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Related papers: Invisible neutron decay and light BSM particles

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We investigate mixing of neutrinos in the $\nu$MSM (neutrino Minimal Standard Model), which is the MSM extended by three right-handed neutrinos. Especially, we study elements of the mixing matrix $\Theta_{\alpha I}$ between three…

High Energy Physics - Phenomenology · Physics 2011-04-08 Takehiko Asaka , Shintaro Eijima , Hiroyuki Ishida

In short-baseline experiments such as LSND and MiniBooNE, an excess of electron neutrinos has been observed, originating from a muon neutrino beam. To address this anomaly, in the line of many works, we investigate various neutrino mixing…

High Energy Physics - Phenomenology · Physics 2026-03-06 Priya , Simran Arora , B. C. Chauhan

We extend the Standard Model with the general effective Hamiltonian for the quark level transition $c \to s \ell \nu$ with a complete set of four fermion operators including right-handed neutrinos. The current experimental measurements in…

High Energy Physics - Phenomenology · Physics 2025-04-10 Priyanka Boora , Dinesh Kumar , Kavita Lalwani

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

This is the first paper of our systematic efforts on lepton number violating (LNV) hadronic decays in the effective field theory approach. These decays provide information complementary to popular nuclear neutrinoless double-$\beta$…

High Energy Physics - Phenomenology · Physics 2020-05-26 Yi Liao , Xiao-Dong Ma , Hao-Lin Wang

We present a possibility that the neutrinoless double beta decay can be hidden in the minimal seesaw mechanism where the standard model is extended by two right-handed neutrinos which have a hierarchical mass structure. In this framework,…

High Energy Physics - Phenomenology · Physics 2021-01-18 Takehiko Asaka , Hiroyuki Ishida , Kazuki Tanaka

The extension of Majorana neutrino mass mechanism of the neutrinoless double-beta decay ($0\nu\beta\beta$) with the inclusion of right-handed leptonic and hadronic currents is revisited. While only the exchange of light neutrinos is…

High Energy Physics - Phenomenology · Physics 2015-11-11 Dusan Stefanik , Rastislav Dvornicky , Fedor Simkovic , Petr Vogel

Observation of non-zero neutrino masses at a scale $\sim 10^{-1} - 10^{-2}$ eV is a major problem in the otherwise highly successful Standard Model. The most elegant mechanism to explain such tiny neutrino masses is the seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2016-02-10 S. Chakdar , K. Ghosh , V. Hoang , P. Q. Hung , S. Nandi

The invisible signals of right-handed sneutrino decays originating from a Z' are analysed at the Large Hadron Collider. The possibility of accessing these events helps disentangling the B-L extension of Minimal Supersymmetric Standard Model…

High Energy Physics - Phenomenology · Physics 2015-09-28 W. Abdallah , J. Fiaschi , S. Khalil , S. Moretti

This paper reports results from a search for nucleon decay through 'invisible' modes, where no visible energy is directly deposited during the decay itself, during the initial water phase of SNO+. However, such decays within the oxygen…

High Energy Physics - Experiment · Physics 2019-08-12 SNO+ Collaboration , : , M. Anderson , S. Andringa , E. Arushanova , S. Asahi , M. Askins , D. J. Auty , A. R. Back , Z. Barnard , N. Barros , D. Bartlett , F. Barão , R. Bayes , E. W. Beier , A. Bialek , S. D. Biller , E. Blucher , R. Bonventre , M. Boulay , D. Braid , E. Caden , E. J. Callaghan , J. Caravaca , J. Carvalho , L. Cavalli , D. Chauhan , M. Chen , O. Chkvorets , K. J. Clark , B. Cleveland , C. Connors , I. T. Coulter , D. Cressy , X. Dai , C. Darrach , B. Davis-Purcell , M. M. Depatie , F. Descamps , F. Di Lodovico , N. Duhaime , F. Duncan , J. Dunger , E. Falk , N. Fatemighomi , V. Fischer , E. Fletcher , R. Ford , N. Gagnon , K. Gilje , P. Gorel , K. Graham , C. Grant , J. Grove , S. Grullon , E. Guillian , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , M. Hedayatipour , W. J. Heintzelman , J. Heise , R. L. Helmer , J. L. Hernández-Hernández , B. Hreljac , J. Hu , T. Iida , A. S. Inácio , C. M. Jackson , N. A. Jelley , C. J. Jillings , C. Jones , P. G. Jones , K. Kamdin , T. Kaptanoglu , J. Kaspar , K. Keeter , C. Kefelian , P. Khaghani , L. Kippenbrock , J. R. Klein , R. Knapik , J. Kofron , L. L. Kormos , B. Krar , C. Kraus , C. B. Krauss , T. Kroupova , K. Labe , I. Lam , C. Lan , B. J. Land , R. Lane , S. Langrock , A. LaTorre , I. Lawson , L. Lebanowski , G. M. Lefeuvre , E. J. Leming , A. Li , J. Lidgard , B. Liggins , X. Liu , Y. Liu , V. Lozza , M. Luo , S. Maguire , A. Maio , K. Majumdar , S. Manecki , J. Maneira , R. D. Martin , E. Marzec , A. Mastbaum , N. McCauley , A. B. McDonald , J. E. McMillan , P. Mekarski , M. Meyer , C. Miller , M. Mlejnek , E. Mony , I. Morton-Blake , M. J. Mottram , S. Nae , M. Nirkko , V. Novikov , H. M. O'Keeffe , E. O'Sullivan , G. D. Orebi Gann , M. J. Parnell , J. Paton , S. J. M. Peeters , T. Pershing , Z. Petriw , L. Pickard , D. Pracsovics , G. Prior , J. C. Prouty , S. Quirk , A. Reichold , R. Richardson , M. Rigan , A. Robertson , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , M. A. Schumaker , M. H. Schwendener , D. Scislowski , J. Secrest , M. Seddighin , L. Segui , S. Seibert , I. Semenec , T. Shantz , T. M. Shokair , L. Sibley , J. R. Sinclair , K. Singh , P. Skensved , T. Sonley , R. Stainforth , M. Strait , M. I. Stringer , R. Svoboda , A. Sörensen , B. Tam , J. Tatar , L. Tian , N. Tolich , J. Tseng , H. W. C. Tseung , E. Turner , R. Van Berg , J. G. C. Veinot , C. J. Virtue , B. von Krosigk , E. Vázquez-Jáuregui , J. M. G. Walker , M. Walker , J. Wang , O. Wasalski , J. Waterfield , J. J. Weigand , R. F. White , J. R. Wilson , T. J. Winchester , P. Woosaree , A. Wright , J. P. Yanez , M. Yeh , T. Zhao , K. Zuber , A. Zummo

