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We study the hadronic $\eta^{\prime}\to\eta\pi\pi$ decays within the framework of $U(3)_{L}\otimes U(3)_{R}$ Chiral Perturbation Theory including resonance states and the complete one-loop corrections. The amplitude is projected in partial…

High Energy Physics - Phenomenology · Physics 2018-10-17 Sergi Gonzàlez-Solís , Emilie Passemar

A reliable calculation of radiative corrections to $\tau\to\pi\pi\nu_\tau$ decays is an important prerequisite for using hadronic $\tau$ decays for a data-driven evaluation of the hadronic-vacuum-polarization contribution to the anomalous…

High Energy Physics - Phenomenology · Physics 2026-03-12 Gilberto Colangelo , Martina Cottini , Martin Hoferichter , Simon Holz

We point out that the spectrum of pseudoscalar and scalar mesons exhibits a cuasi-degenerate chiral nonet in the energy region around 1.4 GeV whose scalar component has a slightly inverted spectrum. Based on the empirical linear rising of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mauro Napsuciale , Simon Rodriguez

We search for the process $B^0 \to \pi^- \tau^+ \nu_\tau$ using the full Belle data set of $711\,{\rm fb}^{-1}$, corresponding to $772 \times 10^6 B\bar{B}$ pairs, collected at the $\Upsilon(4S)$ resonance with the Belle detector at the…

High Energy Physics - Experiment · Physics 2016-03-02 Belle Collaboration , P. Hamer , A. Frey , A. Abdesselam , I. Adachi , H. Aihara , S. Al Said , K. Arinstein , D. M. Asner , T. Aushev , R. Ayad , V. Babu , I. Badhrees , A. M. Bakich , E. Barberio , B. Bhuyan , J. Biswal , A. Bozek , M. Bračko , T. E. Browder , D. Červenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , V. Chobanova , Y. Choi , D. Cinabro , J. Dalseno , M. Danilov , I. Danko , N. Dash , J. Dingfelder , Z. Doležal , Z. Drásal , A. Drutskoy , D. Dutta , S. Eidelman , H. Farhat , J. E. Fast , T. Ferber , B. G. Fulsom , V. Gaur , N. Gabyshev , A. Garmash , D. Getzkow , R. Gillard , R. Glattauer , Y. M. Goh , P. Goldenzweig , B. Golob , D. Greenwald , J. Haba , T. Hara , J. Hasenbusch , K. Hayasaka , H. Hayashii , W. -S. Hou , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , Y. Iwasaki , I. Jaegle , H. B. Jeon , D. Joffe , K. K. Joo , T. Julius , K. H. Kang , E. Kato , T. Kawasaki , C. Kiesling , D. Y. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , A. Kuzmin , Y. -J. Kwon , J. S. Lange , D. H. Lee , I. S. Lee , H. Li , L. Li , Y. Li , J. Libby , Y. Liu , D. Liventsev , P. Lukin , M. Masuda , D. Matvienko , K. Miyabayashi , H. Miyake , H. Miyata , R. Mizuk , G. B. Mohanty , S. Mohanty , A. Moll , H. K. Moon , R. Mussa , E. Nakano , M. Nakao , T. Nanut , Z. Natkaniec , M. Nayak , N. K. Nisar , S. Nishida , S. Ogawa , S. Okuno , C. Oswald , P. Pakhlov , G. Pakhlova , B. Pal , H. Park , T. K. Pedlar , L. Pesántez , R. Pestotnik , M. Petrič , L. E. Piilonen , C. Pulvermacher , J. Rauch , E. Ribežl , M. Ritter , A. Rostomyan , H. Sahoo , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. Shapkin , V. Shebalin , T. -A. Shibata , J. -G. Shiu , A. Sibidanov , F. Simon , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Starič , J. Stypula , T. Sumiyoshi , Y. Teramoto , K. Trabelsi , V. Trusov , M. Uchida , S. Uehara , Y. Unno , S. Uno , P. Urquijo , Y. Usov , C. Van Hulse , P. Vanhoefer , G. Varner , V. Vorobyev , A. Vossen , C. H. Wang , M. -Z. Wang , P. Wang , Y. Watanabe , E. Won , H. Yamamoto , J. Yamaoka , S. Yashchenko , Y. Yook , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

The $\tau$ lepton decays $\tau \to [K^- K^0 \pi^0, K^- K^+ \pi^-, K ^0 \bar{K^0} \pi^-] \nu_{\tau}$ are described in the $U(3) \times U(3)$ NJL quark model. The contact channel and intermediate channels with axial-vector, vector and…

High Energy Physics - Phenomenology · Physics 2023-10-12 M. K. Volkov , A. A. Pivovarov , K. Nurlan

We introduce a novel parameterization of $B\rightarrow\pi\pi\ell\nu$ form factors relying on partial-wave decompositions and series expansions in suitable variables. We bound the expansion coefficients through unitarity and include…

