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Related papers: Observable Neutron-Anti-Neutron Oscillation, Baryo…

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We show that in a large class of supersymmetric models with spontaneously broken B-L symmetry, neutron--antineutron oscillations occur at an observable level even though the scale of B-L breaking is very high, v_{B-L} ~ 2 x 10^{16} GeV, as…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. S. Babu , R. N. Mohapatra

We discuss a realistic high scale ($v_{BL}\sim 10^{12}$ GeV) supersymmetric seesaw model based on the gauge group $SU(2)_L\times SU(2)_R\times SU(4)_c$ where neutron-anti-neutron oscillation can occur at an observable rate. This is contrary…

High Energy Physics - Phenomenology · Physics 2009-11-11 Bhaskar Dutta , Yukihiro Mimura , R. N. Mohapatra

The discovery of neutrino masses has provided strong hints in favor of the possibility that B-L symmetry is an intimate feature of physics beyond the standard model. I discuss how important information about this symmetry as well as other…

High Energy Physics - Phenomenology · Physics 2015-05-13 R. N. Mohapatra

Next-generation experiments, such as the Deep Underground Neutrino Experiment and the European Spallation Source, are set to improve sensitivity to neutron-antineutron oscillation, a direct probe of $\Delta B = 2$ baryon number violation,…

High Energy Physics - Phenomenology · Physics 2025-10-01 Ilja Dorsner , Svjetlana Fajfer , Shaikh Saad

In the near future, the Deep Underground Neutrino Experiment and the European Spallation Source aim to reach unprecedented sensitivity in the search for neutron-antineutron ($n\text{-}\bar{n}$) oscillations, whose observation would directly…

High Energy Physics - Phenomenology · Physics 2021-11-18 Kåre Fridell , Julia Harz , Chandan Hati

Fundamental symmetry tests of baryon number violation in low-energy experiments can probe beyond the Standard Model (BSM) explanations of the matter-antimatter asymmetry of the universe. Neutron-antineutron oscillations are predicted to be…

High Energy Physics - Lattice · Physics 2019-05-20 Enrico Rinaldi , Sergey Syritsyn , Michael L. Wagman , Michael I. Buchoff , Chris Schroeder , Joseph Wasem

The evidence for neutrino oscillations leads to small neutrino masses, which can be realized by means of the seesaw mechanism. In this framework, baryogenesis may be achieved from leptogenesis.

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Falcone

In the canonical seesaw mechanism of neutrino mass, lepton number is only multiplicatively conserved, which enables the important phenomenon of leptogenesis to occur, as an attractive explanation of the present baryon asymmetry of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma

A non-supersymmetric inverse seesaw model of neutrino mass based on the $A^{\prime}_5$ modular symmetry is presented. This framework provides a combined explanation for neutrino masses, mixing, and the cosmic baryon asymmetry through…

High Energy Physics - Phenomenology · Physics 2026-03-20 Xianshuo Zhang , Yakefu Reyimuaji

We discuss the predictions for neutron-anti-neutron oscillation in various supersymmetric and non-supersymmetric grand unified theories. It is pointed out that in a new class of superstring inspired grand unified theories of $E_6$-type that…

High Energy Physics - Phenomenology · Physics 2009-09-25 R. N. Mohapatra

Considering a six-dimensional geometry orbifolded on $S^1/Z_2\times S^1/Z_2$ with quarks and leptons localised on orthogonal branes, we show that the construction admits observable $n-\bar{n}$ oscillation while naturally suppressing the…

High Energy Physics - Phenomenology · Physics 2022-08-31 Mathew Thomas Arun , Debajyoti Choudhury

It has been recently proposed that the matter-antimatter asymmetry of the universe may have its origin in "post-sphaleron baryogenesis" (PSB). It is a TeV scale mechanism that is testable at the LHC and other low energy experiments. In this…

High Energy Physics - Phenomenology · Physics 2009-02-18 K. S. Babu , P. S. Bhupal Dev , R. N. Mohapatra

We study the model with three right-handed neutrinos which masses are smaller than the weak scale ${\cal O}(10^2)$ GeV (called as the $\nu$MSM). The model can explain the origin of neutrino masses by the seesaw mechanism, offer a candidate…

High Energy Physics - Phenomenology · Physics 2015-06-02 Takehiko Asaka , Shintaro Eijima , Kazuhiro Takeda

We numerically study the correlation between CP violation in the neutrino oscillations and baryogenesis in the seesaw model. In this study we get the heavy Majorana neutrino masses and lepton number asymmetries from their decays by fitting…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. Endoh , T. Morozumi , A. Purwanto

As a baryon number violating process with $\Delta B=2$, neutron-antineutron oscillation ($n\to\bar n$) provides a unique test of baryon number conservation. We have performed a search for $n\to\bar n$ oscillation with bound neutrons in…

