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The study of color transparency (CT) in elastic electroproduction of vector mesons off nuclei encounters the problem of the onset of coherence length (CL) effects. The problem of CT-CL separation arises especially at medium energies,…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. Z. Kopeliovich , J. Nemchik , Ivan Schmidt

Within a light-cone QCD formalism based on the Green function technique incorporating color transparency, coherence length effects and gluon shadowing we study electroproduction of vector mesons off nuclei. We found rather large color…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. Nemchik

Using the light-cone QCD dipole formalism we investigate manifestations of color transparency (CT) and coherence length (CL) effects in electroproduction of longitudinally (L) and transversally (T) polarized vector mesons. Motivated by…

High Energy Physics - Phenomenology · Physics 2008-12-18 B. Z. Kopeliovich , J. Nemchik , Ivan Schmidt

Within a light-cone QCD formalism which incorporates color transparency (CT), coherence length (CL) effects and gluon shadowing (GS) we study electroproduction of charmonia off nuclei. In contrast to production of light vector mesons…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. Nemchik

Study of color transparency (CT) effects at moderate energies is more problematic than is usually supposed. Onset of CT can be imitated by other mechanisms, which contain no explicit QCD dynamics. In the case of the $(e,e'p)$ reaction the…

Nuclear Theory · Physics 2008-02-03 B. Z. Kopeliovich , J. Nemchik

Interference between vector mesons electroproduced at different longitudinal coordinates leads within Glauber approximation to a $Q^2$-dependence of nuclear effects similar to what is expected to be an onset of color transparency (CT). We…

Nuclear Theory · Physics 2007-05-23 J. Huefner , B. Z. Kopeliovich

We argue that study of the cross section of coherent photo(electro) production of vector mesons off nuclear targets provides an effective method to probe the leading twist hard QCD regimes of color transparency and perturbative color…

High Energy Physics - Phenomenology · Physics 2014-11-17 L. Frankfurt , M. Strikman , M. Zhalov

The variation of the coherence length $l_c=2\nu/(Q^2+m_V^2)$ in virtual photoproduction of vector mesons off nuclei as a function of the photon energy $\nu$ or virtuality $Q^2$ results in dramatic changes in the values of the nuclear…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Huefner , B. Kopeliovich , J. Nemchik

Coherent electroproduction of vector mesons off $^2$H and $^4$He is considered in the kinematics of deep inelastic scattering. Special emphasis is given to the $-t\sim 0.8-1$ GeV$^2$ region where the cross section is dominated by the…

High Energy Physics - Phenomenology · Physics 2007-05-23 L. Frankfurt , V. Guzey , W. Koepf , M. Sargsian , M. Strikman

Exclusive coherent and incoherent electroproduction of the $\rho^0$ meson from $^1$H and $^{14}$N targets has been studied at the HERMES experiment as a function of coherence length ($l_c$), corresponding to the lifetime of hadronic…

High Energy Physics - Experiment · Physics 2008-11-26 HERMES Collaboration , A. Airapetian

Color transparency (CT) is an effect of suppression of nuclear shadowing of hard reactions, closely related to the color screening. A brief review of theoretical development and experimental search for CT, failed and successful, are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Boris Kopeliovich

We argue that study of the cross section of coherent photo(electro) production of $\rho,\rho^{\prime}, ...$-mesons provides an effective method to probe onset of black body limit(BBL) in the soft and hard QCD interactions. We illustrate the…

High Energy Physics - Phenomenology · Physics 2009-11-07 L. Frankfurt , M. Strikman , M. Zhalov

We demonstrate how the virtual photoproduction of vector mesons on nuclei scans the wave function of vector mesons from the large non-perturbative transverse size $\rho \sim R_{V}$ down to the small perturbative size $\rho \sim…

High Energy Physics - Phenomenology · Physics 2009-10-22 B. Z. Kopeliovich , J. Nemchick , N. N. Nikolaev , B. G. Zakharov

We study the electroproduction of rho mesons in nuclei at intermediate energies, deriving a treatment of the energy lost by the rho in each step of multiple-scattering. This enables a close match between calculations and the experimental…

Nuclear Theory · Physics 2008-11-26 L. Frankfurt , G. A Miller , M. Strikman

A systematic multiple scattering formalism for vector meson electroproduction from nuclei is developed, with emphasis on the formation, propagation and hadronization scales for quark-gluon fluctuations of the virtual high-energy photon. The…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. Renk , G. Piller , W. Weise

The exclusive production of vector mesons in deep inelastic scattering is a hard scattering process with the well controlled size of quark configurations which dominate the production amplitude. This allows an unambiguous prediction of…