High Energy Physics - Phenomenology · Physics 2025-08-25 Florian Herren , Bastian Kubis , Raynette van Tonder

It is shown that a chiral quark model of the Nambu--Jona-Lasinio type can be used to describe "soft"-momenta parts of the amplitudes with large momentum transfer. As a sample, the processes \gamma^* --> \gamma (\pi,\eta,\eta') where one of…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. E. Dorokhov , M. K. Volkov , V. L. Yudichev

We present a study for the measurement of of radiative decays, tau -> l gamma nu nu, l=e, mu, and tau -> pi gamma nu using 500 fb-1 of electron-positron annihilations recorded by the BaBar detector at the PEP-II asymmetric B-factory.

High Energy Physics - Experiment · Physics 2022-03-02 Benjamin Oberhof

The decays $\tau^-\to K^-\eta\nu_\tau$ and $K^-\eta^\prime\nu_\tau$ are studied in the context of Chiral Perturbation Theory supplemented with the explicit inclusion of resonances. For the required vector-form factors we have explored three…

High Energy Physics - Phenomenology · Physics 2014-03-31 Rafel Escribano

Using the close relationship between the low--energy constants of chiral perturbation theory and the chiral invariant interactions of the vector meson resonances with the pseudoscalar mesons, we investigate the process $\rho^0 \ra \pi^+…

High Energy Physics - Phenomenology · Physics 2009-10-28 K. Huber , H. Neufeld

In the framework of the extended Nambu-Jona-Lasinio model, the processes $\tau \to \pi \pi \eta(\eta')\nu_\tau$ and $\tau \to \pi\eta\eta(\eta')\nu_\tau$ are considered taking into account mesons in the ground and first radially excited…

High Energy Physics - Phenomenology · Physics 2025-04-10 M. K. Volkov , A. A. Pivovarov , K. Nurlan

The partial widths of the decays $D^+_s \to \phi \pi^+$ and $D^+_s \to \pi^+ \pi^+ \pi^-$ - nonresonant are computed within the effective quark model with chiral symmetry involving Heavy quark effective theory (HQET) and Chiral perturbation…

High Energy Physics - Phenomenology · Physics 2022-03-02 A. N. Ivanov , N. I. Troitskaya

We present the first study of the vector (Wess-Zumino) current in tau^-\to K^-pi^-K^+\nu_\tau decay using data collected with the CLEO III detector at the Cornell Electron Storage Ring. We determine the quantitative contributions to the…

High Energy Physics - Experiment · Physics 2010-04-08 T. E. Coan , CLEO Collaboration

Using chiral low energy theorems and elastic unitarity assumption, the $\tau\to\pi K \nu $ decay is investigated. The vector and scalar $\pi K$ form factors are calculated. It is found that the $\pi K$ spectrum is dominated by the $K^*$…

High Energy Physics - Phenomenology · Physics 2009-10-28 L. Beldjoudi , Tran N. Truong

The contribution of the rho^{\pm} vector meson to the tau -> pi pi nu gamma decay is considered as a potential source for the determination of the magnetic dipole moment of this light vector meson. In order to keep gauge-invariance of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. Lopez Castro , G. Toledo Sanchez

The resonant structure of the four pion final state in the decay $\tau \to 3\pi\pi^0\nu_\tau$ is analyzed using 4.27 million $\tau^+\tau^-$ pairs collected by the CLEO II experiment. We search for second class currents in the decay $\tau…

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

We present a search for the decay $B^{-} \to \tau^{-} \bar{\nu}_{\tau}$ in a sample of $88.9 \times 10^{6}$ $B\bar{B}$ pairs recorded with the BaBar detector at the SLAC $B$-Factory. One of the two $B$ mesons from the $\Upsilon(4S)$ is…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert , BABAR Collaboration

The amplitudes of $\pi$-meson decays are calculated in a relativistic nonperturbative quark model which assumes that mesons are made of a quark antiquark pair and of a scalar neutral component representing the contribution of the…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. Ghilencea , L. Micu

To date, the weak-phase $\gamma$ has been measured using two-body $B$-meson decays such as $B\to D K$ and $B\to D\pi$, whose amplitudes contain only tree-level diagrams. But $\gamma$ can also be extracted from three-body charmless hadronic…

High Energy Physics - Phenomenology · Physics 2018-11-28 Bhubanjyoti Bhattacharya , David London

We have studied the $P\to\gamma^\star\gamma^\star$ form factor in Resonance Chiral Theory, with $P = \pi^0,\eta,\eta'$, to compute the contribution of the pseudoscalar pole to the hadronic light-by-light piece of the anomalous magnetic…

High Energy Physics - Phenomenology · Physics 2018-12-05 Adolfo Guevara , Pablo Roig , JJ Sanz Cillero