Search results for "GLASS CONDENSATE"

showing 10 items of 65 documents

Confronting the impact parameter dependent JIMWLK evolution with HERA data

2018

The small-$x$ evolution of protons is determined from numerical solutions of the JIMWLK equations, starting from an initial condition at moderate $x$ for a finite size proton. The resulting dipole amplitude is used to calculate the total reduced cross section $\sigma_r$ and charm reduced cross section $\sigma_{rc}$, as well as diffractive vector meson production. We compare results to experimental data from HERA and discuss fundamental problems arising from the regime sensitive to non-perturbative physics. We emphasize that information on the gluonic content of the proton, gluon spatial distributions and correlations over wide ranges in $x$, which can in principle be constrained by our stud…

Physicsparton densitiesParticle physicsprotonitta114protons010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryHERAhiukkasfysiikka7. Clean energy01 natural sciencesGluonColor-glass condensateHigh Energy Physics - Phenomenology0103 physical sciencesContent (measure theory)Saturation (graph theory)High Energy Physics::ExperimentProduction (computer science)Vector mesonImpact parameter010306 general physicsNuclear ExperimentPhysical Review D
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Small-$x$ Physics in the Dipole Picture at NLO Accuracy

2018

International audience; We review recent progress in NLO calculations for dilute-dense processes in the CGC picture. In particular, we focus here on recent steps in understanding high energy renormalization group evolution (BK/JIMWLK), the total DIS cross section at small x and forward particle production in proton-nucleus collisions at next-to-leading order.

Physicssmall-xenergy: highhigher-order: 1hiukkasfysiikkaBalitsky-Kovchegov equationDipoleforward productionQuantum electrodynamicsdeep inelastic scattering[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]color glass condensatesirontarenormalization groupNuclear Experimentp nucleus: scatteringtalkdipole
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Thermalization in the initial stage of heavy ion collisions

2017

The high density non-abelian matter produced in heavy ion collisions is extremely anisotropic. Prethermal dynamics for the anisotropic and weakly coupled matter is discussed. Thermalization is realized with the effective kinetic theory in the leading order accuracy of the weakly coupled expansion. With the initial condition from color glass condensate, hydrodynamization time for the LHC energies is realized to be about 1 fm/c, while the thermalization happens much later than the hydrodynamization. peerReviewed

PhysicsthermalizationLarge Hadron Colliderta114010308 nuclear & particles physicsPhysicsQC1-999heavy ion collisionsHigh density01 natural sciences7. Clean energyColor-glass condensateNuclear physicsThermalisationChemical physics0103 physical sciencesKinetic theory of gasescolor glass condensatehydrodynamizationInitial value problemHeavy ion010306 general physicsAnisotropyQuark Confinement and the Hadron Spectrum
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Use of a running coupling in the NLO calculation of forward hadron production

2018

We address and solve a puzzle raised by a recent calculation [1] of the cross-section for particle production in proton-nucleus collisions to next-to-leading order: the numerical results show an un- reasonably large dependence upon the choice of a prescription for the QCD running coupling, which spoils the predictive power of the calculation. Specifically, the results obtained with a prescription formulated in the transverse coordinate space differ by one to two orders of magnitude from those obtained with a prescription in momentum space. We show that this discrepancy is an artefact of the interplay between the asymptotic freedom of QCD and the Fourier transform from coordinate space to mo…

Position and momentum spaceQCD EVOLUTION01 natural sciencesAsymptotic freedomquantum chromodynamics: correctionhard scatteringHigh Energy Physics - Phenomenology (hep-ph)coupling constant: energy dependencestrong interaction: coupling constantEQUATIONkvanttifysiikkaComputingMilieux_MISCELLANEOUSPhysicsQuantum chromodynamicsQUARKhigher-order: 1nuclear physicssddc:12.39.StHigh Energy Physics - Phenomenology12.38.Bxsymbolsydinfysiikkahadron: forward productionFOS: Physical sciences114 Physical sciencesRENORMALIZATION-GROUP12.38.Cysymbols.namesakeCross section (physics)Theoretical physicsquantum chromodynamics0103 physical sciencessirontarelativistic heavy-ion collisionCoordinate spacenumerical calculations010306 general physicsp nucleus: scatteringcorrection: higher-orderCouplingta114010308 nuclear & particles physics25.75.-qCOLOR GLASS CONDENSATENONLINEAR GLUON EVOLUTIONRenormalization groupFourier transformasymptotic freedom[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Production of inclusive ϒ(1S) and ϒ(2S) in p–Pb collisions at sNN=5.02 TeV

