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Related papers: Testing QCD with Hypothetical Tau Leptons

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Since the numerical path integration in the lattice QCD involves quark and gluon fields (not hadron fields) the lattice QCD cannot calculate any hadronic observable. Because of this reason the hadronic properties are extracted in the…

High Energy Physics - Lattice · Physics 2018-07-18 Gouranga C Nayak

The future FCC-ee collider is designed to deliver $\mathrm{e^+e^-}$ collisions to study with ultimate precision the Z, W, and Higgs bosons, and the top quark. In a high-statistics scan around the Z pole, $1.3\times 10^{11}$ events…

High Energy Physics - Experiment · Physics 2018-12-18 Mogens Dam

We search for lepton-flavor-violating and lepton-number-violating tau decays into a lepton (l = electron or muon) and two charged mesons (h, h' = pion or Kaon) using 854 fb^{-1} of data collected with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2015-06-05 Y. Miyazaki , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , A. M. Bakich , A. Bay , V. Bhardwaj , B. Bhuyan , M. Bischofberger , A. Bozek , M. Bračko , T. E. Browder , M. -C. Chang , A. Chen , P. Chen , B. G. Cheon , R. Chistov , K. Cho , Y. Choi , J. Dalseno , Z. Doležal , A. Drutskoy , S. Eidelman , D. Epifanov , J. E. Fast , V. Gaur , N. Gabyshev , A. Garmash , Y. M. Goh , J. Haba , H. Hayashii , Y. Horii , Y. Hoshi , W. -S. Hou , H. J. Hyun , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , M. Iwabuchi , Y. Iwasaki , T. Julius , J. H. Kang , C. Kiesling , H. J. Kim , H. O. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , B. R. Ko , S. Koblitz , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , A. Kuzmin , Y. -J. Kwon , S. -H. Lee , Y. Li , C. -L. Lim , C. Liu , Z. Q. Liu , D. Liventsev , R. Louvot , D. Matvienko , S. McOnie , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , N. Muramatsu , E. Nakano , M. Nakao , S. Nishida , K. Nishimura , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , Y. Onuki , P. Pakhlov , G. Pakhlova , C. W. Park , H. K. Park , M. Petrič , L. E. Piilonen , M. Röhrken , S. Ryu , H. Sahoo , Y. Sakai , T. Sanuki , Y. Sato , O. Schneider , C. Schwanda , K. Senyo , O. Seon , M. Shapkin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , J. B. Singh , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , S. Stanič , M. Starič , T. Sumiyoshi , G. Tatishvili , Y. Teramoto , K. Trabelsi , T. Tsuboyama , M. Uchida , S. Uehara , Y. Unno , S. Uno , P. Urquijo , G. Varner , C. H. Wang , P. Wang , E. Won , Y. Yamashita , Y. Yusa , Z. P. Zhang , V. Zhulanov

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

The thorough analysis of the ALEPH data on hadronic tau-decay is performed in the framework of QCD. The perturbative calculations are performed in 3 and 4-loop approximations. The terms of the operator product expansion (OPE) are accounted…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. V. Geshkenbein , B. L. Ioffe , K. N. Zyablyuk

We review the determinations of the QCD coupling $\alpha_s$ from the inclusive and exclusive modes of $\tau$-decays. The most recent $\tau$-data provide the average value $ \alpha_ s \left(M^2_\tau \right)\simeq 0.347\pm 0.030 $…

High Energy Physics - Phenomenology · Physics 2012-08-27 S. Narison , :

The inclusive tau lepton hadronic decay and its description within Dispersive approach to Quantum Chromodynamics are briefly discussed.

