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Related papers: Pion to photon transition form factors with basis …

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We discuss what can be learned about the shape of the pion distribution amplitude from the form factor for gamma* gamma(*) to pi transitions.

High Energy Physics - Phenomenology · Physics 2007-05-23 Carsten Vogt

The pion decay constants of the lowest orbitally excited states of the nucleon and the $\Delta(1232)$ along with the corresponding axial transition form factors are calculated with Poincar\'e covariant constituent-quark models with instant,…

Nuclear Theory · Physics 2009-11-10 B. Julia-Diaz , D. O. Riska , F. Coester

We compute the pion electromagnetic form factor in a hybrid calculation with domain wall valence quarks and improved staggered (asqtad) sea quarks. This method can easily be extended to rho-to-gamma-pi transition form factors.

High Energy Physics - Lattice · Physics 2014-11-17 LHP Collaboration , George T. Fleming , Frederic D. R. Bonnet , Robert G. Edwards , Randy Lewis , David G. Richards

New, accurate measurements of the pion and kaon electromagnetic form factors are expected in the near future from experiments at electron-positron colliders,using the radiative return method. We construct a model for the timelike pion…

High Energy Physics - Phenomenology · Physics 2015-06-25 Christine Bruch , Alexander Khodjamirian , Johann H. Kuhn

The analysis of the $\pi\gamma$ transition form factor provides severe constraints on the pion's wave function. This information is used to examine charmonium decays into two pions critically. It will be argued that the standard…

High Energy Physics - Phenomenology · Physics 2007-05-23 Peter Kroll

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 study two versions of lightcone sum rules to calculate the $\gamma^*\gamma\rightarrow\pi^0$ transition form factor (TFF) within QCD. While the standard version is based on fixed-order perturbation theory by means of a power-series…

High Energy Physics - Phenomenology · Physics 2022-02-16 Sergey Mikhailov , Alexandr Pimikov , N. G. Stefanis

Within the basis light-front quantization framework, we systematically investigate the unpolarized and longitudinally polarized double parton distributions (DPDs) of quarks inside the proton. We utilize the light-front wave functions of the…

High Energy Physics - Phenomenology · Physics 2025-07-11 Tian-Cai Peng , Zhi Hu , Sreeraj Nair , Siqi Xu , Xiang Liu , Chandan Mondal , Xingbo Zhao , James P. Vary

In this talk it is reported on an analysis of the form factors for the transitions from a photon to one of the pseudoscalar mesons pi0, eta, eta', etac within the modified perturbative approach in which quark transverse degrees of freedom…

High Energy Physics - Phenomenology · Physics 2015-05-30 Peter Kroll

Measurements and theoretical calculations of meson form factors are essential for our understanding of internal hadron structure and QCD, the dynamics that bind the quarks in hadrons. The pion electromagnetic form factor has been measured…

High Energy Physics - Lattice · Physics 2018-04-18 Jonna Koponen , André Zimermmane-Santos , Christine Davies , G. Peter Lepage , Andrew Lytle

We present a general representation for the nucleon distribution amplitudes and for the nucleon to pion transition distribution amplitudes in terms of light-cone wave functions. We apply our formalism to a light-cone constituent quark model…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. Pincetti , B. Pasquini , S. Boffi

Baryon-to-meson Transition Distribution Amplitudes (TDAs) encoding valuable new information on hadron structure appear as building blocks in the collinear factorized description for several types of hard exclusive reactions. In this paper,…

