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Related papers: omega -> pi pi decay in nuclear medium

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We present the ingredients necessary for the determination of physical K->pi pi decay amplitudes for Delta I=3/2 transitions, from lattice simulations at unphysical kinematics and the use of chiral perturbation theory at next-to-leading…

High Energy Physics - Lattice · Physics 2008-11-26 C. -J. D. Lin , G. Martinelli , E. Pallante , C. T. Sachrajda , G. Villadoro

We discuss the possibility to study the in-medium changes of the properties of the omega meson in reactions on ordinary nuclei with elementary electromagnetic probes. We present a tree-level calculation of the elementary gamma p -> omega p…

Nuclear Theory · Physics 2008-11-26 P. Muehlich , U. Mosel

Neutrinoless double beta decay (\( 0 \nu \beta \beta \)) is a hypothetical nuclear decay mode with important implications. In particular, observation of this decay would demonstrate that the neutrino is a Majorana particle and that lepton…

High Energy Physics - Lattice · Physics 2020-04-17 W. Detmold , D. J. Murphy

Using heavy-baryon chiral perturbation theory, we have calculated all the diagrams up to two-loop order which contribute to the S-wave pion self-energy in symmetric nuclear matter. Some subtleties related to the definition of pion fields…

Nuclear Theory · Physics 2008-11-26 Tae-Sun Park , Hong Jung , Dong-Pil Min

Measurements of the rates for the hadronic decays B^+- -> pi K along with the CP-averaged B^+- -> pi^+- pi^0 branching ratio can be used to bound and extract the weak phase gamma=-arg(V_ub). Using preliminary CLEO data, we obtain the bounds…

High Energy Physics - Phenomenology · Physics 2007-05-23 Matthias Neubert

The $\omega$- and $\rho$-resonance production and their dileptonic decay in $\pi^- A$ reactions at GSI energies are calculated within the intranuclear cascade (INC) approach. The invariant mass distribution of the dilepton pair for each…

Nuclear Theory · Physics 2009-10-30 W. Cassing , Ye. S. Golubeva , A. S. Iljinov , L. A. Kondratyuk

A review of the modern theory of hadronic atoms based on the non-relativistic effective Lagrangian approach and ChPT, is given. As an application of the general framework, we consider the decay of the pi+pi- atom into two neutral pions, and…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. Rusetsky

The claim that the light quark mass ratio (m_d - m_u)/m_s can be extracted from the decay width ratio Gamma(eta' -> pi^0 pi^+ pi^-)/Gamma(eta' -> eta pi^+ pi^-) is critically investigated within a U(3) chiral unitary framework. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. Borasoy , Ulf-G. Meißner , R. Nißler

We present the results of searches for nucleon decays via $p\rightarrow\nu\pi^{+}$ and $n\rightarrow\nu\pi^{0}$ using a 0.484 Mt$\cdot$yr exposure of Super-Kamiokande I-V data covering the entire pure water phase of the experiment. Various…

High Energy Physics - Experiment · Physics 2026-02-03 Kamiokande Collaboration , S. Jung , K. Abe , S. Abe , Y. Asaoka , M. Harada , Y. Hayato , K. Hiraide , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Sato , H. Sekiya , R. Shinoda , M. Shiozawa , Y. Suzuki , A. Takeda , Y. Takemoto , H. Tanaka , T. Yano , T. H. Hung , Y. Itow , T. Kajita , R. Nishijima , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , P. Fernandez , L. Labarga , D. Samudio , B. Zaldivar , C. Yanagisawa , E. Kearns , L. Wan , T. Wester , B. W. Pointon , J. Bian , B. Cortez , N. J. Griskevich , Y. Jiang , M. B. Smy , H. W. Sobel , V. Takhistov , A. Yankelevich , J. Hill , M. C. Jang , S. H. Lee , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , O. Drapier , A. Ershova , Th. A. Mueller , A. D. Santos , P. Paganini , C. Quach , R. Rogly , M. Ferey , T. Nakamura , J. S. Jang , R. P. Litchfield , L. N. Machado , F. J. P. Soler , J. G. Learned , K. Choi , S. Cao , L. H. V. Anthony , N. W. Prouse , M. Scott , Y. Uchida , V. Berardi , N. F. Calabria , M. G. Catanesi , N. Ospina , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , S. Horiuchi , A. Kawabata , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , R. Akutsu , M. Friend , T. Hasegawa , Y. Hino , T. Ishida , T. Kobayashi , M. Jakkapu , T. Matsubara , T. Nakadaira , Y. Oyama , A. Portocarrero Yrey , K. Sakashita , T. Sekiguchi , T. Tsukamoto , N. Bhuiyan , G. T. Burton , F. Di Lodovico , J. Gao , T. Katori , R. M. Ramsden , N. Latham , R. Kralik , H. Ito , T. Sone , A. T. Suzuki , Y. Takeuchi , S. Wada , H. Zhong , J. Feng , L. Feng , S. Han , J. Hikida , J. R. Hu , Z. Hu , M. Kawaue , T. Kikawa , T. Nakaya , T. V. Ngoc , R. A. Wendell , S. J. Jenkins , N. McCauley , A. Tarrant , M. Faní , M. J. Wilking , Z. Xie , Y. Fukuda , H. Menjo , Y. Yoshioka , J. Lagoda , M. Mandal , J. Zalipska , M. Mori , J. Jiang , K. Hamaguchi , H. Ishino , Y. Koshio , F. Nakanishi , T. Tada , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , T. Peacock , P. Stowell , M. D. Thiesse , L. F. Thompson , H. Okazawa , S. M. Lakshmi , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , A. K. Ichikawa , K. D. Nakamura , S. Goto , S. Kodama , Y. Mizuno , T. Muro , K. Nakagiri , Y. Nakajima , N. Taniuchi , M. Yokoyama , H. Hayasaki , Y. Masaki , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , M. Kuze , S. Izumiyama , R. Matsumoto , R. Asaka , M. Ishitsuka , M. Sugo , M. Wako , K. Yamauchi , Y. Nakano , F. Cormier , R. Gaur , M. Hartz , A. Konaka , X. Li , B. R. Smithers , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , M. Girgus , P. Govindaraj , M. Posiadala-Zezula , Y. S. Prabhu , H. Adhikary , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , C. Bronner , D. Horiguchi , A. Minamino , Y. Sasaki , R. Shibayama , R. Shimamura

