Double-Hadron Leptoproduction in the Nuclear Medium

Airapetian, A.; Акопов, Н.; Akopov, Z.; Amarian, M.; Andrus, A.; Aschenauer, E. C.; Augustyniak, W.; Avakian, R.; Avetissian, A.; Avetissian, E.; Bailey, P.; Belostotski, S.; Bianchi, N.; Blok, H. P.; Böttcher, H.; Borissov, A.; Borysenko, A.; Brüll, A.; Bryzgalov, V.; Capiluppi, M.; Capitani, G. P.; Ciullo, G.; Contalbrigo, M.; Dalpiaz, P.; Deconinck, W.; Лео, Р. Де; Demey, M.; Nardo, L. De; Sanctis, E. De; Devitsin, E.; Diefenthaler, M.; Nezza, P. Di; Dreschler, J.; Düren, M.; Ehrenfried, M.; Elalaoui-Moulay, A.; Elbakian, G.; Ellinghaus, F.; Elschenbroich, U.; Fabbri, R.; Fantoni, A.; Felawka, L.; Frullani, S.; Funel, A.; Gapienko, G.; Гапиенко, В. А.; Garibaldi, F.; Garrow, K.; Gavrilov, G.; Gharibyan, V.; Giordano, F.; Grebeniouk, O.; Gregor, I. M.; Griffioen, K. A.; Güler, H.; Hadjidakis, C.; Hartig, M.; Hasch, D.; Hasegawa, T.; Hesselink, W.H.A.; Hillenbrand, A.; Hoek, M.; Holler, Y.; Hommez, B.; Hristova, I.; Iarygin, G.; Ivanilov, A.; Izotov, A.; Jackson, H. E.; Jgoun, A.; Kaiser, R.; Keri, T.; Kinney, E.; Kisselev, A.; Kobayashi, T.; Kopytin, M.; Коротков, В. А.; Kozlov, V.; Krauß, Bernhard; Kravchenko, P.; Krivokhijine, V. G.; Lagamba, L.; Lapikás, L.; Lenisa, P.; Liebing, P.; Linden-Levy, L. A.; Lorenzon, W.; Lu, J.; Lü, Shaozhe; Q., B.; Maiheu, B.; Makins, N.; Mao, Y.; Mariański, B.; Marukyan, H.; Masoli, F.; Mexner, V.; Meyners, N.; Michler, T.; Mikloukho, O.; Miller, C. A.; Miyachi, Y.; Muccifora, V.; Murray, M.; Нагайцев, А.; Nappi, E.; Naryshkin, Y.; Negodaev, M.; Nowak, W.-D.; Ohsuga, H.; Osborne, A.M.; Pérez-Benito, R.; Pickert, N.; Raithel, Martin; Reggiani, D.; Reimer, P. E.; Reischl, A.; Roelon, A. R.; Riedl, C.; Rith, Klaus; Rosner, G.; Rostomyan, A.; Rubáček, L.; Rubin, J.; Ryckbosch, D.; Salomatin, Y.; Sanjiev, I.; Savin, I.; Schäfer, Andreas; Schnell, G.; Schüler, K. P.; Seele, J.; Seidl, R.; Seitz, B.; Shearer, C.; Shibata, T. A.; Shutov, V.; Sinram, K.; Stancari, M.; Statera, M.; Steffens, E.; Steijger, J. J. M.; Stenzel, H.; Stewart, J.; Stinzing, F.; Streit, J.; Tait, P.; Tanaka, Hiroki; Taroian, S.; Tchuiko, B.; Terkulov, A.; Trzciński, A.; Tytgat, M.; Vandenbroucke, A.; Nat, P. B. van der; Steenhoven, G. van der; Haarlem, Y. Van; Veretennikov, D.; Vikhrov, V.; Vogel, Christian; Wang, S.; Ye, Y.; Ye, Z.; Yen, S.; Zihlmann, B.; Żuprański, P.

doi:10.1103/physrevlett.96.162301

Cited by 27 publications

(15 citation statements)

References 39 publications

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“…For SIDIS the relevant transverse SSA (Collins asymmetry) is schematically defined in (122). Both, HERMES and COMPASS performed measurements of Collins transverse SSA on proton targets [139,249,420,421,422] for charged pions and kaons. Fig.…”

Section: Experimental Data On Tmd Ff H ⊥mentioning

confidence: 99%

Parton fragmentation functions

Metz

Vossen

2016

Progress in Particle and Nuclear Physics

187

169

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The field of fragmentation functions of light quarks and gluons is reviewed. In addition to integrated fragmentation functions, attention is paid to the dependence of fragmentation functions on transverse momenta and on polarization degrees of freedom. Higher-twist and di-hadron fragmentation functions are considered as well. Moreover, the review covers both theoretical and experimental developments in hadron production in electron-positron annihilation, deep-inelastic lepton-nucleon scattering, and proton-proton collisions.

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Section: Experimental Data On Tmd Ff H ⊥mentioning

confidence: 99%

Parton fragmentation functions

Metz

Vossen

2016

Progress in Particle and Nuclear Physics

187

169

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show abstract

“…Liquefied noble gases, such as argon or xenon, are becoming more and more popular media for ionization particle detectors to be employed in high energy physics [1], neutrino physics [2][3][4][5][6][7][8], dark matter search experiments [9][10][11][12] and other applications in particle and astroparticle physics. The required target (detector) mass gradually increases with the precision of the experiments.…”

Section: Introductionmentioning

confidence: 99%

Experimental study of electric breakdowns in liquid argon at centimeter scale

Blatter¹,

Ereditato²,

Hsu³

et al. 2014

J. Inst.

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In this paper we present results on measurements of the dielectric strength of liquid argon near its boiling point and cathode-anode distances in the range of 0.1 mm to 40 mm with spherical cathode and plane anode. We show that at such distances the applied electric field at which breakdowns occur is as low as 40 kV/cm. Flash-overs across the ribbed dielectric of the high voltage feed-through are observed for a length of 300 mm starting from a voltage of 55 kV. These results contribute to set reference for the breakdown-free design of ionization detectors, such as Liquid Argon Time Projection Chambers (LAr TPC).

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“…[13], to (1 − α)R A + 2αR ′ A , where R A and R ′ A are the absorption functions for the hadron produced in the single string event and in one of the strings of the two string event, respectively. R ′ A is integrated over β with energy division functions w(β) presented by equations (12) and (14). Now, following the formalism of [13] we can write the NA in form:…”

Section: Resultsmentioning

confidence: 99%

Possible influence of the two string events on the hadron formation in a nuclear environment

2007

Self Cite

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One of the basic assumptions of the string model is that as a result of a DIS in nucleus a single string arises, which then breaks into hadrons. However the pomeron exchange considered in this work, leads to the production of two strings in the one event. The hadrons produced in these events have smaller formation lengths, than those with the same energy produced in the single string events. As a consequence, they undergo more substantial absorption in the nuclear matter.

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Double-Hadron Leptoproduction in the Nuclear Medium

Cited by 27 publications

References 39 publications

Parton fragmentation functions

Parton fragmentation functions

Experimental study of electric breakdowns in liquid argon at centimeter scale

Possible influence of the two string events on the hadron formation in a nuclear environment

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