The mass estimates of active and sterile (right-handed) neutrinos are considered at the phenomenological level using the seesaw mechanism. It is assumed that the neutrino mass values depend on three characteristic scales, and the sum of the…

High Energy Physics - Phenomenology · Physics 2025-05-13 V. V. Khruschov , S. V. Fomichev

The extension of the Standard Model by right handed neutrinos with masses in the GeV range can simultaneously explain the observed neutrino masses via the seesaw mechanism and the baryon asymmetry of the universe via leptogenesis. It has…

High Energy Physics - Phenomenology · Physics 2017-01-18 Marco Drewes , Shintaro Eijima

Joint analysis of the results of the Neutrino-4 experiment and the data of the GALLEX, SAGE and BEST experiments confirms the parameters of neutrino oscillations declared by the Neutrino-4 experiment $(\Delta m_{14}^2= 7.3 \text{eV}^2$ and…

High Energy Physics - Phenomenology · Physics 2024-04-22 A. P. Serebrov , R. M. Samoilov , O. M. Zherebtsov , N. S. Budanov

The Majorana nature of neutrinos will be the confirmed by the observation of the rare process called as neutrinoless double beta decay process, i.e. the simultaneous decay of two neutrons in the nucleus of an isotope (A, Z) into two protons…

High Energy Physics - Phenomenology · Physics 2022-04-27 Pritam Kumar Bishee , Purushottam Sahu , Sudhanwa Patra

If the heaviest neutrino mass eigenstate is unstable, its decay modes could include lighter neutrino eigenstates. In this case part of the decay products could be visible, as they would interact at neutrino detectors via mixing. At neutrino…

High Energy Physics - Phenomenology · Physics 2017-05-11 Pilar Coloma , Orlando L. G. Peres

A right-handed neutrino is a promising candidate for dark matter (DM) which has no interaction with nuclei. Since two right-handed neutrinos explain neutrino oscillation data and baryon number asymmetry through both the seesaw mechanism and…

High Energy Physics - Phenomenology · Physics 2026-02-17 Daijiro Suematsu

If the only contribution to neutrinoless double beta decay (NLDBD) are neutrino masses its discovery may be very difficult, especially if neutrinos present a normal hierarchy spectrum. However, this is not the only possibility; NLDBD can in…

High Energy Physics - Phenomenology · Physics 2013-05-22 F. del Águila , A. Aparici , S. Bhattacharya , A. Santamaria , J. Wudka

The see-saw mechanism is usually applied to explain the lightness of neutrinos. The traditional see-saw mechanism introduces at least two right-handed neutrinos for the realistic neutrino spectrum. In the case of supersymmetry, loop…

High Energy Physics - Phenomenology · Physics 2014-12-01 Yi-Lei Tang

If the Standard Model particle content is extended by gauge singlet fermions (right-handed neutrinos), active neutrinos generically acquire (Majorana) masses, in agreement with our current understanding of the lepton sector. If the…

High Energy Physics - Phenomenology · Physics 2007-07-11 Andre de Gouvea

We study the indirect effects of New Physics in the Higgs decay into four charged leptons, using an Effective Field Theory (EFT) approach to Higgs interactions. We evaluate the deviations induced by the EFT dimension-six operators in…

High Energy Physics - Phenomenology · Physics 2018-02-14 S. Boselli , C. M. Carloni Calame , G. Montagna , O. Nicrosini , F. Piccinini , A. Shivaji