We evaluate two-body decay modes of charginos in the Minimal Supersymmetric Standard Model with complex parameters (cMSSM). Assuming heavy scalar quarks we take into account all decay channels involving charginos, neutralinos, (scalar)…

High Energy Physics - Phenomenology · Physics 2012-10-20 S. Heinemeyer , F. von der Pahlen , C. Schappacher

We investigate the rare radiative eta decay modes $\eta\to\pi^+\pi^-\gamma\gamma$ and $\eta\to\pi^0\pi^0\gamma\gamma$ within the framework of chiral perturbation theory at $O(p^4)$. We present photon spectra and partial decay rates for both…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Kn"ochlein , S. Scherer , D. Drechsel

In the framework of the Standard Model (SM) a theoretical description of the neutron beta decay is given at the level of 10^{-5}. The neutron lifetime and correlation coefficients of the neutron beta decay for a polarized neutron, a…

High Energy Physics - Phenomenology · Physics 2021-09-08 A. N. Ivanov , R. Höllwieser , N. I. Troitskaya , M. Wellenzohn , Ya. A. Berdnkov

The temperature dependence of the $\phi$ meson mass and its decay width ($\phi \rightarrow K \bar{K}$)have been studied from an effective non-linear chiral Lagrangian in $SU(3)$. Effective mass has been obtained from the pole position of…

Nuclear Theory · Physics 2008-11-26 Abhijit Bhattacharyya , Sanjay K. Ghosh , S. C. Phatak , Sibaji Raha

The semileptonic decay B->pi is studied starting from a simple quark model that takes into account the effect of the B* resonance. A novel, multiply subtracted, Omnes dispersion relation has been implemented to extend the predictions of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Albertus , J. M. Flynn , E. Hernandez , J. Nieves , J. M. Verde-Velasco

Using the light-front pion wave function based on a Bethe-Salpeter amplitude model, we study the properties of the pion in symmetric nuclear matter. The pion model we adopt is well constrained by previous studies to explain the pion…

High Energy Physics - Phenomenology · Physics 2014-09-10 J. P. B. C. de Melo , K. Tsushima , Bruno El-Bennich , E. Rojas , T. Frederico

We decompose the neutrinoless double-beta decay matrix elements into sums of products over the intermediate nucleus with two less nucleons. We find that the sum is dominated by the J^pi=0^+ ground state of this intermediate nucleus for both…

Nuclear Theory · Physics 2015-06-23 B. A. Brown , M. Horoi , R. A. Sen'kov

The decay of the Standard Model Higgs boson into four leptons via a virtual W-boson or Z-boson pair is one of the most important decay modes in the Higgs-boson search at the LHC. We present the complete electroweak radiative corrections of…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Bredenstein , A. Denner , S. Dittmaier , M. M. Weber

Using the chiral model of pseudoscalar, vector, and axial vector mesons based on the hidden local symmetry added with the terms induced by the Wess-Zumino anomaly, the results of calculations of the branching fractions of the decays…

High Energy Physics - Phenomenology · Physics 2009-11-11 N. N. Achasov , A. A. Kozhevnikov

Using e+e- annihilation data collected by the CLEO~II detector at CESR, we have observed the decay Ds+ to omega pi+. This final state may be produced through the annihilation decay of the Ds+, or through final state interactions. We find a…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , R. Balest et al

The usage of nuclear emulsion with molybdenum filling for observation of $\beta\beta$ decay are shown to be possible. Estimates for 1 kg of $^{100}$Mo with zero background give the sensitivity for the $0\nu\beta\beta$ decay of $^{100}$Mo at…

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