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Related papers: Inverse Neutrinoless Double Beta Decay Revisited

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The low-energy neutrino physics constraints on the TeV scale type I see-saw scenarios of neutrino mass generation are revisited. It is shown that lepton charge (L) violation, associated to the production and decays of heavy Majorana…

High Energy Physics - Phenomenology · Physics 2015-05-27 A. Ibarra , E. Molinaro , S. T. Petcov

We have studied the correlations among the three absolute neutrino mass observables - the effective Majorana mass ($m_{ee}$) which can be obtained from neutrinoless double beta decay, the electron neutrino mass ($m_{\beta}$) which is…

High Energy Physics - Phenomenology · Physics 2021-03-31 Srubabati Goswami , Vishnudath K N

Doubly charged Higgs s-channel resonances are analyzed in the $e^-e^- \to W^-W^-$ process. In our analysis recent stringent constraint on an effective neutrino mass $<m_{\nu}>$ coming from neutrinoless double-$\beta$ decay is implemented.…

High Energy Physics - Phenomenology · Physics 2009-10-30 Janusz Gluza

We interpret the newly observed muon g-2 anomaly in the framework of a leptonic Higgs doublet model with nearly degenerate neutrino masses and nearly bi-maximal neutrino mixing. Useful constraints are obtained on the rates of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Zhi-zhong Xing

The $\nu_M{\rm SM}$ is defined as the SM extended to include dimension-5 operators. In this model neutrino masses violate lepton number, and two parameters of the lepton mixing matrix, the Majorana phases, are yet to be constrained. One…

High Energy Physics - Phenomenology · Physics 2024-10-16 Avital Dery , Stefania Gori , Yuval Grossman , Zoltan Ligeti

We report a search for the lepton-flavor-violating decays $\tau^{\pm}\to\ell^{\pm}\alpha$~($\ell=e,\mu$), where $\alpha$ is an undetected spin-0 particle, such as an axion-like particle using $736\times10^{6}$ tau lepton pairs collected by…

High Energy Physics - Experiment · Physics 2025-07-11 Belle Collaboration , K. Uno , K. Hayasaka , K. Inami , H. Aihara , R. Ayad , Sw. Banerjee , K. Belous , J. Bennett , M. Bessner , D. Biswas , D. Bodrov , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , G. De Nardo , G. De Pietro , F. Di Capua , J. Dingfelder , Z. Doležal , P. Ecker , D. Epifanov , T. Ferber , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , Y. Guan , K. Gudkova , C. Hadjivasiliou , T. Hara , H. Hayashii , D. Herrmann , C. -L. Hsu , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Y. Jin , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , E. Kovalenko , P. Krokovny , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , T. Lam , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , Y. Ma , M. Masuda , T. Matsuda , D. Matvienko , F. Meier , M. Merola , K. Miyabayashi , G. B. Mohanty , M. Nakao , H. Nakazawa , A. Natochii , M. Niiyama , S. Nishida , S. Ogawa , H. Ono , S. Pardi , J. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , L. E. Piilonen , T. Podobnik , S. Prell , E. Prencipe , M. T. Prim , G. Russo , S. Sandilya , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , W. Shan , J. -G. Shiu , B. Shwartz , F. Simon , J. B. Singh , E. Solovieva , M. Starič , M. Sumihama , M. Takizawa , K. Tanida , F. Tenchini , K. Trabelsi , S. Uehara , T. Uglov , Y. Unno , S. Uno , M. -Z. Wang , E. Won , B. D. Yabsley , Y. Yook , C. Z. Yuan , L. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich

Neutrinoless double beta decay ($\beta\beta0\nu$) is among the only realistic probes of Majorana neutrinos. In the standard scenario, dominated by light neutrino exchange, the process amplitude is proportional to $m_{ee}$, the $e-e$ element…

High Energy Physics - Phenomenology · Physics 2010-05-27 James Jenkins

Neutrino are massless in the Standard Model. The most popular mechanism to generate neutrino masses are the type I and type II seesaw, where right-handed neutrinos and a scalar triplet are augmented to the Standard Model, respectively. In…

