English
Related papers

Related papers: Dimension-six Proton Decays in the Modified Missin…

200 papers

We study a renormalizable SUSY $SO(10)$ GUT model where the Yukawa couplings of single ${\bf 10}$, single ${\bf \overline{126}}$ and single ${\bf 120}$ fields, $Y_{10},Y_{126},Y_{120}$, account for the quark and lepton Yukawa couplings and…

High Energy Physics - Phenomenology · Physics 2021-02-17 Naoyuki Haba , Yukihiro Mimura , Toshifumi Yamada

Without supersymmetry, the gauge couplings in the standard model with five Higgs doublets unify around 10^14 GeV. In this case, the trinified model, SU(3)_C x SU(3)_L x SU(3)_R x Z_3, with the minimal Higgs sector required for symmetry…

High Energy Physics - Phenomenology · Physics 2008-11-26 Soren Wiesenfeldt

We comment on the status and prospects of the minimal non-supersymmetric renormalizable SO(10) grand unified model. We emphasize its unique predictive power owing to the particular robustness of the gauge unification pattern to the…

High Energy Physics - Phenomenology · Physics 2014-10-29 Helena Kolešová , Michal Malinský

We have searched for proton decay via $p \rightarrow e^{+} \pi^{0}$ and $p \rightarrow \mu^{+} \pi^{0}$ using Super-Kamiokande data from April 1996 to March 2015, 0.306 megaton$\cdot$years exposure in total. The atmospheric neutrino…

High Energy Physics - Experiment · Physics 2017-01-11 M. Miura

It is pointed out that a class of flipped SU(5) models based on F-theory naturally explains the gauge coupling unification. It is because the group SU(5) x U(1)_X is embedded in SO(10) and E_8. To prohibit the dimension 4 and 5 proton decay…

High Energy Physics - Theory · Physics 2015-05-27 Kang-Sin Choi , Bumseok Kyae

A non-minimal, semi-realistic version of supersymmetric SU(5) grand unified theory is discussed. The solution of the doublet-triplet splitting problem leads to a better agreement between the predicted and observed values of the low-energy…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ferruccio Feruglio

Proton decay, although unobserved so far, is a natural expectation when attempting to explain the baryon asymmetry of the universe. $p\to K^+\bar{\nu}$ or $p\to K^+\tilde{\chi}_1^0$, with $\tilde{\chi}_1^0$ a light exotic neutral particle,…

High Energy Physics - Phenomenology · Physics 2024-03-28 Florian Domingo , Herbi K. Dreiner , Dominik Köhler , Saurabh Nangia , Apoorva Shah

We consider the interplay of the muon $g-2$ anomaly and the proton decay in the SUSY SU(5) GUTs with generation-independent scalar soft masses. In these scenarios, we introduce a number of $\bf 5+{\bar 5}$ messenger fields with…

High Energy Physics - Phenomenology · Physics 2024-04-02 Seong-Sik Kim , Hyun Min Lee , Sung-Bo Sim

Current theoretical and experimental issues are reviewed in the light of the recent SuperKamiokande discovery. By using quark-lepton symmetries, derived from Grand Unification and/or string theories, we show how to determine the necessary…

High Energy Physics - Phenomenology · Physics 2014-11-17 P. Ramond

We perform a detailed study of the grand unified theories $SO(10)$ and $E(6)$ with left-right intermediate gauge symmetries of the form $SU(N)_L\otimes SU(N)_R \otimes \mathcal{G}$. Proton decay lifetime constrains the unification scale to…

High Energy Physics - Phenomenology · Physics 2018-05-16 Joydeep Chakrabortty , Rinku Maji , Subhendra Mohanty , Sunando Kumar Patra , Tripurari Srivastava

In the standard model the proton is protected from decay naturally by gauge symmetries, whereas in the ordinary minimal supersymmetric standard model an ad hoc discrete symmetry is imposed for the proton stability. We present a new…

High Energy Physics - Phenomenology · Physics 2009-10-31 Mayumi Aoki , Noriyuki Oshimo

We propose a $SU(5) \times U(1)_X \times U(1)_{PQ}$ model, where $U(1)_X$ is the generalization of the $B-L$ (baryon minus lepton number) gauge symmetry and $U(1)_{PQ}$ is the global Peccei-Quinn (PQ) symmetry. There are four fermions…

High Energy Physics - Phenomenology · Physics 2021-10-04 Nobuchika Okada , Digesh Raut , Qaisar Shafi

The unification of gauge coupling constants in the minimal supersymmetric model (MSSM) is unaffected at the one-loop level by the inclusion of additional mass-degenerate SU(5) multiplets. Perturbativity puts an upper limit on the number of…

High Energy Physics - Phenomenology · Physics 2016-09-01 Ralf Hempfling

Minimal supersymmetric hybrid inflation utilizes a canonical Kahler potential and a renormalizable superpotential which is uniquely determined by imposing a U(1) R-symmetry. In computing the scalar spectral index $n_s$ we take into account…

