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Related papers: One meson radiative tau decays

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In this paper we document the modifications introduced to the previous version of the Resonance Chiral Lagrangian current ({\it Phys.Rev.} {\bf D86} (2012) 113008) of the $\tau^\pm \to \pi^\pm \pi^\pm \pi^\mp \nu_\tau$ decay which enable…

High Energy Physics - Phenomenology · Physics 2013-12-02 I. M. Nugent , T. Przedzinski , P. Roig , O. Shekhovtsova , Z. Was

The \tau -> (\omega, \phi)P^-\nu decays, where P^-=\pi^-, K^-, are considered within a phenomenological model with dominance of meson intermediate states. We assume SU(3) flavor symmetry to fix some of the unknown strong interaction…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Flores-Tlalpa , G. Lopez Castro

It is now a firmly established fact that all family lepton numbers are violated in Nature. In this paper we discuss the implications of this observation for future searches for rare tau decays in the supersymmetric see-saw model. Using the…

High Energy Physics - Phenomenology · Physics 2011-03-23 Alejandro Ibarra , Cristoforo Simonetto

We investigate the transition formfactors for the B -> K^* l^+ l^- (l = mu, tau) decay in the light cone QCD. It is found that the light cone and 3-point QCD sum rules analyses for some of the formfactors for the decay B -> K^* l^+ l^- lead…

High Energy Physics - Phenomenology · Physics 2009-10-30 T. M. Aliev , A. Ozpineci , M. Savci

The tau decays to four hadrons have been studied with the CLEO III detector at the Cornell Electron Storage Ring (CESR) using (7.56 +- 0.15) fb^{-1} of data collected near the Y(4S) resonance. We present the first statistically significant…

High Energy Physics - Experiment · Physics 2010-04-08 K. Arms , CLEO Collaboration

We present the first measurements of branching fractions of rare tau-lepton decays, $\tau^- \rightarrow \pi^- \nu_{\tau} \ell^+ \ell^-$ ($\ell = e$ or $\mu$), using a data sample corresponding to 562 fb$^{-1}$ collected at a center-of-mass…

High Energy Physics - Experiment · Physics 2019-10-23 Belle Collaboration , Y. Jin , H. Aihara , D. Epifanov , I. Adachi , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , I. Badhrees , S. Bahinipati , V. Bansal , P. Behera , M. Berger , V. Bhardwaj , T. Bilka , J. Biswal , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , M. Campajola , L. Cao , D. Červenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Di Carlo , Z. Doležal , T. V. Dong , D. Dossett , S. Eidelman , J. E. Fast , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Giri , P. Goldenzweig , B. Golob , D. Greenwald , O. Grzymkowska , J. Haba , K. Hayasaka , H. Hayashii , M. T. Hedges , W. -S. Hou , K. Huang , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , H. B. Jeon , S. Jia , D. Joffe , K. K. Joo , J. Kahn , A. B. Kaliyar , G. Karyan , T. Kawasaki , H. Kichimi , C. Kiesling , D. Y. Kim , H. J. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , R. Kulasiri , R. Kumar , A. Kuzmin , Y. -J. Kwon , K. Lalwani , J. S. Lange , J. Y. Lee , S. C. Lee , C. H. Li , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , Z. Liptak , D. Liventsev , P. -C. Lu , T. Luo , J. MacNaughton , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , H. Miyata , R. Mizuk , T. Mori , R. Mussa , E. Nakano , M. Nakao , K. J. Nath , Z. Natkaniec , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , Y. Onuki , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , V. Popov , E. Prencipe , A. Rostomyan , G. Russo , D. Sahoo , Y. Sakai , M. Salehi , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , O. Seon , M. E. Sevior , V. Shebalin , C. P. Shen , J. -G. Shiu , B. Shwartz , F. Simon , J. B. Singh , A. Sokolov , E. Solovieva , S. Stanič , M. Starič , Z. S. Stottler , J. F. Strube , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , R. Van Tonder , G. Varner , A. Vinokurova , V. Vorobyev , A. Vossen , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , S. Watanuki , E. Won , S. B. Yang , H. Ye , J. H. Yin , C. Z. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

We perform a measurement of the branching fractions for tau -> l gamma nu anti-nu (l= e, mu) decays for a minimum photon energy of 10 MeV in the tau rest frame using 430 fb^-1 of e^+ e^- collisions collected at the center-of-mass energy of…

