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Related papers: Exclusive diffractive photoproduction of dileptons…

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Dilepton production from two photon interactions $\gamma\gamma\rightarrow l^+l^-$ are studied in semi-central and peripheral nuclear collisions. Based on Weizs\"acker-Williams approach, it is shown that the dilepton photoproduction is…

Nuclear Theory · Physics 2020-02-19 Guansong Li , Kai Zhou , Baoyi Chen

For the first time at LEP the production of prompt photons is studied in the collisions of quasi-real photons using the OPAL data taken at e+e- centre-of-mass energies between 183 GeV and 209 GeV. The total inclusive production…

High Energy Physics - Experiment · Physics 2008-11-26 The OPAL collaboration , G. Abbiendi

The reaction e+ e- -> e+ e- gamma* gamma* -> e+ e- hadrons is analysed for quasi-real virtual photons using data collected by the L3 detector during the LEP high energy runs at sqrt(s) = 183 and 189 GeV. Preliminary results on the cross…

High Energy Physics - Experiment · Physics 2007-05-23 Akos Csilling

First we calculate cross section for the $\gamma p \to \omega p$ reaction from the threshold to very large energies. At low energies the pion exchange is the dominant mechanism. At large energies the experimental cross section can be well…

High Energy Physics - Phenomenology · Physics 2015-03-18 Anna Cisek , Piotr. Lebiedowicz , Wolfgang Schäfer , Antoni Szczurek

We discuss diffractive production of open charm and bottom mesons at the LHC. The differential cross sections for single- and central-diffractive mechanisms for $c\bar c$ and $b\bar b$ pair production are calculated in the framework of the…

High Energy Physics - Phenomenology · Physics 2015-03-25 Marta Luszczak , Rafal Maciula , Antoni Szczurek

Deeply Virtual Compton Scattering in the near forward kinematic region is the golden access to Generalized Parton Distributions. We studied the O(alphaS) corrections to the scattering amplitude for both spacelike and timelike kinematics…

High Energy Physics - Phenomenology · Physics 2015-06-18 H. Moutarde , B. Pire , F. Sabatié , L. Szymanowski , J. Wagner

We report the measurement of the $\gamma p \rightarrow K^{+}\Lambda$ and $\gamma p \rightarrow K^{+}\Sigma^{0}$ reactions at SPring-8. The differential cross sections and photon-beam asymmetries are measured at forward $K^{+}$ production…

The next-to-leading-order (NLO) cross section for the production of heavy quarks at large transverse momenta ($p_\perp$) in $\gamma\gamma$ collisions is calculated with perturbative fragmentation functions (PFF's). This approach allows for…

High Energy Physics - Phenomenology · Physics 2016-08-15 M. Cacciari , M. Greco , B. A. Kniehl , M. Krämer , G. Kramer , M. Spira

At the electron-proton collider HERA the inclusive $D^{*\pm}$ meson photoproduction cross section has been measured with the H1 detector in two different, but partly overlapping, kinematical regions. For the first, where $<W_{\gamma p}>…

High Energy Physics - Experiment · Physics 2008-11-26 S. Aid

The cross section for the diffractive reaction gamma* + p -> c cbar + p with a real or virtual photon is calculated in the nonperturbative two-gluon exchange model of Landshoff and Nachtmann. Numerical predictions are given for cross…

High Energy Physics - Phenomenology · Physics 2015-06-25 M. Diehl

In the framework of the kt-factorization approach, the isolated prompt photon pair production in pp and p \bar p collisions at high energies is studied. The consideration is based on the quark-antiquark annihilation, quark-gluon scattering…

High Energy Physics - Phenomenology · Physics 2013-02-11 A. V. Lipatov

Exclusive photoproduction cross sections have been measured for the process $\gamma p \rightarrow p\pi^0(e^+e^-(\gamma))$ with the Dalitz decay final state using tagged photon energies in the range of $E_{\gamma} = 1.275-5.425$ GeV. The…