High Energy Physics - Phenomenology · Physics 2012-08-27 B. Z. Kopeliovich , J. Nemchick , N. N. Nikolaev , and B. G. Zakharov

We review a unique prediction of Quantum Chromo Dynamics, called color transparency (CT), where the final (and/or initial) state interactions of hadrons with the nuclear medium must vanish for exclusive processes at high momentum transfers.…

Nuclear Theory · Physics 2015-06-12 D. Dutta , K. Hafidi , M. Strikman

We show that nuclear sigma, omega, and pi mesons can contribute coherently to enhance the electroproduction cross section on nuclei for longitudinal virtual photons at low Q^2 while depleting the cross section for transverse photons. We are…

High Energy Physics - Phenomenology · Physics 2009-09-11 G. A. Miller , S. J. Brodsky , M. Karliner

We review the current status of the phenomenon of Color Transparency (CT), a fundamental consequence of the description of hadrons from Quantum Chromo Dynamics. CT refers to the vanishing of final (and/or initial) state interactions with…

Nuclear Experiment · Physics 2025-08-20 Holly Szumila-Vance , Dipangkar Dutta , Gerald A. Miller , Misak Sargsian

We have measured the nuclear transparency of the incoherent diffractive $A(e,e'\rho^0)$ process in $^{12}$C and $^{56}$Fe targets relative to $^2$H using a 5 GeV electron beam. The nuclear transparency, the ratio of the produced $\rho^0$'s…

Nuclear Experiment · Physics 2015-06-03 L. El Fassi , L. Zana , K. Hafidi , M. Holtrop , B. Mustapha , W. K. Brooks , H. Hakobyan , X. Zheng , K. P. Adhikari , D. Adikaram , M. Aghasyan , M. J. Amaryan , M. Anghinolfi , J. Arrington , H. Avakian , H. Baghdasaryan , M. Battaglieri , V. Batourine , I. Bedlinskiy , A. S. Biselli , C. Bookwalter , D. Branford , W. J. Briscoe , S. Bultmann , V. D. Burkert , D. S. Carman , A. Celentano , S. Chandavar , P. L. Cole , M. Contalbrigo , V. Crede , A. D'Angelo , A. Daniel , N. Dashyan , R. De Vita , E. De Sanctis , A. Deur , B. Dey , R. Dickson , C. Djalali , G. E. Dodge , D. Doughty , R. Dupre , H. Egiyan , A. El Alaoui , L. Elouadrhiri , P. Eugenio , G. Fedotov , S. Fegan , M. Y. Gabrielyan , M. Garcon , N. Gevorgyan , G. P. Gilfoyle , K. L. Giovanetti , F. X. Girod , J. T. Goetz , W. Gohn , E. Golovatch , R. W. Gothe , K. A. Griffioen , M. Guidal , L. Guo , C. Hanretty , D. Heddle , K. Hicks , R. J. Holt , C. E. Hyde , Y. Ilieva , D. G. Ireland , B. S. Ishkhanov , E. L. Isupov , S. S. Jawalkar , D. Keller , M. Khandaker , P. Khetarpal , A. Kim , W. Kim , A. Klein , F. J. Klein , V. Kubarovsky , S. E. Kuhn , S. V. Kuleshov , V. Kuznetsov , J. M. Laget , H. Y. Lu , I. J. D. MacGregor , Y. Mao , N. Markov , M. Mayer , J. McAndrew , B. McKinnon , C. A. Meyer , T. Mineeva , M. Mirazita , V. Mokeev , B. Moreno , H. Moutarde , E. Munevar , P. Nadel-Turonski , A. Ni , S. Niccolai , G. Niculescu , I. Niculescu , M. Osipenko , A. I. Ostrovidov , L. Pappalardo , R. Paremuzyan , K. Park , S. Park , E. Pasyuk , S. Anefalos Pereira , E. Phelps , S. Pisano , S. Pozdniakov , J. W. Price , S. Procureur , D. Protopopescu , B. A. Raue , P. E. Reimer , G. Ricco , D. Rimal , M. Ripani , B. G. Ritchie , G. Rosner , P. Rossi , F. Sabatie , M. S. Saini , C. Salgado , D. Schott , R. A. Schumacher , H. Seraydaryan , Y. G. Sharabian , E. S. Smith , G. D. Smith , D. I. Sober , D. Sokhan , S. S. Stepanyan , S. Stepanyan , P. Stoler , S. Strauch , M. Taiuti , W. Tang , C. E. Taylor , D. J. Tedeschi , S. Tkachenko , M. Ungaro , B . Vernarsky , M. F. Vineyard , H. Voskanyan , E. Voutier , D. Watts , L. B. Weinstein , D. P. Weygand , M. H. Wood , N. Zachariou , B. Zhao , Z. W. Zhao
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