High Energy Physics - Phenomenology · Physics 2020-01-08 Manoel M. Ferreira , Tessio B. de Melo , Sergey Kovalenko , Paulo R. D. Pinheiro , Farinaldo S. Queiroz

We have searched for lepton-flavor-violating $\tau$ decays with a pseudoscalar meson ($\eta$, $\eta'$ {and} $\pi^0$) using a data sample of 401 fb$^{-1}$ collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. No…

High Energy Physics - Experiment · Physics 2019-08-14 Y. Miyazaki

A search for rare lepton decays of the eta meson was performed using the WASA detector at CELSIUS. Two candidates for double Dalitz decay eta->e+e-e+e- events are reported with a background of 1.3+/-0.2 events. This allows to set an upper…

In this work we introduce CPT-odd non-minimal Lorentz-symmetry violating couplings to the electroweak sector modifying the interaction between leptons and gauge bosons. The vertex rules allow us to calculate tree-level processes modified by…

High Energy Physics - Phenomenology · Physics 2020-04-08 Y. M. P. Gomes , P. C. Malta , M. J. Neves

In this paper we study the Lepton Flavor Violating $Z$ boson decays $Z \to \tau \mu$ and $Z \to \tau e$ in the context of low scale seesaw models with new heavy Majorana neutrinos whose masses could be reachable at the LHC. Our computations…

High Energy Physics - Phenomenology · Physics 2017-04-26 V. De Romeri , M. J. Herrero , X. Marcano , F. Scarcella

We study the search potential of heavy triplet leptons in Type III Seesaw mechanism at future high-energy and high-luminosity muon colliders. The impact of up-to-date neutrino oscillation results is taken into account on neutrino parameters…

High Energy Physics - Phenomenology · Physics 2022-09-27 Tong Li , Han Qin , Chang-Yuan Yao , Man Yuan

Lepton number violation (LNV) can be induced by Majorana neutrinos in four-body decays of the neutral B meson and the top quark. We study the effects of Majorana neutrinos in these |\Delta L|=2 decays in an scenario where a single heavy…

High Energy Physics - Phenomenology · Physics 2011-12-05 D. Delepine , G. Lopez Castro , N. Quintero

We investigate baryon number violating (BNV) nucleon decays into three leptons from noncontact contributions that are induced by dimension-6 (dim-6) BNV operators in low-energy effective field theory (LEFT) with an exchange of a baryon,…

High Energy Physics - Phenomenology · Physics 2026-04-13 Jing Chen , Yi Liao , Xiao-Dong Ma , Hao-Lin Wang

Using a three neutrino framework we investigate bounds for the effective Majorana neutrino mass matrix. The mass measured in neutrinoless double beta decay is its (11) element. Lepton-number and -flavor violating processes sensitive to each…

High Energy Physics - Phenomenology · Physics 2011-02-07 W. Rodejohann

A general Lorentz--invariant parameterization for the long-range part of the $0\nu\beta\beta$ decay rate is derived. Combined with the short range part this general parameterization in terms of effective $B-L$ violating couplings will allow…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. Päs , M. Hirsch , H. V. Klapdor-Kleingrothaus , S. G. Kovalenko

Angular and energy distributions for leptons and bottom quarks in the process e+e- --> t tbar --> l/b ... have been calculated assuming the most general top-quark couplings. The double distributions depend both on modification of the…

High Energy Physics - Phenomenology · Physics 2016-11-03 B. Grzadkowski , Z. Hioki

We consider the possibility of Lorentz-invariance violation in weak-decay processes. We present a general approach that entails modifying the W-boson propagator by adding a Lorentz-violating tensor to it. We describe the effects of Lorentz…

High Energy Physics - Phenomenology · Physics 2017-08-23 J. P. Noordmans , H. W. Wilschut , R. G. E. Timmermans

We give predictions for the neutrinoless double beta decay rate in a simple variant of the A_4 family symmetry model. We show that there is a lower bound for the neutrinoless double beta decay amplitude even in the case of normal…

High Energy Physics - Phenomenology · Physics 2014-11-18 M. Hirsch , Ernest Ma , J. W. F. Valle , A. Villanova del Moral