High Energy Physics - Phenomenology · Physics 2014-11-20 Mansoor Ur Rehman , Qaisar Shafi , Joshua R. Wickman

Using 0.37 megaton$\cdot$years of exposure from the Super-Kamiokande detector, we search for 10 dinucleon and nucleon decay modes that have a two-body final state with no hadrons. These baryon and lepton number violating modes have the…

High Energy Physics - Experiment · Physics 2018-12-03 Kamiokande Collaboration , S. Sussman , K. Abe , C. Bronner , Y. Hayato , M. Ikeda , K. Iyogi , J. Kameda , Y. Kato , Y. Kishimoto , Ll. Marti , M. Miura , S. Moriyama , T. Mochizuki , M. Nakahata , Y. Nakajima , Y. Nakano , S. Nakayama , T. Okada , K. Okamoto , A. Orii , G. Pronost , H. Sekiya , M. Shiozawa , Y. Sonoda , A. Takeda , A. Takenaka , H. Tanaka , T. Yano , R. Akutsu , T. Kajita , Y. Nishimura , K. Okumura , R. Wang , J. Xia , L. Labarga , P. Fernandez , F. d. M. Blaszczyk , C. Kachulis , E. Kearns , J. L. Raaf , J. L. Stone , S. Berkman , J. Bian , N. J. Griskevich , W. R. Kropp , S. Locke , S. Mine , P. Weatherly , M. B. Smy , H. W. Sobel , V. Takhistov , K. S. Ganezer , J. Hill , J. Y. Kim , I. T. Lim , R. G. Park , B. Bodur , K. Scholberg , C. W. Walter , O. Drapier , M. Gonin , J. Imber , Th. A. Mueller , P. Paganini , T. Ishizuka , T. Nakamura , J. S. Jang , K. Choi , J. G. Learned , S. Matsuno , R. P. Litchfield , A. A. Sztuc , Y. Uchida , M. O. Wascko , N. F. Calabria , M. G. Catanesi , R. A. Intonti , E. Radicioni , G. De Rosa , A. Ali , G. Collazuol , F. Iacob , L. Ludovici , S. Cao , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , T. Nakadaira , K. Nakamura , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , KE. Abe , M. Hasegawa , Y. Isobe , H. Miyabe , T. Sugimoto , A. T. Suzuki , Y. Takeuchi , Y. Ashida , T. Hayashino , S. Hirota , M. Jiang , T. Kikawa , M. Mori , KE. Nakamura , T. Nakaya , R. A. Wendell , L. H. V. Anthony , N. McCauley , A. Pritchard , K. M. Tsui , Y. Fukuda , Y. Itow , M. Murrase , P. Mijakowski , K. Frankiewicz , C. K. Jung , X. Li , J. L. Palomino , G. Santucci , C. Vilela , M. J. Wilking , C. Yanagisawa , D. Fukuda , K. Hagiwara , H. Ishino , S. Ito , Y. Koshio , M. Sakuda , Y. Takahira , C. Xu , Y. Kuno , C. Simpson , D. Wark , F. Di Lodovico , B. Richards , S. Molina Sedgwick , R. Tacik , S. B. Kim , M. Thiesse , L. Thompson , H. Okazawa , Y. Choi , K. Nishijima , M. Koshiba , M. Yokoyama , A. Goldsack , K. Martens , M. Murdoch , B. Quilain , Y. Suzuki , M. R. Vagins , M. Kuze , Y. Okajima , T. Yoshida , M. Ishitsuka , J. F. Martin , C. M. Nantais , H. A. Tanaka , T. Towstego , M. Hartz , A. Konaka , P. de Perio , S. Chen , L. Wan , A. Minamino

We explore the consequences of promoting bilinear R-parity violation, usually formulated in the minimal supersymmetric standard model framework, to a supersymmetric SU(5) grand unified theory. We observe that the limits on proton decay and…

High Energy Physics - Phenomenology · Physics 2015-09-07 Najimuddin Khan , Subhendu Rakshit , Amitava Raychaudhuri

We calculate the proton decay rate due to five dimensional SU(5) gauge bosons in the Randall-Sundrum scenario with two branes (Planck brane and TeV brane). We consider matter in the usual 10 and \bar 5 SU(5) representations localized on a…

High Energy Physics - Phenomenology · Physics 2014-11-17 Shrihari Gopalakrishna

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 discuss baryon and lepton violation in the context of a simple 5-dimensional grand unified model, based on the orbifold S^1/(Z_2 x Z_2'). While gauge and Higgs degrees of freedom live in the bulk, matter is located on the boundaries of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ferruccio Feruglio

Supersymmetric standard model (MSSM) has two sources of rapid proton decay: (i) R-parity breaking terms and (ii) higher dimensional Planck induced B-violating terms; its extensions to include neutrino masses via the type I seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2009-10-02 Rabindra N. Mohapatra
‹ Prev 1 8 9 10 Next ›