Herman , T. Husek , O. Hutanu , D. Hutchcroft , L. Iacobuzio , E. Iacopini , E. Imbergamo , O. Jamet , P. Jarron , E. Jones , T. Jones K. Kampf , J. Kaplon , V. Kekelidze , S. Kholodenko , G. Khoriauli , A. Khotyantsev , A. Khudyakov , Yu. Kiryushin , A. Kleimenova , K. Kleinknecht , A. Kluge , M. Koval , V. Kozhuharov , M. Krivda , Z. Kucerova , Yu. Kudenko , J. Kunze , G. Lamanna , G. Latino , C. Lazzeroni , G. Lehmann-Miotto , R. Lenci , M. Lenti , E. Leonardi , P. Lichard , R. Lietava , V. Likhacheva , L. Litov , R. Lollini , D. Lomidze , A. Lonardo , M. Lupi , N. Lurkin , K. McCormick , D. Madigozhin , G. Maire , C. Mandeiro , I. Mannelli , G. Mannocchi , A. Mapelli , F. Marchetto , R. Marchevski , S. Martellotti , P. Massarotti , K. Massri , P. Matak , E. Maurice , M. Medvedeva , A. Mefodev , E. Menichetti , E. Migliore , E. Minucci , M. Mirra , M. Misheva , N. Molokanova , J. Morant , M. Morel , M. Moulson , S. Movchan , D. Munday , M. Napolitano , I. Neri , F. Newson , J. Noël , A. Norton , M. Noy , G. Nuessle , T. Numao , V. Obraztsov , A. Ostankov , S. Padolski , R. Page , V. Palladino , G. Paoluzzi , C. Parkinson , E. Pedreschi , M. Pepe , F. Perez Gomez , M. Perrin-Terrin , L. Peruzzo , P. Petrov , F. Petrucci , R. Piandani , M. Piccini , D. Pietreanu , J. Pinzino , I. Polenkevich , L. Pontisso , 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 , C. Santoni , G. Saracino , F. Sargeni , V. Semenov , A. Sergi , M. Serra , A. Shaikhiev , S. Shkarovskiy , I. Skillicorn , D. Soldi , A. Sotnikov , V. Sugonyaev , M. Sozzi , T. Spadaro , F. Spinella , R. Staley , A. Sturgess , P. Sutcliffe , N. Szilasi , D. Tagnani , S. Trilov , M. Valdata-Nappi , P. Valente , M. Vasile , T. Vassilieva , B. Velghe , M. Veltri , S. Venditti , P. Vicini , R. Volpe , M. Vormstein , H. Wahl , R. Wanke , P. Wertelaers , A. Winhart , R. Winston , B. Wrona , O. Yushchenko , M. Zamkovsky , A. Zinchenko

While all models of Majorana neutrino masses lead to the same dimension five effective operator, which does not conserve lepton number, the dimension six operators induced at low energies conserve lepton number and differ depending on the…

High Energy Physics - Phenomenology · Physics 2009-01-06 A. Abada , C. Biggio , F. Bonnet , M. B. Gavela , T. Hambye

We consider, in a model-independent framework, the potential for observing dark matter in neutrino detectors through the interaction $\bar{f} p \to e^+ n$, where $f$ is a dark fermion. Operators of dimension six or less are considered, and…

High Energy Physics - Phenomenology · Physics 2009-10-19 Jennifer Kile

The possibility of direct detection of light fermionic dark matter in neutrino detectors is explored from a model-independent standpoint. We consider all operators of dimension six or lower which can contribute to the interaction $\bar{f} p…

High Energy Physics - Phenomenology · Physics 2010-01-07 Jennifer Kile , Amarjit Soni

We discuss electroweak precision constraints on dimension-6 operators in the effective theory beyond the standard model. We identify the combinations of these operators that are constrained by the pole observables (the W and Z masses and…

High Energy Physics - Phenomenology · Physics 2015-06-23 Adam Falkowski , Francesco Riva

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 NA62 experiment at CERN reports searches for $K^+\to\mu^+N$ and $K^+\to\mu^+\nu X$ decays, where $N$ and $X$ are massive invisible particles, using the 2016-2018 data set. The $N$ particle is assumed to be a heavy neutral lepton, and…

High Energy Physics - Experiment · Physics 2021-04-08 NA62 collaboration

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

Using chiral low energy theorems and elastic unitarity assumption, the $\tau\to\pi K \nu $ decay is investigated. The vector and scalar $\pi K$ form factors are calculated. It is found that the $\pi K$ spectrum is dominated by the $K^*$…

High Energy Physics - Phenomenology · Physics 2009-10-28 L. Beldjoudi , Tran N. Truong
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