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Related papers: Improved Upper Limits on Baryon-Number Violating D…

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Searches for lepton number violating $K^+\to\pi^-e^+e^+$ and $K^+\to\pi^-\pi^0e^+e^+$ decays have been performed using the complete dataset collected by the NA62 experiment at CERN in 2016-2018. Upper limits of $5.3\times 10^{-11}$ and…

High Energy Physics - Experiment · Physics 2022-05-18 NA62 collaboration

The decays $\Xi_b \to \Lambda_b \pi$ are strangeness changing weak transitions involving only the light diquark in the baryon. Thus these decays can test the properties of such diquarks, in particular the suggestions existing in the…

High Energy Physics - Phenomenology · Physics 2014-09-05 Xin Li , M. B. Voloshin

We report on measurements of the decays of $\overline{B}$ mesons into the semileptonic final states $\overline{B} \to D^{(*)} \pi^+\pi^- \ell^-\overline{\nu}$, where $D^{(*)}$ represents a $D$ or $D^*$ meson and $\ell^-$ is an electron or a…

High Energy Physics - Experiment · Physics 2016-02-03 The BABAR Collaboration

The $d^* \to d \pi \pi$ partial decay width has been calculated in a wave-function model for $d^*$ and $d$. It is found to be smaller than a previous estimate by a factor of 7. A previously proposed dependence on dibaryon sizes is…

Nuclear Theory · Physics 2014-11-18 Chun Wa Wong

A search for the $K^{+} \to \pi^{0}\pi^{0}\pi^{0}e^+\nu$ decay is performed by the OKA collaboration. The search is based on $3.65 \times 10^9 ~ K^+$ decays. No signal is observed. The upper limit set is $BR(K^{+} \to…

A search for new particles (X) that decay to electron or muon pairs has been performed using approximately 200 pb**(-1) of pbarp collision data at sqrt(s)=1.96 TeV collected by the CDF II experiment at the Fermilab Tevatron. Limits on…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , A. Abulencia

The NA48/2 experiment at CERN collected a large sample of charged kaon decays into final states with multiple charged particles in 2003--2004. A new upper limit on the rate of the lepton number violating decay…

High Energy Physics - Experiment · Physics 2016-11-23 Karim Massri

We analyze rare kaon decays in models in which the dominant new effect is an enhanced $\bar s d Z$ vertex $Z_{ds}$. We point out that in spite of large theoretical uncertainties the CP-violating ratio $\epsilon^\prime/\epsilon$ provides at…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andrzej J. Buras , Luca Silvestrini

A search for nu_bar_mu to nu_bar_e oscillations has been conducted at the Los Alamos Meson Physics Facility using nu_bar_mu from mu+ decay at rest. The nu_bar_e are detected via the reaction (nu_bar_e,p) -> (e+,n), correlated with the 2.2…

We have searched for tau lepton decays, tau- -> Lambda-bar pi- and tau- -> Lambda pi-, that simultaneously violate the conservation of the lepton and baryon number using a data sample of 154 fb^{-1} collected with the Belle detector at the…

High Energy Physics - Experiment · Physics 2019-08-14 Y. Miyazaki

We use recent data that show a narrow peak around $\sqrt{s}=2.37\ \text{GeV}$ in the $pn \to d \pi^+ \pi^-$ cross section, with about double strength at the peak than in the analogous $pn \to d \pi^0 \pi^0$ reaction, and, assuming that it…

Nuclear Theory · Physics 2013-08-09 Miguel Albaladejo , Eulogio Oset

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

The most general supersymmetric model contains baryon number violating terms of the form $\lambda_{ijk}\;\ov{D}_i\, \ov{D}_j\, \ov{U}_k$ in the superpotential. We reconsider the bounds on these couplings, assuming that lepton number…

High Energy Physics - Phenomenology · Physics 2014-11-17 J. L. Goity , Marc Sher

The $\pi N$ system in decays of $J/\psi\to\bar NN\pi$ is limited to be isospin 1/2 by isospin conservation. This provides a big advantage in studying $N^*\to \pi N$ compared with $\pi N$ and $\gamma N$ experiments which mix isospin 1/2 and…

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

In this report we discuss the main theories to understand the origin of baryon and lepton number violation in physics beyond the Standard Model. We present the theoretical predictions for rare processes such as neutrinoless double beta…

The NA48/2 experiment at CERN collected a large sample of charged kaon decays into final states with multiple charged particles in 2003--2004. A new upper limit on the rate of the lepton number violating decay $K^{\pm} \to \pi^{\mp}…

High Energy Physics - Experiment · Physics 2016-07-15 Karim Massri

We use information from rare nonleptonic decays of heavy-quark mesons to put new bounds on the magnitudes of certain product combinations of baryon nonconserving R-parity violating couplings in supersymmetric models. Product combinations of…

High Energy Physics - Phenomenology · Physics 2009-10-28 Carl Carlson , Probir Roy , Marc Sher

We show that discovery of baryon number violation in two processes with at least one obeying the selection rule \Delta (B-L) = \pm 2 can determine the Majorana character of neutrinos. Thus observing p \to e^+ \pi^0 and n \to e^- \pi^0…

High Energy Physics - Phenomenology · Physics 2015-06-22 K. S. Babu , Rabindra N. Mohapatra

We have searched a sample of 9.6 million BBbar events for the flavor-changing neutral current decays B -> K l^+ l^- and B -> K^*(892) l^+ l^-. We subject the latter decay to the requirement that the dilepton mass exceed 0.5 GeV. There is no…

High Energy Physics - Experiment · Physics 2010-05-28 S. Anderson , CLEO Collaboration

Baryon number violating (BNV) processes are heavily constrained by experiments searching for nucleon decay and neutron-antineutron oscillations. If the baryon number violation occurs via the third generation quarks, however, we may be able…

High Energy Physics - Phenomenology · Physics 2012-05-10 Iason Baldes , Nicole F. Bell , Raymond R. Volkas