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Related papers: The mass of the tau neutrinos

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In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Freitas , W. Porod , P. M. Zerwas

We compute the cross section for neutrino-photon scattering taking into account a neutrino mass. We explore the possibility of using intense neutrino beams, such as those available at proposed muon colliders, together with high powered…

High Energy Physics - Phenomenology · Physics 2009-10-31 Duane A. Dicus , Wayne W. Repko , Roberto Vega

In a wide class of unified models there is an additional (and possibly dominant) term in the neutrino mass formula that under the simplest assumption takes the form M_{\nu} = (M_N + M_N^T)u/M_G, where M_N is the neutrino Dirac mass matrix,…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr

The sum of the masses of the three neutrino mass eigenstates is now constrained both from above and below, and lies between 55 and 6900 meV. The lower limit is set by neutrino oscillations and the fact that masses are non-negative. The…

Nuclear Experiment · Physics 2009-07-24 R. G. Hamish Robertson

A mechanism for generating massive but naturally light Dirac neutrinos is proposed. It involves composite Higgs within the standard model as well as some new interaction beyond the standard model. According to this scenario, a neutrino mass…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. P. Divakaran , G. Rajasekaran

In this letter, we show that upper-limits on neutrino mass translate into upper-limits on the class of neutrino-matter interactions that can generate loop corrections to the neutrino mass matrix. We apply our results to $\mu$- and…

High Energy Physics - Phenomenology · Physics 2016-08-16 Gary Prézeau , Andriy Kurylov

The D^+ --> omega + pi^+ decay is studied by decomposing its amplitude into a sum of factorizable and non-factorizable ones. Its rate is predicted as a function of mass and width of a hypothetical hybrid meson.

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Terasaki

The impact of unstable Majorana tau neutrinos on primordial nucleosynthesis is considered. The mass and lifetime of nu_tau are taken in the intervals 0.1-20 MeV and 0.001-400 sec respectively. The studied decay modes are nu_tau -> nu_mu +…

High Energy Physics - Phenomenology · Physics 2009-09-25 A. D. Dolgov , S. H. Hansen , S. Pastor , D. V. Semikoz

The existence of a neutrino magnetic moment implies contributions to the neutrino mass via radiative corrections. We derive model-independent "naturalness" upper bounds on the magnetic moments of Dirac neutrinos, generated by physics above…

High Energy Physics - Phenomenology · Physics 2009-11-11 Nicole F. Bell , V. Cirigliano , M. J. Ramsey-Musolf , P. Vogel , Mark B. Wise

By combining experimental constraints from atmospheric and solar neutrino oscillations and the tritium beta decay endpoint, we infer upper limits of 4.4 eV on the $\nu_\mu$ and $\nu_\tau$ masses, if the universe consists of three neutrinos.…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , T. J. Weiler , K. Whisnant

We study the origin of neutrino mass from $SO(10)$ arising from $M$ Theory compactified on a $G_2$-manifold. This is linked to the problem of the breaking of the extra $U(1)$ gauge group, in the $SU(5)\times U(1)$ subgroup of $SO(10)$,…

High Energy Physics - Phenomenology · Physics 2016-12-21 Bobby S. Acharya , Krzysztof Bozek , Miguel Crispim Romão , Stephen F. King , Chakrit Pongkitivanichkul

In this lecture we review some of the basic properties of neutrinos, in particular their mass and the oscillation behavior. First we discuss how to describe the neutrino mass. Then, under the assumption that neutrinos are massive and mixed,…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. W. Kim

We consider the rate at which energy is emitted by neutrinos from the dense interior of neutron stars containing a Bose condensate of pions or kaons. The rates obtained are larger, by a factor of 2, than those found earlier, and are…

Nuclear Theory · Physics 2016-09-08 V. Thorsson , M. Prakash , T. Tatsumi , C. J. Pethick

Decays of B mesons to states involving tau leptons can be used as a tool to search for the effects of new physics, such as those involving a charged Higgs boson. The experimental status of the decays B -> tau nu and B -> D^(*) tau nu is…

High Energy Physics - Experiment · Physics 2009-03-30 M. Barrett

Searches for heavy neutrinos often rely on the possibility that the heavy neutrinos will decay to detectable particles. Interpreting the results of such searches requires a particular model for the heavy-neutrino decay. We present a method…

High Energy Physics - Phenomenology · Physics 2015-03-16 Andrew Kobach , Sean Dobbs

Under the assumption of symmetric four zero texture for fermion mass matrices in SO(10) model, the neutrino Dirc mass matrix is derived from the up-quark mass matrix. By adjusting two scales of the Majorana mass sector, we can derive…

High Energy Physics - Phenomenology · Physics 2007-05-23 Masako Bando , Midori Obara

If the generating mechanism for neutrino mass is to account for both the newly observed muon anomalous magnetic moment as well as the present experimental bounds on lepton flavor nonconservation, then the neutrino mass matrix should be…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma , Martti Raidal

We study possible contributions of heavy sterile neutrinos $\nu_h$ to the decays $\tau^-\to e^{\pm}(\mu^{\pm})\pi^{\mp}\pi^-$. From the experimental upper bounds on their rates we derive new constraints on the $\nu_h-\nu_{\tau}$ mixing in…

High Energy Physics - Phenomenology · Physics 2009-11-07 Vladimir Gribanov , Sergey Kovalenko , Ivan Schmidt

In spite of the general belief that neutrinos are Majorana particles, their character should be revealed experimentally. We begin by discussing why it is so difficult in terrestrial experiments. If neutrinos are Majorana particles, the…

High Energy Physics - Phenomenology · Physics 2011-04-15 M. Czakon , J. Gluza , M. Zralek