High Energy Physics - Phenomenology · Physics 2016-04-26 A. V. Nesterenko

The tau is the only known lepton that can decay hadronically. From this class of decays, high precision measurements of several quantities can be extracted: the CKM matrix element $V_{us}$, the mass of the strange quark, etc. Also, as a…

High Energy Physics - Phenomenology · Physics 2012-08-15 A. Moyotl

Using recently developed methods for the evaluation of five-loop amplitudes in perturbative QCD, corrections of order alpha_s^4 for the cross section of electron-positron annihilation into hadrons and for the decay rates of the Z-boson and…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. A. Baikov , K. G. Chetyrkin , J. H. Kühn

A novel method for the direct measurement of the elusive magnetic and electric dipole moments of the tau lepton is presented. The experimental approach relies on the production of tau+ leptons from Ds+ -> tau+ nu_tau decays, originated in…

High Energy Physics - Experiment · Physics 2019-07-10 J. Fu , M. A. Giorgi , L. Henry , D. Marangotto , F. Martinez Vidal , A. Merli , N. Neri , J. Ruiz Vidal

We apply perturbative QCD factorization theorems to inclusive heavy hadron decays, and obtain simultaneously a low semileptonic branching ratio $B(B\to Xl\bar{\nu})=10.16%$, the average charm yield $<n_c>=1.17$ per $B$ decay, a small…

High Energy Physics - Phenomenology · Physics 2009-10-31 We-Fu Chang , Hsiang-nan Li , Hoi-Lai Yu

In a small window of phase space, chiral perturbation theory can be used to make standard model predictions for tau decays into two and three pions. For $\tau \to 2\pi \nu_\tau$, we give the analytical result for the relevant form factor…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Colangelo , M. Finkemeier , R. Urech

The angular analysis of exclusive rare B-meson decays via intermediate vector mesons V into 4-body final states of two pseudo-scalars P_1, P_2 and a pair of light leptons l = e, mu offers a large set of observables. They can be used to test…

High Energy Physics - Phenomenology · Physics 2015-05-28 Christoph Bobeth , Gudrun Hiller , Danny van Dyk

A numerical analysis of QED radiative corrections for elastic e(mu)p cattering in hadronic variables at energies of the current experiment at JLab is performed. The explicit formulas from the review of Akhundov et al. resulting from the…

High Energy Physics - Phenomenology · Physics 2009-09-29 A. A. Akhundov , H. H. Alharbi , H. A. Alhendi

We determine the equation of state of QCD at finite chemical potential, to order $(\mu_B/T)^6$, for a system of 2+1 quark flavors. The simulations are performed at the physical mass for the light and strange quarks on several lattice…

High Energy Physics - Lattice · Physics 2018-03-14 J. Gunther , R. Bellwied , S. Borsanyi , Z. Fodor , S. D. Katz , A. Pasztor , C. Ratti

We present a search for the lepton flavor violating decay modes B+/- to h+/- tau l (h= K,pi; l= e,mu) using the BaBar data sample, which corresponds to 472 million BBbar pairs. The search uses events where one B meson is fully reconstructed…

High Energy Physics - Experiment · Physics 2012-08-27 The BABAR Collaboration

In the Standard Model, scalar contributions to leptonic and semileptonic decays are helicity suppressed. The hypothesis of additional physical neutral/charged Higgses can enhance such scalar contributions and give detectable effects…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jernej F. Kamenik , Federico Mescia

Evidence of a new particle with mass ~125 GeV decaying into a pair of tau leptons at the Large Hadron Collider spurs interest in ascertaining its spin in this channel. Here we present a comparative study between spin-0 and spin-2 nature of…

High Energy Physics - Phenomenology · Physics 2015-06-12 Swagato Banerjee , Jan Kalinowski , Wojciech Kotlarski , Tomasz Przedzinski , Zbigniew Was

Hadronization in tau -> K K pi nu_tau decays is driven by both vector and axial-vector currents that we study, guided by the following principles: The 1/N_C expansion -worked out at leading order, considering only the contribution of the…

High Energy Physics - Phenomenology · Physics 2016-01-21 Pablo Roig

Selected results from tau analyses performed using the BaBar detector at the SLAC National Accelerator Laboratory are presented. A precise measurement of the tau mass and the tau{+} tau{-} mass difference is undertaken using the hadronic…

High Energy Physics - Experiment · Physics 2019-08-13 S. Paramesvaran
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