High Energy Physics - Experiment · Physics 2015-02-09 Benjamin Oberhof

Combining heavy quark effective theory and the chiral Lagrangian approach we investigate radiative decays of pseudoscalar $D$ mesons. We first reanalyse $D^{*} \rightarrow D \gamma$ decays within the effective Lagrangian approach using…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Bajc , S. Fajfer , R. J. Oakes

In this article we analyze the contribution from intermediate spin-0 and spin-2 resonances to the $\tau\to\nu \pi\pi\pi$ decay by means of a chiral invariant Lagrangian incorporating these mesons. In particular, we study the corresponding…

High Energy Physics - Phenomenology · Physics 2018-01-17 Juan Jose Sanz-Cillero , Olga Shekhovtsova

We analyze the dominant decay mechanisms in the radiative decays D -> V gamma, D -> P(V) l+ l-, D -> gamma gamma, D -> l+ l- gamma, and we discuss possible chances to observe the effects of new physics in these decays. Then we comment on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Svjetlana Fajfer

We present a concise review of the recent theoretical progress concerning the standard model calculations of the rare K_L -> pi^0 nu anti-nu, K^+ -> pi^+ nu anti-nu (gamma), anti-B -> X_s gamma, and anti-B -> X_s l^+ l^- decays. The current…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ulrich Haisch

The tau -> pi pi pi nu_tau decay is driven by the hadronization of the axial-vector current. Within the resonance chiral theory, and considering the large-Nc expansion, this process has been studied in Ref.[1]. In the light of later…

High Energy Physics - Phenomenology · Physics 2011-08-25 D. Gomez Dumm , P. Roig , A. Pich , J. Portoles

In a combined study of the decay spectra of $\tau^-\to K_S\pi^-\nu_\tau$ and $\tau^-\to K^-\eta\nu_\tau$ decays within a dispersive representation of the required form factors, we illustrate how the $K^*(1410)$ resonance parameters, defined…

High Energy Physics - Phenomenology · Physics 2014-09-11 R. Escribano , S. González-Solís , M. Jamin , P. Roig

Hadronic tau decays represent a clean laboratory for the precise study of quantum chromodynamics (QCD). Observables (sum rules) based on the spectral functions of hadronic tau decays can be related to QCD quark-level calculations to…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Davier , A. Hocker , Z. Zhang

We present a calculation of the rare decay mode D^0 -> gamma gamma, in which the long distance contributions are expected to be dominant. Using the Heavy Quark Chiral Perturbation Theory Lagrangian with a strong g coupling as recently…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. Fajfer , P. Singer , J. Zupan

The radiative decay of the axial-vector resonances into a pseudoscalar meson and a photon is studied using the vector meson Lagrangian obtained from the hidden gauge symmetry (HGS) formalism. The formalism is well suited to study this…

High Energy Physics - Phenomenology · Physics 2009-02-26 H. Nagahiro , L. Roca , A. Hosaka , E. Oset

We review the recent measurements of the rare pion decays: Pi+ -> Pi0 e+ Nu [pion beta, Pi_(e3), or Pi_beta decay], radiative decay Pi+ -> e+ Nu Gamma [Pi_(e2Gamma) or RPD], and Pi+ -> e+ Nu [Pi_(e2)] decay, as well as the radiative muon…

High Energy Physics - Experiment · Physics 2010-04-26 D. Pocanic

We perform a thorough analysis of the VP\gamma(\gamma*) and P\gamma\gamma(\gamma*) decays in the resonance chiral theory, where V stand for the vector resonances \rho, K*, \omega, \phi, P stand for \pi, K, \eta, \eta' and \gamma*…

High Energy Physics - Phenomenology · Physics 2013-05-30 Yun-Hua Chen , Zhi-Hui Guo , Han-Qing Zheng

The branching ratio of the tau lepton to a neutral K meson is measured from a sample of approximately 200,000 tau decays recorded by the OPAL detector at centre-of-mass energies near the Z0 resonance. The measurement is based on two samples…

High Energy Physics - Experiment · Physics 2008-11-26 G. Abbiendi , the OPAL collaboration

We present the first observation of tau lepton decays to hadronic final states with a phi-meson. This analysis is based on 401 fb^-1 of data accumulated at the Belle experiment. The branching fraction obtained is B(tau- -> phi K- nu) =…

High Energy Physics - Experiment · Physics 2008-11-26 Belle colaboration