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Related papers: Experimental evidence for G.U.T. Proton Decay

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We discuss the status of supersymmetric grand unified theories [SUSY GUTs] with regards to the observation of proton decay. In this talk we focus on SUSY GUTs in 4 dimensions. We outline the major theoretical uncertainties present in the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stuart Raby

In the supersymmetric grand unified theories (SUSY GUTs), gauge bosons associated with the unified gauge group induce proton decay. We investigate the proton decay rate via the gauge bosons in the SUSY GUTs under the two situations; one is…

High Energy Physics - Phenomenology · Physics 2012-09-21 Junji Hisano , Daiki Kobayashi , Natsumi Nagata

We calculate the proton lifetime in an SO(10) supersymmetric grand unified theory [SUSY GUT] with U(2) family symmetry. This model fits the low energy data, including the recent data for neutrino oscillations. We discuss the predictions of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Radovan Dermisek

We have searched for nucleon decay into five two-body final states using a 4.4 kiloton-year fiducial exposure of the Soudan 2 iron tracking calorimeter. For proton decay into the fully visible final states mu+ eta and e+ eta, we observe…

High Energy Physics - Experiment · Physics 2008-11-26 D. Wall

Current laboratory bounds imply that protons are extremely long-lived. However, this conclusion may not hold for all time and in all of space. We find that the proton lifetime can be $\sim 15$ orders of magnitude shorter in the relatively…

High Energy Physics - Phenomenology · Physics 2025-03-03 Hooman Davoudiasl , Peter B. Denton

Models of supersymmetric grand unified theories based on SU(5)_GUT \times U(N)_H gauge group (N = 2,3) have a symmetry that guarantees light Higgs doublets and absence of dimension-five proton decay operators. We analysed the proton decay…

High Energy Physics - Phenomenology · Physics 2009-11-10 Masahiro Ibe , T. Watari

A minimal renormalizable SUSY SO(10) model with B-L symmetry broken by {\bf 126} Higgs field has recently been shown to predict all neutrino mixings and the ratio $\Delta m^2_{\odot}/\Delta m^2_A$ in agreement with observations. Unlike…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. S. Goh , R. N. Mohapatra , S. Nasri , Siew-Phang Ng

We consider proton decay and $g_\mu - 2$ in flipped SU(5) GUT models. We first study scenarios in which the soft supersymmetry-breaking parameters are constrained to be universal at some high scale $M_{in}$ above the standard GUT scale…

High Energy Physics - Phenomenology · Physics 2022-01-05 John Ellis , Jason L. Evans , Natsumi Nagata , Dimitri V. Nanopoulos , Keith A. Olive

Proton decay is a generic prediction of GUT models and is therefore an important channel to detect the existence of unification or to set limits on GUT models. Current bounds on the proton lifetime are around 10^33 years, which sets…

High Energy Physics - Phenomenology · Physics 2013-05-30 Adam Martin , Gerben C. Stavenga

An experimental observation of proton decay would be a spectacular proof of grand unification. Currently, the best constraint on the proton lifetime for the p->e+ pi0 decay channel, coming from the Super-Kamiokande experiment, reaches…

Nuclear Theory · Physics 2009-04-24 Dorota Stefan , Artur M. Ankowski

In preparation for upcoming nucleon decay searches at Hyper-Kamiokande, it is important to derive a theoretical upper bound on the proton lifetime in a general class of grand unified theory (GUT) models. In this paper, we make an attempt…

High Energy Physics - Phenomenology · Physics 2019-04-24 Naoyuki Haba , Yukihiro Mimura , Toshifumi Yamada

Data from the Sudbury Neutrino Observatory have been used to constrain the lifetime for nucleon decay to ``invisible'' modes, such as n -> 3 nu. The analysis was based on a search for gamma-rays from the de-excitation of the residual…

High Energy Physics - Experiment · Physics 2012-08-27 SNO Collaboration

We have searched for proton decay via $p \rightarrow \nu K^{+}$ using Super-Kamiokande data from April 1996 to February 2013, 260 kiloton$\cdot$year exposure in total. No evidence for this proton decay mode is found. A lower limit of the…

We have searched for proton decay via p -> e+ pi0 using data from a 25.5 kton-year exposure of the Super-Kamiokande detector. We find no candidate events with an expected background induced by atmospheric neutrinos of 0.1 events. From these…

High Energy Physics - Experiment · Physics 2012-08-27 Kamiokande Collaboration , M. Shiozawa

Semi-simple unification is one of a model which naturally solves two difficulties in the supersymmetric grand unification theory: doublet-triplet splitting problem and suppression of dimension 5 proton decay. We analyzed the dimension 6…

High Energy Physics - Phenomenology · Physics 2009-11-07 Masaaki Fujii , T. Watari

We study the proton lifetime in the $SO(10)$ Grand Unified Theory (GUT), which has the left-right (LR) symmetric gauge theory below the GUT scale. In particular, we focus on the minimal model without the bi-doublet Higgs field in the LR…

High Energy Physics - Phenomenology · Physics 2020-06-24 Yuta Hamada , Masahiro Ibe , Yu Muramatsu , Kin-ya Oda , Norimi Yokozaki

The unification of gauge interactions in the context of Adjoint SU(5) and its phenomenological consequences are investigated. We show the allowed mass spectrum of the theory which is compatible with proton decay, and discuss the possibility…

