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We consider proton decay in theories that contain large extra dimensions. If virtual black hole states are allowed by the theory, as is generally the case, then proton decay can proceed via virtual black holes. The experimental limits on…

High Energy Physics - Phenomenology · Physics 2009-10-31 Fred C. Adams , Gordon L. Kane , Manasse Mbonye , Malcolm J. Perry

We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upper bound is $4\pi v^2/\sqrt 3 m_\nu$, where $v \simeq 246$ GeV is the weak scale and $m_\nu$ is the Majorana neutrino mass. For neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. M. Niczyporuk

We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upper bound is $4\pi v^2/\sqrt 3 m_\nu$, where $v \simeq 246$ GeV is the weak scale and $m_\nu$ is the Majorana neutrino mass. For neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. Maltoni , J. M. Niczyporuk , S. Willenbrock

We study proton decay in finite supersymmetric SU(5) grand unified theories. We find that the dimension-five operators due to color triplet higgsino induce too rapid a proton decay. This behaviour can be traced to the large Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2011-07-19 N. Deshpande , Xiao-Gang He , E. Keith

A search for long-lived particles decaying to photons and weakly interacting particles, using proton-proton collision data at $\sqrt{s} =$ 13 TeV collected by the CMS experiment in 2016-2017 is presented. The data set corresponds to an…

High Energy Physics - Experiment · Physics 2019-12-18 CMS Collaboration

The article provides a theoretical substantiation for a significant increase in the level of accuracy in determining the neutron lifetime using an alternative concept of neutron beta decay. Neutrons are distributed among different subsets…

Nuclear Theory · Physics 2023-08-03 V. V. Vasiliev

The logarithmic running of the gauge couplings alpha_1, alpha_2 and alpha_3, indicates that they may unify at some scale M_GUT ~ 10^16. This is often taken to imply that the standard model gauge group is embedded into some larger simple…

High Energy Physics - Phenomenology · Physics 2007-05-23 Neal Weiner

In the framework of a baryon-number-violating effective Lagrangian, we calculate improved lower bounds on partial lifetimes for proton and bound neutron decays, including $p \to \ell^+ \ell'^+ \ell'^-$, $n \to \bar\nu \ell^+ \ell'^-$, $p…

High Energy Physics - Phenomenology · Physics 2019-12-17 Sudhakantha Girmohanta , Robert Shrock

The lifetime of the Lambda-hyperon for the nonmesonic decay Lambda N ---> N N has been determined by a measurement at COSY Juelich of the delayed fission of heavy hypernuclei produced in proton - Au collisions at T_p=1.9 GeV. It is found…

High Energy Physics - Experiment · Physics 2009-10-31 B. Kamys , P. Kulessa , H. Ohm , K. Pysz , Z. Rudy , H. Stroeher , W. Cassing

Even if the concerns related to the naturalness of the electroweak scale are repressed, the Higgs mass and stability of the electroweak vacuum do not allow arbitrarily large supersymmetry breaking scale, $M_S$, in the minimal models with…

High Energy Physics - Phenomenology · Physics 2020-07-01 V. Suryanarayana Mummidi , Ketan M. Patel

We study the lifetimes of TeV-scale heavy neutral leptons (Majorana neutrinos) that appear in a model suggested by Okamura et al. [2]. We develop a convenient way to parametrize the neutrino mass texture of the model, and illustrate our…

High Energy Physics - Phenomenology · Physics 2009-09-29 Alexey Pronin , Tatsu Takeuchi

By considering the constraints from nucleon decay we obtain upper limits on tan beta in generalized supersymmetric SU(5) grand unified theories with gauge-mediated supersymmetry breaking. We find that the predicted values of tan beta in…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. Hamidian , K. Huitu , K. Puolamaki , D. -X. Zhang

The modern theories of Grand Unification (GUT) and supersymmetric (SUSY) extensions of standard model (SM) suppose that the conservation laws of the SM may be violated to some small degree. The nuclei are well-suited as a laboratory to test…

High Energy Physics - Phenomenology · Physics 2011-04-15 Amand Faessler , Fedor Simkovic

Recently, a new mechanism, which explains why the three gauge coupling constants meet at a certain scale in the minimal supersymmetric standard model, has been proposed in a scenario of grand unified theories with anomalous $U(1)_A$ gauge…

High Energy Physics - Phenomenology · Physics 2009-11-07 Nobuhiro Maekawa , Toshifumi Yamashita

We give a detailed renormalization group analysis for the SU(16) grandunified group with general breaking chains in which quarks and leptons transform separately at intermediate energies. Our analysis includes the effects of Higgs bosons.…

High Energy Physics - Phenomenology · Physics 2009-10-22 N. G. Deshpande , E. Keith , Palash B. Pal

It is shown that in realistic SUSY GUT models of quark and lepton masses both the proton decay rate and branching ratios differ in general from those predicted in the minimal $SU(5)$ supersymmetric model. The observation of proton decay,…

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

Dark Matter is essential for structure formation in the late Universe so it must be stable on cosmological time scales. But how stable exactly? Only assuming decays into relativistic particles, we report an otherwise model independent bound…

Cosmology and Nongalactic Astrophysics · Physics 2015-01-19 Benjamin Audren , Julien Lesgourgues , Gianpiero Mangano , Pasquale Dario Serpico , Thomas Tram

We show that in supersymmetric grand unified theories new effective D=4 and D=5 operators for proton decay are induced by soft SUSY-breaking terms, when heavy GUT gauge bosons are integrated out, in addition to the standard D=6 ones. As a…

High Energy Physics - Phenomenology · Physics 2009-11-11 Zurab Berezhiani , Fabrizio Nesti , Luigi Pilo

A review is given of recent developments on the implications of supergravity grand unification with SU(5)-type proton decay under the condition $M_{H_3} /m_G < 10$ (where $M_{H_3}$ is the Higgs triplet mass) and the naturalness condition…

High Energy Physics - Phenomenology · Physics 2009-09-25 Pran Nath , R. Arnowitt

At present, the strongest upper limit on $\sum m_{\nu}$, the sum of neutrino masses, is from cosmological measurements. However, this bound assumes that the neutrinos are stable on cosmological timescales, and is not valid if the neutrino…

High Energy Physics - Phenomenology · Physics 2020-05-04 Zackaria Chacko , Abhish Dev , Peizhi Du , Vivian Poulin , Yuhsin Tsai