High Energy Physics - Experiment · Physics 2018-08-01 M. C. Kunkel , 32 , 18 M. J. Amaryan , 32 , I. I. Strakovsky , 16 J. Ritman , 3 , 18 G. R. Goldstein , 43 K. P. Adhikari , 28 S Adhikari , 13 H. Avakian , 39 J. Ball , 7 I. Balossino , 19 L. Barion , 19 M. Battaglieri , 21 V. Batourine , 39 , 27 I. Bedlinskiy , 25 A. S. Biselli , 11 , 5 S. Boiarinov , 39 W. J. Briscoe , 16 W. K. Brooks , 40 , 39 S. Bueltmann , 32 V. D. Burkert , 39 F. Cao , 9 D. S. Carman , 39 A. Celentano , 21 G. Charles , 32 T. Chetry , 31 G. Ciullo , 19 , 12 L. Clark , 42 P. L. Cole , 17 M. Contalbrigo , 19 O. Cortes , 17 V. Crede , 14 A. DAngelo , 22 , 35 N. Dashyan , 47 R. De Vita , 21 E. De Sanctis , 20 P. V. Degtyarenko , 39 M. Defurne , 7 A. Deur , 39 C. Djalali , 37 M. Dugger , 2 R. Dupre , 24 H. Egiyan , 39 A. El Alaoui , 40 L. El Fassi , 28 L. Elouadrhiri , 39 P. Eugenio , 14 G. Fedotov , 31 R. Fersch , 8 , 46 A. Filippi , 23 A. Fradi , 24 G. Gavalian , 39 , 29 Y. Ghandilyan , 47 S. Ghosh , 10 G. P. Gilfoyle , 34 K. L. Giovanetti , 26 F. X. Girod , 39 D. I. Glazier , 42 W. Gohn , 9 , E. Golovatch , 36 R. W. Gothe , 37 K. A. Griffioen , 46 L. Guo , 13 , 39 M. Guidal , 24 K. Hafidi , 1 H. Hakobyan , 40 , 47 N. Harrison , 39 M. Hattawy , 1 K. Hicks , 31 M. Holtrop , 29 C. E. Hyde , 32 D. G. Ireland , 42 B. S. Ishkhanov , 36 E. L. Isupov , 36 D. Jenkins , 44 K. Joo , 9 M. L. Kabir , 28 D. Keller , 45 G. Khachatryan , 47 M. Khachatryan , 32 M. Khandaker , 30 , A. Kim , 9 W. Kim , 27 A. Klein , 32 F. Klein , 6 , 16 V. Kubarovsky , 39 S. E. Kuhn , 32 J. M. Laget , 39 , 7 L. Lanza , 22 , 35 P. Lenisa , 19 D. Lersch , 18 K. Livingston , 42 I . J . D. MacGregor , 42 N. Markov , 9 G. Mbianda , 32 B. McKinnon , 42 T. Mineeva , 40 , 9 V. Mokeev , 39 , 36 R. A. Montgomery , 42 A Movsisyan , 19 C. Munoz Camacho , 24 P. Nadel-Turonski , 39 S. Niccolai , 24 G. Niculescu , 26 M. Osipenko , 21 A. I. Ostrovidov , 14 M. Paolone , 38 K. Park , 39 , 37 E. Pasyuk , 39 D. Payette , 32 W. Phelps , 13 , 16 O. Pogorelko , 25 J. Poudel , 32 J. W. Price , 4 S. Procureur , 7 Y. Prok , 32 , 45 D. Protopopescu , 42 M. Ripani , 21 B. G. Ritchie , 2 A. Rizzo , 22 , 35 G. Rosner , 42 A. Roy , 10 F. Sabatie , 7 C. Salgado , 30 S. Schadmand , 18 R. A. Schumacher , 5 Y. G. Sharabian , 39 Iu. Skorodumina , 37 , 36 D. G. Ireland , 42 D. Sokhan , 42 D. I. Sober , 6 N. Sparveris , 38 S. Strauch , 37 , 16 M. Taiuti , 21 , 15 J. A. Tan , 27 M. Ungaro , 39 , 33 H. Voskanyan , 47 E. Voutier , 24 D. P. Watts , 41 L. Weinstein , 32 X. Wei , 39 D. P. Weygand , 8 N. Zachariou , 41 J. Zhang , 45 , Z. W. Zhao32

We calculate diffractive dijet production in deep-inelastic scattering at next-to-leading order of perturbative QCD, including contributions from direct and resolved photons, and compare our predictions to preliminary data from the H1…

High Energy Physics - Phenomenology · Physics 2014-11-18 M. Klasen , G. Kramer

Instrumenting the LHC to measure the outgoing protons in the process pp -> p+X+p opens up new possibilities for physics studies in the Standard Model and beyond. In this talk I first present an overview of the underlying QCD calculation and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jeffrey R. Forshaw

The amplitudes for the $p p \to p p \pi^{0}$ process applicable at high energy are discussed in detail. Both diffractive bremsstrahlung (Drell-Hiida-Deck--type model), photon-photon and photon-omega exchange mechanisms are included in the…

High Energy Physics - Phenomenology · Physics 2013-05-08 Piotr Lebiedowicz , Antoni Szczurek

Following recent predictions that the geometric scaling properties of deep inelastic scattering data in inclusive gamma*-p collisions are expected also in exclusive diffractive processes, we investigate the diffractive production of vector…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Marquet , R. Peschanski , G. Soyez

We show that the data on $\gamma p$ and $\gamma\gamma$ interactions can be derived from the $pp$ and $\bar p p$ forward scattering amplitudes using vector meson dominance and the additive quark model. The nucleon-nucleon data are…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. M. Block , E. M. Gregores , F. Halzen , G. Pancheri

In this paper we propose the study of the diffractive quarkonium photoproduction in $pp$ collisions at LHC energies to probe the photon flux associated to a ultrarelativistic proton. The total photon distribution is expected to be given in…

High Energy Physics - Phenomenology · Physics 2015-03-16 V. P. Goncalves , G. Gil da Silveira

The production of jets in low $Q^2$ $ep$ scattering (photoproduction) and in low $Q^2$ $e^+e^-$ scattering ($\gamma\gamma$ scattering) allows for testing perturbative QCD and for measuring the proton and photon structure functions. This…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Klasen , Thorsten Kleinwort , Gustav Kramer

We compute the order-$\as$ corrections to the total cross section and to jet rates for the process $\epem\to\epem +$ hadrons, where the hadrons are produced through crossed-channel quark exchange in the hard scattering of two off-shell…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Cacciari , V. Del Duca , S. Frixione , Z. Trocsanyi
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