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Related papers: Pion-Photon Transition Distribution Amplitudes

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We study the exclusive production of pi-pi and rho-pi in hard gamma* gamma scattering in the forward kinematical region where the virtuality of one photon provides us with a hard scale in the process. The newly introduced concept of…

High Energy Physics - Phenomenology · Physics 2008-12-18 J. P. Lansberg , B. Pire , L. Szymanowski

The pion-photon Transition Distribution Amplitudes (TDAs) are studied, treating the pion as a bound state in the sense of Bethe-Salpeter, in the formalism of the NJL model. The results obtained explicitly verify support, sum rules and…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Courtoy , S. Noguera

Baryon to meson transition distribution amplitudes (TDAs) extend the concept of generalized parton distributions. Baryon to meson TDAs appear as building blocks in the collinear factorized description of amplitudes for a class of hard…

High Energy Physics - Phenomenology · Physics 2011-10-12 Bernard Pire , Kirill Semenov-Tian-Shansky , Lech Szymanowski

We use general relations between the Transition Distribution Amplitudes (TDAs), entering the description of the p -> pi0 transition, and the proton Distribution Amplitudes (DAs) in the soft-pion limit to estimate the size of the amplitude…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. P. Lansberg , B. Pire , L. Szymanowski

Baryon-to-meson Transition Distribution Amplitudes (TDAs) appear as building blocks in the collinear factorized description of amplitudes for a class of hard exclusive reactions, prominent examples being hard exclusive pion…

High Energy Physics - Phenomenology · Physics 2013-12-30 B. Pire , K. Semenov-Tian-Shansky , L. Szymanowski

We define the pion-photon Transition Distribution Amplitudes (TDA) in a field theoretic formalism from a covariant Bethe-Salpeter approach for the determination of the bound state. We apply our formalism to the Nambu - Jona Lasinio model,…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Courtoy , S. Noguera

Baryon-to-meson and baryon-to-photon transition distribution amplitudes (TDAs) arise in the collinear factorized description of a class of hard exclusive reactions characterized by the exchange of a non-zero baryon number in the cross…

High Energy Physics - Phenomenology · Physics 2022-02-02 B. Pire , K. Semenov-Tian-Shansky , L. Szymanowski

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

Baryon to meson transition distribution amplitudes (TDAs), non-diagonal matrix elements of the nonlocal three quark operator between a nucleon and a meson state, extend the concept of generalized parton distributions. These non-perturbative…

High Energy Physics - Phenomenology · Physics 2012-06-29 B. Pire , K. Semenov-Tian-Shansky , L. Szymanowski

The extension of the concept of generalized parton distributions leads to the introduction of baryon to meson transition distribution amplitudes (TDAs), non-diagonal matrix elements of the nonlocal three quark operator between a nucleon and…

High Energy Physics - Phenomenology · Physics 2015-06-03 J. P. Lansberg , B. Pire , K. Semenov-Tian-Shansky , L. Szymanowski

We study the exclusive production of pi pi and rho pi in hard gamma* gamma scattering in the forward kinematical region where the virtuality of one photon provides us with a hard scale in the process. The newly introduced concept of…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. P. Lansberg , B. Pire , L. Szymanowski

To study cross sections and polarization asymmetries for the processes $e p \to e n \pi^+$ and $e p \to e p \pi^0$ in the backward region, we develop a flexible phenomenological model for nucleon-to-pion transition distribution amplitudes…

High Energy Physics - Phenomenology · Physics 2025-11-03 Bernard Pire , Kirill Semenov-Tian-Shansky , Paweł Sznajder , Lech Szymanowski

We discuss the status of the pion distribution amplitude (DA) in connection with QCD sum rules and experimental data on the $\gamma^*\gamma^\to \pi^0$ transition form factor. Contents: (a) Pion DA in generalized QCD Sum Rules (SRs); (b)…

High Energy Physics - Phenomenology · Physics 2010-12-17 Alexander P. Bakulev , S. V. Mikhailov , N. G. Stefanis

We introduce a new approach to modeling transition distribution amplitudes (TDAs) for the processes $e p \to e n \pi^+$ and $e p \to e p \pi^0$. The modeling is flexible, constrained by sparsely available experimental data, and satisfies…

High Energy Physics - Phenomenology · Physics 2025-09-03 B. Pire , K. Semenov-Tian-Shansky , P. Sznajder , L. Szymanowski

We discuss the relevance of a dedicated measurement of exclusive production of a pair of neutral pions in a hard gamma* gamma scattering at small momentum transfer. In this case, the virtuality of one photon provides us with a hard scale in…

High Energy Physics - Phenomenology · Physics 2009-07-21 J. P. Lansberg , B. Pire , L. Szymanowski

We provide an in-depth analysis of the $\pi$ distribution amplitude in terms of two different Gegenbauer representations. Detailed predictions for the $\pi-\gamma$ transition form factor are presented, obtained with light-cone sum rules.…

High Energy Physics - Phenomenology · Physics 2014-12-01 N. G. Stefanis , S. V. Mikhailov , A. V. Pimikov

We discuss two applications of the {\it Virtuality Distribution Amplitudes} (VDA) formalism developed in our recent papers. We start with an overview of the main properties of the pion distribution amplitude emphasizing the quantitative…

High Energy Physics - Phenomenology · Physics 2015-10-13 A. V. Radyushkin

We report results on the $\pi$-$\gamma$ transition form factor obtained within the hard scattering approach including transverse momentum effects and Sudakov corrections. The results clearly favor distribution amplitudes close to the…

High Energy Physics - Phenomenology · Physics 2009-09-25 R. Jakob , P. Kroll , M. Raulfs

The exclusive production of \pi\pi and \pi\rho in hard \gamma^{\star}\gamma scattering in the forward kinematical region where the virtual photon is highly off-shell are studied through the \gamma\to\pi^- Transition Distribution Amplitudes.…

High Energy Physics - Phenomenology · Physics 2009-03-31 A. Courtoy , S. Noguera

We study the scaling regime of nucleon-anti-nucleon annihilation into a deeply virtual photon and a photon or meson, \bar p N -> gamma ^* pi, \bar p N -> gamma ^* gamma, in the forward direction. The leading twist amplitude factorizes into…

High Energy Physics - Phenomenology · Physics 2011-04-11 B. Pire , L. Szymanowski
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