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Within the kt-factorization approach, we evaluate the impact factor of the transition gamma* -> rhoT taking into account the twist 3 contributions. We show that a gauge invariant expression is obtained with the help of QCD equations of…

High Energy Physics - Phenomenology · Physics 2009-09-23 I. V. Anikin , D. Yu. Ivanov , B. Pire , L. Szymanowski , S. Wallon

In the paper, we derive the $\xi$-moments $\langle\xi_{2;b_1}^{n;\|}\rangle$ of the longitudinal leading-twist distribution amplitude $\phi_{2;b_1}^{\|}$ for $^1P_1$-state $b_1(1235)$-meson by using the QCD sum rules under the background…

High Energy Physics - Phenomenology · Physics 2025-04-02 Long Zeng , Xing-Gang Wu , Dan-Dan Hu , Hai-Bing Fu , Tao Zhong

We suggest to carry out lattice calculations of current correlators in position space, sandwiched between the vacuum and a hadron state (e.g. pion), in order to access hadronic light-cone distribution amplitudes (DAs). In this way the…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. Braun , D. Müller

We apply chiral quark model with momentum dependent quark mass to two kinds of non-perturbative objects. These are: photon Distribution Amplitudes which we calculate up to twist-4 in tensor, vector and axial channels and pion-photon…

High Energy Physics - Phenomenology · Physics 2010-02-19 Piotr Kotko

Higher-twist transverse momentum dependent parton distribution functions (TMDs) are a valuable probe of the quark-gluon dynamics in the nucleon, and play a vital role for the explanation of sizable azimuthal asymmetries in hadron production…

High Energy Physics - Phenomenology · Physics 2015-06-23 C. Lorcé , B. Pasquini , P. Schweitzer

We present a novel framework for analyzing four-body semileptonic weak decays, performing the first high-twist analysis of the $D_s \to \left[ \pi\pi \right]_{\rm S}$ form factors using light-cone distribution amplitudes for the isoscalar…

High Energy Physics - Phenomenology · Physics 2026-02-04 Shan Cheng , Ling-yun Dai , Jian-ming Shen , Shu-lei Zhang

We describe a method of analytic evolution of distribution amplitudes (DA) that have singularities, such as non-zero values at the end-points of the support region, jumps at some points inside the support region and cusps. We illustrate the…

High Energy Physics - Phenomenology · Physics 2014-04-23 A. V. Radyushkin , A. Tandogan

We investigate the pseudoscalar (PS) meson ($\pi$ and $K$) quasi-distribution amplitude (QDA), which is supposed to be an asymptotic analog to the meson distribution amplitude (DA) $\phi_{\pi,K}(x)$ in the limit of the large longitudinal…

High Energy Physics - Phenomenology · Physics 2017-12-20 Seung-il Nam

Based on the flavor structure of four-quark effective operators, we develop an automatic computation program to calculate hadronic two-body $B$ meson decay amplitudes, and apply it to their global analysis in the perturbative QCD (PQCD)…

High Energy Physics - Phenomenology · Physics 2021-08-04 Jun Hua , Hsiang-nan Li , Cai-Dian Lu , Wei Wang , Zhi-Peng Xing

In this paper the dynamical spin effects of the light-front holographic wavefunctions for light pseudoscalar mesons are studied using two different assumptions. These improved wavefunctions are then confronted with a number of sensitive…

High Energy Physics - Phenomenology · Physics 2017-06-07 Qin Chang , Stanley J. Brodsky , Xin-Qiang Li

The recently-proposed quasi distributions point out a promising direction for lattice QCD to investigate the light-cone correlators, such as parton distribution functions (PDF) and distribution amplitudes (DA), directly in the $x$-space.…

High Energy Physics - Phenomenology · Physics 2016-11-09 Yu Jia , Xiaonu Xiong

To access information on the internal structure of the nucleon, data from a variety of scattering experiments can be analyzed, in regimes where the information factorizes from an otherwise known scattering amplitude. A recent development,…

High Energy Physics - Phenomenology · Physics 2024-04-05 B. Pasquini , A. Schiavi

The form factors of the light pseudoscalar mesons are investigated in a dispersive formalism based on hadronic unitarity, analyticity and the OPE expansion of the QCD Green functions. We propose generalizations of the original mathematical…

High Energy Physics - Phenomenology · Physics 2011-09-13 Irinel Caprini

We present a systematic study of the B meson light-cone distribution amplitudes which are relevant for the QCD factorization approach for the exclusive B meson decays. We construct representations for the quark-antiquark distribution…

High Energy Physics - Phenomenology · Physics 2009-11-07 Hiroyuki Kawamura , Jiro Kodaira , Cong-Feng Qiao , Kazuhiro Tanaka

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

We present the leading-twist quark transverse momentum-dependent parton distribution functions (TMDs) for the spin-1 target, such as the $\rho$-meson, in the light-front framework. Specifically, we predict the TMDs in the light-front…

High Energy Physics - Phenomenology · Physics 2021-02-24 Satvir Kaur , Chandan Mondal , Harleen Dahiya

Light-Front Quantization provides a physical, frame-independent formalism for hadron dynamics and structure. Observables such as structure functions, transverse momentum distributions, and distribution amplitudes are defined from the…

High Energy Physics - Phenomenology · Physics 2016-04-20 Stanley J. Brodsky

This paper is devoted to the study of leading twist light cone wave function of $\eta_c$ meson. The moments of this wave function have been calculated within three approaches: potential models, nonrelativistic QCD and QCD sum rules. Using…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. V. Braguta , A. K. Likhoded , A. V. Luchinsky

The light-front quantization of QCD provides an alternative to lattice gauge theory for computing the mass spectrum, scattering amplitudes, and other physical properties of hadrons directly in Minkowski space. Nonperturbative light-front…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. J. Brodsky

We investigate the leading-twist light-cone distribution amplitudes for the pion and kaon based on the gauge-invariant nonlocal chiral quark model from the instanton vacuum in the presence of external axial-vector currents. We find that the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Seung-il Nam , Hyun-Chul Kim
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