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Related papers: Pion structure in QCD: From theory to lattice to e…

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We apply the non-local chiral quark model to study vector and axial pion-to-photon transition amplitudes that are needed as a nonperturbative input to estimate the cross section of pion annihilation into the real and virtual photon. We use…

High Energy Physics - Phenomenology · Physics 2009-07-22 Piotr Kotko , Michal Praszalowicz

We analyze the moments of parton distribution functions in the pion calculated in lattice QCD, paying particular attention to their chiral extrapolation. Using the lowest three non-trivial moments calculated on the lattice, we assess the…

High Energy Physics - Lattice · Physics 2008-11-26 W. Detmold , W. Melnitchouk , A. W. Thomas

The electromagnetic form factor of the pion is calculated in the "point-form" of relativistic quantum mechanics using simple, phenomenological wave functions. It is found that the squared charge radius of the pion is predicted one order of…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Amghar , B. Desplanques , L. Theussl

Based on a global fit to experimental measurements of the pion electromagnetic form factor and parton distribution functions (PDFs), we report a data-driven determination of the unpolarized quark generalized parton distributions (GPDs) for…

High Energy Physics - Phenomenology · Physics 2026-04-14 Satyajit Puhan , Shubham Sharma , Narinder Kumar , Harleen Dahiya

We use dispersive techniques to address the behavior of the pion form factor as $Q^2 \to \infty$ and $Q^2 \to 0$. We perform the matching with the constraints of perturbative QCD and chiral perturbation theory in the high energy and low…

High Energy Physics - Phenomenology · Physics 2011-07-19 John F. Donoghue , Euy Soo Na

The pion light-cone distribution amplitude (LCDA) is a central non-perturbative object of interest for high-energy exclusive processes in quantum chromodynamics. In this article, the second Mellin moment of the pion LCDA is determined as a…

High Energy Physics - Lattice · Physics 2022-02-23 William Detmold , Anthony Grebe , Issaku Kanamori , C. -J. David Lin , Santanu Mondal , Robert Perry , Yong Zhao

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

We calculate the electromagnetic form factor of the pion in quenched lattice QCD. The non-perturbatively improved Sheikoleslami-Wohlert lattice action is used together with the consistently O(a) improved current. We calculate the pion form…

High Energy Physics - Lattice · Physics 2009-11-10 J. van der Heide , J. H. Koch , E. Laermann

The electromagnetic pion form factor, $F_\pi(q^2)$, is calculated for spacelike-$q^2$ in impulse approximation using a confining quark propagator, $S$, and a dressed quark-photon vertex, $\Gamma_\mu$, obtained from realistic,…

High Energy Physics - Phenomenology · Physics 2010-03-04 Craig D. Roberts

We analyze $F_\pi(Q^2)$ and $F_{P\gamma}(Q^2)$, $P=\pi,\eta,\eta'$, within the local-duality (LD) version of QCD sum rules, which allows one to obtain predictions for hadron form factors in a broad range of momentum transfers. To probe the…

High Energy Physics - Phenomenology · Physics 2012-02-14 Irina Balakireva , Wolfgang Lucha , Dmitri Melikhov

We adopt a non-perturbative relativistic constituent-quark model for the pi-meson electromagnetic form factor, which have successfully predicted experimental results, and supplement it with the effective momentum-dependent quark mass to…

High Energy Physics - Phenomenology · Physics 2013-11-19 S. V. Troitsky , V. E. Troitsky

We scrutinize recent findings on the charged-pion elastic form factor and the form factors entering in neutral-meson-to-photons transition amplitudes within the framework of QCD sum rules.

High Energy Physics - Phenomenology · Physics 2015-06-05 Irina Balakireva , Wolfgang Lucha , Dmitri Melikhov

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

Following Polchinski and Strassler [1] and our previous work [2], we study high-energy pion scattering in the holographic QCD hard-wall model. In particular, we focus on comparing our predictions for the angular dependence of $\pi^{+}…

High Energy Physics - Phenomenology · Physics 2026-04-08 Adi Armoni , Dorin Weissman

We propose a data-driven approach to extract the Kaon leading-twist distribution amplitude (DA) from empirical information on the ratio of the neutral-to-charged kaon electromagnetic form factors, $\mathcal{R}_K$. Our study employs a…

High Energy Physics - Phenomenology · Physics 2025-04-11 Lei Chang , Yu-Bin Liu , Khépani Raya , M. Atif Sultan

Generalized Parton Distributions of the pion are evaluated in chiral quark models with the help of double distributions. As a result the polynomiality conditions are automatically satisfied. In addition, positivity constraints, proper…

High Energy Physics - Phenomenology · Physics 2009-11-13 Wojciech Broniowski , Enrique Ruiz Arriola , Krzysztof Golec-Biernat

The behavior of the transition pion form factor for processes \gamma^*\gamma -> \pi^0 and \gamma^* \gamma^* -> \pi^0 at large values of space-like photon momenta is estimated within the nonlocal covariant quark-pion model. It is shown that,…

High Energy Physics - Phenomenology · Physics 2009-10-31 I. V. Anikin , A. E. Dorokhov , Lauro Tomio

We revisit the hard QCD contributions to the pion gravitational form factors (GFFs), in terms of the twist-2,3 pion distribution amplitudes (DA), including novel semi-hard contributions from the instantons. The pion DAs are evaluated in the…

High Energy Physics - Phenomenology · Physics 2024-10-16 Wei-Yang Liu , Edward Shuryak , Ismail Zahed

We report on our computation of the pion transition form factor ${\cal F}_{P\rightarrow \gamma^*\gamma^*}$ from twisted mass lattice QCD in order to determine the numerically dominant light pseudoscalar pole contribution in the hadronic…

A model for the twist-3 wave function $\psi_p(x,\mathbf{k_\perp})$ of the pion has been constructed based on the moment calculation by applying the QCD sum rules, whose distribution amplitude has a better end-point behavior than that of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tao Huang , Xing-Gang Wu
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