High Energy Physics - Experiment · Physics 2016-12-01 PANDA Collaboration , B. P. Singh , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher % , B. Liu , H. Liu , Z. Liu , X. Shen , C. Wang , J. Zhao % , M. Albrecht , M. Fink , F. H. Heinsius , T. Held , T. Holtmann , H. Koch , B. Kopf , M. Kümmel , G. Kuhl , M. Kuhlmann , M. Leyhe , M. Mikirtychyants , P. Musiol , A. Mustafa , M. Pelizäus , J. Pychy , M. Richter , C. Schnier , T. Schröder , C. Sowa , M. Steinke , T. Triffterer , U. Wiedner , R. Beck , C. Hammann , D. Kaiser , B. Ketzer , M. Kube , P. Mahlberg , M. Rossbach , C. Schmidt , R. Schmitz , U. Thoma , D. Walther , C. Wendel , A. Wilson , A. Bianconi , M. Bragadireanu , M. Caprini , D. Pantea , D. Pietreanu , M. E. Vasile , B. Patel , D. Kaplan , P. Brandys , T. Czyzewski , W. Czyzycki , M. Domagala , M. Hawryluk , G. Filo , M. Krawczyk , D. Kwiatkowski , E. Lisowski , F. Lisowski , T. Fiutowski , M. Idzik , B. Mindur , D. Przyborowski , K. Swientek , B. Czech , S. Kliczewski , K. Korcyl , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Malgorzata , K. Pysz , W. Schäfer , R. Siudak , A. Szczurek , J. Biernat , S. Jowzaee , B. Kamys , S. Kistryn , G. Korcyl , W. Krzemien , A. Magiera , P. Moskal , M. Palka , A. Psyzniak , Z. Rudy , P. Salabura , J. Smyrski , P. Strzempek , A. Wrońska , I. Augustin , I. Lehmann , D. Nicmorus , G. Schepers , L. Schmitt , M. Al-Turany , U. Cahit , L. Capozza , A. Dbeyssi , H. Deppe , R. Dzhygadlo , A. Ehret , H. Flemming , A. Gerhardt , K. Götzen , R. Karabowicz , R. Kliemt , J. Kunkel , U. Kurilla , D. Lehmann , J. Lühning , F. Maas , C. Morales Morales , M. C. Mora Espí , F. Nerling , H. Orth , K. Peters , D. Rodríguez Pineiro , N. Saito , T. Saito , A. Sánchez Lorente , C. J. Schmidt , C. Schwarz , J. Schwiening , M. Traxler , R. Valente , B. Voss , P. Wieczorek , A. Wilms , M. Zühlsdorf , V. M. Abazov , G. Alexeev , A. Arefiev , V. I. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Yu. I. Davydov , V. Kh. Dodokhov , A. A. Efremov , A. G. Fedunov , A. A. Festchenko , A. S. Galoyan , S. Grigoryan , A. Karmokov , E. K. Koshurnikov , V. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. Olshevskiy , M. A. Pasyuk , E. A. Perevalova , A. A. Piskun , T. A. Pocheptsov , G. Pontecorvo , V. K. Rodionov , Yu. N. Rogov , R. A. Salmin , A. G. Samartsev , M. G. Sapozhnikov , G. S. Shabratova , N. B. Skachkov , A. N. Skachkova , E. A. Strokovsky , M. K. Suleimanov , R. Sh. Teshev , V. V. Tokmenin , V. V. Uzhinsky , A. S. Vodopyanov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , D. Glazier , D. Watts , P. Woods , A. Britting , W. Eyrich , A. Lehmann , F. Uhlig , S. Dobbs , K. Seth , A. Tomaradze , T. Xiao , D. Bettoni , V. Carassiti , A. Cotta Ramusino , P. Dalpiaz , A. Drago , E. Fioravanti , I. Garzia , M. Savriè , G. Stancari , V. Akishina , I. Kisel , I. Kulakov , M. Zyzak , R. Arora , T. Bel , A. Gromliuk , G. Kalicy , M. Krebs , M. Patsyuk , M. Zuehlsdorf , N. Bianchi , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , G. Bracco , M. Macri , R. F. Parodi , S. Bianco , D. Bremer , K. T. Brinkmann , S. Diehl , V. Dormenev , P. Drexler , M. Düren , T. Eissner , E. Etzelmüller , K. Föhl , M. Galuska , T. Gessler , E. Gutz , A. Hayrapetyan , J. Hu , B. Kröck , W. Kühn , T. Kuske , S. Lange , Y. Liang , O. Merle , V. Metag , D. Mülhheim , D. Münchow , M. Nanova , R. Novotny , A. Pitka , T. Quagli , J. Rieke , C. Rosenbaum , R. Schnell , B. Spruck , H. Stenzel , U. Thöring , M. Ullrich , T. Wasem , M. Werner , H. G. Zaunick , D. Ireland , G. Rosner , B. Seitz , P. N. Deepak , A. V. Kulkarni , A. Apostolou , M. Babai , M. Kavatsyuk , P. Lemmens , M. Lindemulder , H. Löhner , J. Messchendorp , P. Schakel , H. Smit , J. C. van der Weele , M. Tiemens , R. Veenstra , S. Vejdani , K. Kalita , D. P. Mohanta , A. Kumar , A. Roy , R. Sahoo , H. Sohlbach , M. Büscher , L. Cao , A. Cebulla , D. Deermann , R. Dosdall , S. Esch , I. Georgadze , A. Gillitzer , A. Goerres , F. Goldenbaum , D. Grunwald , A. Herten , Q. Hu , G. Kemmerling , H. Kleines , V. Kozlov , A. Lehrach , S. Leiber , R. Maier , R. Nellen , H. Ohm , S. Orfanitski , D. Prasuhn , E. Prencipe , J. Ritman , S. Schadmand , J. Schumann , T. Sefzick , V. Serdyuk , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , S. Li , Z. Li , Z. Sun , H. Xu , V. Rigato , S. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schröder , P. Achenbach , S. Bleser , M. Cardinali , O. Corell , M. Deiseroth , A. Denig , M. Distler , F. Feldbauer , M. Fritsch , P. Jasinski , M. Hoek , D. Kangh , A. Karavdina , W. Lauth , H. Leithoff , H. Merkel , M. Michel , C. Motzko , U. Müller , O. Noll , S. Plueger , J. Pochodzalla , S. Sanchez , S. Schlimme , C. Sfienti , M. Steinen , M. Thiel , T. Weber , M. Zambrana , V. I. Dormenev , A. A. Fedorov , M. V. Korzihik , O. V. Missevitch , P. Balanutsa , V. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , V. Varentsov , A. Boukharov , O. Malyshev , I. Marishev , A. Semenov , I. Konorov , S. Paul , S. Grieser , A. K. Hergemöller , A. Khoukaz , E. Köhler , A. Täschner , J. Wessels , S. Dash , M. Jadhav , S. Kumar , P. Sarin , R. Varma , V. B. Chandratre , V. Datar , D. Dutta , V. Jha , H. Kumawat , A. K. Mohanty , B. Roy , Y. Yan , K. Chinorat , K. Khanchai , L. Ayut , S. Pornrad , A. Y. Barnyakov , A. E. Blinov , V. E. Blinov , V. S. Bobrovnikov , S. A. Kononov , E. A. Kravchenko , I. A. Kuyanov , A. P. Onuchin , A. A. Sokolov , Y. A. Tikhonov , E. Atomssa , T. Hennino , M. Imre , R. Kunne , C. Le Galliard , B. Ma , D. Marchand , S. Ong , B. Ramstein , P. Rosier , E. Tomasi-Gustafsson , J. Van de Wiele , G. Boca , S. Costanza , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , V. Abramov , N. Belikov , S. Bukreeva , A. Davidenko , A. Derevschikov , Y. Goncharenko , V. Grishin , V. Kachanov , V. Kormilitsin , Y. Melnik , A. Levin , N. Minaev , V. Mochalov , D. Morozov , L. Nogach , S. Poslavskiy , A. Ryazantsev , S. Ryzhikov , P. Semenov , I. Shein , A. Uzunian , A. Vasiliev , A. Yakutin , B. Yabsley , T. Bäck , B. Cederwall , K. Makónyi , P. E. Tegnér , K. M. von Würtemberg , S. Belostotski , G. Gavrilov , A. Izotov , A. Kashchuk , O. Levitskaya , S. Manaenkov , O. Miklukho , Y. Naryshkin , K. Suvorov , D. Veretennikov , A. Zhadanov , A. K. Rai , S. S. Godre , R. Duchat , A. Amoroso , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Fava , L. Ferrero , M. Greco , M. Maggiora , G. Maniscalco , S. Marcello , S. Sosio , S. Spataro , L. Zotti , D. Calvo , S. Coli , P. De Remigis , A. Filippi , G. Giraudo , S. Lusso , G. Mazza , M. Mingnore , A. Rivetti , R. Wheadon , F. Balestra , F. Iazzi , R. Introzzi , A. Lavagno , H. Younis , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , B. Gålnander , L. Caldeira Balkeståhl , H. Calén , K. Fransson , T. Johansson , A. Kupsc , P. Marciniewski , J. Pettersson , K. Schönning , M. Wolke , J. Zlomanczuk , J. Díaz , A. Ortiz , P. C. Vinodkumar , A. Parmar , A. Chlopik , D. Melnychuk , B. Slowinski , A. Trzcinski , M. Wojciechowski , S. Wronka , B. Zwieglinski , P. Bühler , J. Marton , K. Suzuki , E. Widmann , J. Zmeskal , B. Fröhlich , D. Khaneft , D. Lin , I. Zimmermann , K. Semenov-Tian-Shansky