High Energy Physics - Phenomenology · Physics 2008-07-17 Pavel Fileviez Perez , Hoernisa Iminniyaz , German Rodrigo

A search for proton decay into $e^+/\mu^+$ and a $\eta$ meson has been performed using data from a 0.373 Mton$\cdot$year exposure (6050.3 live days) of Super-Kamiokande. Compared to previous searches this work introduces an improved model…

High Energy Physics - Experiment · Physics 2024-10-01 Kamiokande Collaboration , N. Taniuchi , K. Abe , S. Abe , Y. Asaoka , C. Bronner , M. Harada , Y. Hayato , K. Hiraide , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , R. Kaneshima , Y. Kashiwagi , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Okamoto , K. Sato , H. Sekiya , H. Shiba , K. Shimizu , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , S. Watanabe , T. Yano , T. Kajita , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , G. D. Megias , P. Fernandez , L. Labarga , N. Ospina , B. Zaldivar , B. W. Pointon , E. Kearns , J. Mirabito , J. L. Raaf , L. Wan , T. Wester , J. Bian , N. J. Griskevich , W. R. Kropp , S. Locke , M. B. Smy , H. W. Sobel , V. Takhistov , A. Yankelevich , J. Hill , M. C. Jang , J. Y. Kim , S. H. Lee , I. T. Lim , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , L. Bernard , A. Coffani , O. Drapier , S. El Hedri , A. Giampaolo , Th. A. Mueller , A. D. Santos , P. Paganini , R. Rogly , T. Nakamura , J. S. Jang , L. N. Machado , J. G. Learned , K. Choi , N. Iovine , S. Cao , L. H. V. Anthony , D. Martin , N. W. Prouse , M. Scott , A. A. Sztuc , Y. Uchida , V. Berardi , N. F. Calabria , M. G. Catanesi , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Lamoureux , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , C. Fujisawa , S. Horiuchi , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , R. Okazaki , R. Akutsu , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , M. Jakkapu , T. Matsubara , T. Nakadaira , K. Nakamura , Y. Oyama , A. Portocarrero Yrey , K. Sakashita , T. Sekiguchi , T. Tsukamoto , N. Bhuiyan , T. Boschi , G. T. Burton , F. Di Lodovico , J. Gao , A. Goldsack , T. Katori , J. Migenda , R. M. Ramsden , M. Taani , Z. Xie , S. Zsoldos , Y. Kotsar , H. Ozaki , A. T. Suzuki , Y. Takagi , Y. Takeuchi , S. Yamamoto , H. Zhong , J. Feng , L. Feng , S. Han , J. R. Hu , Z. Hu , M. Kawaue , T. Kikawa , M. Mori , T. Nakaya , R. A. Wendell , K. Yasutome , S. J. Jenkins , N. McCauley , P. Mehta , A. Tarrant , M. J. Wilking , Y. Fukuda , Y. Itow , H. Menjo , K. Ninomiya , Y. Yoshioka , J. Lagoda , M. Mandal , P. Mijakowski , Y. S. Prabhu , J. Zalipska , M. Jia , J. Jiang , C. K. Jung , W. Shi , C. Yanagisawa , Y. Hino , H. Ishino , S. Ito , H. Kitagawa , Y. Koshio , W. Ma , F. Nakanishi , S. Sakai , T. Tada , T. Tano , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , S. Jung , J. Y. Yang , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , O. Stone , P. Stowell , M. D. Thiesse , L. F. Thompson , S. T. Wilson , H. Okazawa , S. M. Lakshmi , S. B. Kim , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , A. K. Ichikawa , K. D. Nakamura , S. Tairafune , K. Nishijima , M. Koshiba , A. Eguchi , S. Goto , K. Iwamoto , Y. Mizuno , T. Muro , K. Nakagiri , Y. Nakajima , S. Shima , E. Watanabe , M. Yokoyama , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , S. Izumiyama , M. Kuze , R. Matsumoto , K. Terada , R. Asaka , M. Inomoto , M. Ishitsuka , H. Ito , T. Kinoshita , Y. Ommura , N. Shigeta , M. Shinoki , T. Suganuma , K. Yamauchi , T. Yoshida , Y. Nakano , J. F. Martin , H. A. Tanaka , T. Towstego , R. Gaur , V. Gousy-Leblanc , M. Hartz , A. Konaka , X. Li , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , M. Posiadala-Zezula , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , S. Amanai , A. Minamino , G. Pintaudi , S. Sano , R. Sasaki , R. Shibayama , R. Shimamura , S. Suzuki , K. Wada

We discuss proton decay in a recently proposed model of supersymmetric hybrid inflation based on the gauge symmetry $SU(4)_c \times SU(2)_L \times SU(2)_R$. A $U(1)\, R$ symmetry plays an essential role in realizing inflation as well as in…

High Energy Physics - Phenomenology · Physics 2020-10-15 George Lazarides , Mansoor Ur Rehman , Qaisar Shafi

We present a search for the proton decay mode $p \rightarrow \overline{\nu} K^{+}$ based on an exposure of 8.97 kton-years in the KamLAND experiment. The liquid scintillator detector is sensitive to successive signals from $p \rightarrow…

High Energy Physics - Experiment · Physics 2015-09-25 KamLAND Collaboration
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