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The transition pion-photon form factor is studied within the framework of Light-Cone QCD Sum Rules. The spectral density for the next-to-leading order corrections is calculated for any Gegenbauer harmonic. At the level of the…

High Energy Physics - Phenomenology · Physics 2011-05-13 S. V. Mikhailov , N. G. Stefanis

The meson-photon transition form factors $\gamma\gamma^*\to P$ ($P$ stands for $\pi$, $\eta$ and $\eta'$) provide strong constraints on the distribution amplitudes of the pseudoscalar mesons. In this paper, these transition form factors are…

High Energy Physics - Phenomenology · Physics 2011-10-11 Xing-Gang Wu , Tao Huang

The vector and axial pion-photon transition distribution amplitudes are analyzed in the Spectral Quark Model. We proceed by the evaluation of double distributions through the use of a manifestly covariant calculation based on the alpha…

High Energy Physics - Phenomenology · Physics 2010-10-27 Wojciech Broniowski , Enrique Ruiz Arriola

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

In this paper, we study the pion leading-twist distribution amplitude $\phi_{2;\pi}(x,\mu)$ by improving the traditional light-cone harmonic oscillator model within the reconstruction of the function $\varphi_{2;\pi}(x)$. In order to…

High Energy Physics - Phenomenology · Physics 2021-07-28 Tao Zhong , Zhi-Hao Zhu , Hai-Bing Fu , Xing-Gang Wu , Tao Huang

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 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

Pion electroproduction amplitudes predicted by three theoretical models in the $Q^2 \leq 0.5$ (GeV/c)$^2$ region are compared. The objective is to facilitate the analyses of the data from new experiments on investigating the pion cloud…

Nuclear Theory · Physics 2007-05-23 T. Sato , T. -S. H. Lee

We study the hard exclusive production of two pions in the virtual photon fragmentation region with various invariant masses including the resonance region. The amplitude is expressed in terms of two-pion light cone distribution amplitudes…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. V. Polyakov

High-statistics data on the $e^+e^-\to \pi^+\pi^-$ cross section and the pion vector form factor have been obtained recently by several collaborations. Unfortunately, there are some tensions between different datasets, especially the most…

High Energy Physics - Phenomenology · Physics 2020-11-18 B. Ananthanarayan , Irinel Caprini , Diganta Das

The charged pion form factor, Fpi(Q^2), is an important quantity which can be used to advance our knowledge of hadronic structure. However, the extraction of Fpi from data requires a model of the 1H(e,e'pi+)n reaction, and thus is…

Following the proposal in [1], we study the feasibility to calculate the pion distribution amplitude (DA) from suitably chosen Euclidean correlation functions at large momentum. In our lattice study we employ the novel momentum smearing…

Using non-local chiral quark model with simple pole ansatz for mass dependence on momentum and non-local currents satisfying Ward-Takahashi identities, we calculate pion to photon transition distribution amplitudes and relevant form…

High Energy Physics - Phenomenology · Physics 2009-11-06 P. Kotko , M. Praszalowicz

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

We consider the pion-photon transition form factor at low to intermediate spacelike momenta within the theoretical framework of light-cone sum rules. We derive predictions which take into account all currently known contributions stemming…

High Energy Physics - Phenomenology · Physics 2017-03-24 S. V. Mikhailov , A. V. Pimikov , N. G. Stefanis

A novel method is employed to compute the pion electromagnetic form factor, F_\pi(Q^2), on the entire domain of spacelike momentum transfer using the Dyson-Schwinger equation (DSE) framework in quantum chromodynamics (QCD). The DSE…

Nuclear Theory · Physics 2015-06-16 L. Chang , I. C. Cloet , C. D. Roberts , S. M. Schmidt , P. C. Tandy

We analyze the pion transition form factor using dispersion theory. We calculate the singly-virtual form factor in the time-like region based on data for the $e^+e^-\to 3\pi$ cross section, generalizing previous studies on…

High Energy Physics - Phenomenology · Physics 2014-12-19 Martin Hoferichter , Bastian Kubis , Stefan Leupold , Franz Niecknig , Sebastian P. Schneider

We describe the present status of the pion distribution amplitude as originated from two sources: (i) a nonperturbative approach, based on QCD sum rules with nonlocal condensates, and (ii) a NLO QCD analysis of the CLEO data on…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. P. Bakulev

We present an investigation of the pion's electromagnetic form factor F_{\pi}(Q^2) in the spacelike region utilizing two new ingredients: (i) a double-humped, endpoint-suppressed pion distribution amplitude derived before via QCD sum rules…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. P. Bakulev , K. Passek-Kumerički , W. Schroers , N. G. Stefanis

We study the pion electromagnetic and $\gamma^* + \pi^0 \to \gamma$ transition form factors at intermediate momentum transfer. We calculate soft, nonperturbative corrections to the leading perturbative amplitudes which arise from the $q\bar…

High Energy Physics - Phenomenology · Physics 2010-03-04 A. Szczepaniak , A. G. Williams