High Energy Physics - Experiment · Physics 2021-01-27 Kamiokande Collaboration , K. Abe , C. Bronner , Y. Hayato , M. Ikeda , S. Imaizumi , H. Ito , J. Kameda , Y. Kataoka , M. Miura , S. Moriyama , Y. Nagao , M. Nakahata , Y. Nakajima , S. Nakayama , T. Okada , K. Okamoto , A. Orii , G. Pronost , H. Sekiya , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , T. Yano , R. Akutsu , S. Han , T. Kajita , K. Okumura , T. Tashiro , R. Wang , J. Xia , D. Bravo-Berguño , L. Labarga , Ll. Marti , B. Zaldivar , F. d. M. Blaszczyk , E. Kearns , J. D. Gustafson , J. L. Raaf , J. L. Stone , L. Wan , T. Wester , J. Bian , N. J. Griskevich , W. R. Kropp , S. Locke , S. Mine , M. B. Smy , H. W. Sobel , V. Takhistov , P. Weatherly , J. Hill , J. Y. Kim , I. T. Lim , R. G. Park , B. Bodur , K. Scholberg , C. W. Walter , A. Coffani , O. Drapier , S. El Hedri , A. Giampaolo , M. Gonin , Th. A. Mueller , P. Paganini , B. Quilain , T. Ishizuka , T. Nakamura , J. S. Jang , J. G. Learned , L. H. V. Anthony , A. A. Sztuc , Y. Uchida , V. Berardi , M. G. Catanesi , E. Radicioni , N. F. Calabria , L. N. Machado , G. De Rosa , G. Collazuol , F. Iacob , M. Lamoureux , N. Ospina , L. Ludovici , Y. Nishimura , S. Cao , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , T. Matsubara , T. Nakadaira , M. Jakkapu , K. Nakamura , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , Y. Nakano , T. Shiozawa , A. T. Suzuki , Y. Takeuchi , S. Yamamoto , A. Ali , Y. Ashida , J. Feng , S. Hirota , A. K. Ichikawa , T. Kikawa , M. Mori , T. Nakaya , R. A. Wendell , K. Yasutome , P. Fernandez , N. McCauley , P. Mehta , A. Pritchard , K. M. Tsui , Y. Fukuda , Y. Itow , H. Menjo , T. Niwa , K. Sato , M. Tsukada , P. Mijakowski , M. Posiadala-Zezula , C. K. Jung , C. Vilela , M. J. Wilking , C. Yanagisawa , M. Harada , K. Hagiwara , T. Horai , H. Ishino , S. Ito , Y. Koshio , W. Ma , N. Piplani , S. Sakai , Y. Kuno , G. Barr , D. Barrow , L. Cook , A. Goldsack , S. Samani , C. Simpson , D. Wark , F. Nova , T. Boschi , F. Di Lodovico , S. Molina Sedgwick , M. Taani , S. Zsoldos , J. Y. Yang , S. J. Jenkins , J. M. McElwee , M. D. Thiesse , L. F. Thompson , M. Malek , O. Stone , H. Okazawa , S. B. Kim , I. Yu , K. Nishijima , M. Koshiba , N. Ogawa , K. Iwamoto , M. Yokoyama , K. Martens , M. R. Vagins , M. Kuze , S. Izumiyama , M. Tanaka , T. Yoshida , M. Inomoto , M. Ishitsuka , R. Matsumoto , K. Ohta , M. Shinoki , J. F. Martin , H. A. Tanaka , T. Towstego , M. Hartz , A. Konaka , P. de Perio , N. W. Prouse , B. W. Pointon , S. Chen , B. D. Xu , B. Richards , B. Jamieson , J. Walker , A. Minamino , K. Okamoto , G. Pintaudi , R. Sasaki

It is usually believed that the observation of the neutrino-antineutrino (${\nu}$-$\bar{\nu}$) oscillations is almost impossible since the oscillation probabilities are expected to be greatly suppressed by the square of tiny ratio of…

High Energy Physics - Phenomenology · Physics 2017-04-05 Chao-Qiang Geng , Da Huang

A simplified but very instructive analysis of the seesaw mechanism is here performed. Assuming a nearly diagonal Dirac neutrino mass matrix, we study the forms of the Majorana mass matrix of right-handed neutrinos, which reproduce the…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Falcone

Heavy neutrinos with masses below the electroweak scale can simultaneously generate the light neutrino masses via the seesaw mechanism and the baryon asymmetry of the universe via leptogenesis. The requirement to explain these phenomena…

High Energy Physics - Phenomenology · Physics 2017-09-13 Marco Drewes , Bjorn Garbrecht , Dario Gueter , Juraj Klaric

A sensitive search for neutron-antineutron oscillations can provide a unique probe of some of the central questions in particle physics and cosmology: the energy scale and mechanism for baryon number violation, the origin of the…

Instrumentation and Detectors · Physics 2015-10-07 David Milstead

The detection of neutron-antineutron oscillation will be a discovery of fundamental importance in particle physics and cosmology. In models discussed widely in literature, the process is generated through heavy New Physics with weak,…

High Energy Physics - Phenomenology · Physics 2023-03-22 Mathew Thomas Arun
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