This letter is an investigation of the pion form factor utilizing recently developed effective field theory techniques. The primary results reported are: Both the transition and electromagnetic form factors are corrected at order…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ira Z. Rothstein

We have reexamined the elastic pion form factor over a broad range of momentum transfers with the mass evolution from current quark to constituent quark being taken into account. We have also studied the effect of Sudakov form factors, of…

High Energy Physics - Phenomenology · Physics 2016-09-01 Leonard S. Kisslinger , Siwen Wang

The CLEO experimental data on the $\pi\gamma$ transition are analyzed to next-to-leading order accuracy in QCD perturbation theory using light-cone QCD sum rules. By processing these data along the lines proposed by Schmedding and Yakovlev,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alexander P. Bakulev , S. V. Mikhailov , N. G. Stefanis

The pion electromagnetic form factor is investigated by using the dispersion relation with the superconvergence condition, which was proposed to synthesize the vector meson dominance model and QCD. The absorptive part is given as an…

High Energy Physics - Phenomenology · Physics 2007-05-23 Keiji Watanabe , Hirohisa Ishikawa , Masami Nakagawa

We take into account dynamical spin effects in the holographic light-front pion wavefunction in order to predict the pion radius, decay constant, the pion electromagnetic and photon-to-pion transition form factors. We report a striking…

High Energy Physics - Phenomenology · Physics 2017-04-12 M. Ahmady , F. Chishtie , R. Sandapen

We present the differential branching fractions for the $B\rightarrow \psi \pi\pi$ decays with the charmonia $\psi=J/\psi,\psi(2S)$ in the invariant mass of the $P$-wave pion pairs in the perturbative QCD approach. The two-pion distribution…

High Energy Physics - Phenomenology · Physics 2018-12-12 Zhou Rui , Ya Li , Hsiang-nan Li

We present predictions for the pion-photon transition form factor, derived with the help of light-cone sum rules and including the main part of the NNLO radiative corrections. We show that, when the Bakulev-Mikhailov-Stefanis (BMS) pion…

High Energy Physics - Phenomenology · Physics 2015-05-14 S. V. Mikhailov , N. G. Stefanis

In a Poincare'-covariant vector-boson-exchange theory, the pion possesses components of pseudovector origin, which materially influence its observable properties. For a range of such quantities, we explore the consequences of a…

Nuclear Theory · Physics 2010-11-11 L. X. Gutierrez-Guerrero , A. Bashir , I. C. Cloet , C. D. Roberts
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