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Statements

Subject Item
n2:RIV%2F68407700%3A21340%2F14%3A00219198%21RIV15-MSM-21340___
rdf:type
skos:Concept n12:Vysledek
rdfs:seeAlso
http://www.epj-conferences.org/articles/epjconf/abs/2014/08/epjconf_icnfp2013_00070/epjconf_icnfp2013_00070.html
dcterms:description
A parton produced with a high transverse momentum in a hard collision is regenerating its color field, intensively radiating gluons and losing energy. This process cannot last long, if it ends up with production of a leading hadron carrying the main fraction zh of the initial parton momentum. So energy conservation imposes severe constraints on the length scale of production of a single hadron with high p_T . As a result, the main reason for hadron quenching observed in heavy ion collision is not energy loss, but attenuation of the produced colorless dipole in the created dense medium. The latter mechanism, calculated with the path-integral methods, explains well the observed suppression of light hadrons and elliptic flow in a wide range of energies, from the lowest energy of RHIC up to LHC, and in a wide range of transverse momenta. The values of the transport coefficient extracted from data range within 1-2 GeV^2/fm, dependent on energy, so agree well with the theoretical expectations. A parton produced with a high transverse momentum in a hard collision is regenerating its color field, intensively radiating gluons and losing energy. This process cannot last long, if it ends up with production of a leading hadron carrying the main fraction zh of the initial parton momentum. So energy conservation imposes severe constraints on the length scale of production of a single hadron with high p_T . As a result, the main reason for hadron quenching observed in heavy ion collision is not energy loss, but attenuation of the produced colorless dipole in the created dense medium. The latter mechanism, calculated with the path-integral methods, explains well the observed suppression of light hadrons and elliptic flow in a wide range of energies, from the lowest energy of RHIC up to LHC, and in a wide range of transverse momenta. The values of the transport coefficient extracted from data range within 1-2 GeV^2/fm, dependent on energy, so agree well with the theoretical expectations.
dcterms:title
Quenching of high-pT hadrons: a non-energy-loss scenario Quenching of high-pT hadrons: a non-energy-loss scenario
skos:prefLabel
Quenching of high-pT hadrons: a non-energy-loss scenario Quenching of high-pT hadrons: a non-energy-loss scenario
skos:notation
RIV/68407700:21340/14:00219198!RIV15-MSM-21340___
n3:aktivita
n5:Z n5:P
n3:aktivity
P(GA13-20841S), Z(MSM6840770039)
n3:dodaniDat
n7:2015
n3:domaciTvurceVysledku
Nemčík, Ján
n3:druhVysledku
n17:D
n3:duvernostUdaju
n4:S
n3:entitaPredkladatele
n20:predkladatel
n3:idSjednocenehoVysledku
41139
n3:idVysledku
RIV/68407700:21340/14:00219198
n3:jazykVysledku
n14:eng
n3:klicovaSlova
quenching; transport coefficient; path-integral methods; non-energy-loss scenario
n3:klicoveSlovo
n8:quenching n8:path-integral%20methods n8:non-energy-loss%20scenario n8:transport%20coefficient
n3:kontrolniKodProRIV
[FE55C9209CA6]
n3:mistoKonaniAkce
Kolymbari
n3:mistoVydani
Les Ulis Cedex A
n3:nazevZdroje
EPJ Web of Conferences
n3:obor
n18:JB
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
4
n3:projekt
n21:GA13-20841S
n3:rokUplatneniVysledku
n7:2014
n3:tvurceVysledku
Nemčík, Ján Potashnikova, I. K. Schmidt, I. Kopeliovich, B. Z.
n3:typAkce
n6:WRD
n3:wos
000342375000070
n3:zahajeniAkce
2013-08-28+02:00
n3:zamer
n22:MSM6840770039
s:issn
2101-6275
s:numberOfPages
13
n13:doi
10.1051/epjconf/20147100070
n19:hasPublisher
EDP Sciences
n15:organizacniJednotka
21340