2015

We report on the production of inclusive Y{hooktop}(1S) and Y{hooktop}(2S) in p-Pb collisions at √sNN=5.02 TeV at the LHC. The measurement is performed with the ALICE detector at backward (-4.46<ycms<-2.96) and forward (2.03<ycms<3.53) rapidity down to zero transverse momentum. The production cross sections of the Y{hooktop}(1S) and Y{hooktop}(2S) are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of Y{hooktop}(1S). A suppression of the inclusive Y{hooktop}(1S) yield in p-Pb collisions with respect to the yield from pp collisions scaled by the number of binary nucleon-nucleon collisions is observed at forward rapidity but not at backwar…

Quantum chromodynamicsNuclear physicsPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderYield (chemistry)Transverse momentumBinary numberProduction (computer science)RapidityNuclear Experiment7. Clean energyColor-glass condensatePhysics Letters B
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The ridge in proton-proton collisions at the LHC

2010

We show that the key features of the CMS result on the ridge correlation seen for high multiplicity events in sqrt(s)=7TeV proton-proton collisions at the LHC can be understood in the Color Glass Condensate framework of high energy QCD. The same formalism underlies the explanation of the ridge events seen in A+A collisions at RHIC, albeit it is likely that flow effects may enhance the magnitude of the signal in the latter.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsHigh energyParticle physicsLarge Hadron ColliderNuclear Theoryta114010308 nuclear & particles physicsFOS: Physical sciencesHigh multiplicityKey features01 natural sciencesColor-glass condensateHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)Formalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentNuclear theoryPhysics Letters B
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Initial conditions of heavy ion collisions and small x

2009

The Color Glass Condensate (CGC), describing the physics of the nonlinear gluonic interactions of QCD at high energy, provides a consistent first-principles framework to understand the initial conditions of heavy ion collisions. This talk reviews some aspects of the initial conditions at RHIC and discusses implications for LHC heavy ion phenomenology. The CGC provides a way compute bulk particle production and understand recent experimental observations of long range rapidity correlations in terms of the classical glasma field in the early stages of the collision.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesCollisionColor-glass condensateNuclear physicsNonlinear systemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaRapidityNuclear ExperimentPhenomenology (particle physics)
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Diffractive dijet production and Wigner distributions from the color glass condensate

2019

Experimental processes that are sensitive to parton Wigner distributions provide a powerful tool to advance our understanding of proton structure. In this work, we compute gluon Wigner and Husimi distributions of protons within the Color Glass Condensate framework, which includes a spatially dependent McLerran-Venugopalan initial configuration and the explicit numerical solution of the JIMWLK equations. We determine the leading anisotropy of the Wigner and Husimi distributions as a function of the angle between impact parameter and transverse momentum. We study experimental signatures of these angular correlations at a proposed Electron Ion Collider by computing coherent diffractive dijet p…

QuarkCOLLISIONSprotonitNuclear TheoryHIGH-ENERGY FACTORIZATIONFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciences114 Physical sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsDEEP-INELASTIC SCATTERINGUNITARITYHigh Energy Physics - Phenomenology (hep-ph)Recoil0103 physical sciences010306 general physicsNuclear Experimentproton structureQuantum chromodynamicsPhysicsta114010308 nuclear & particles physicsQUARKNONLINEAR GLUON EVOLUTIONQCDGluonHigh Energy Physics - Phenomenologyparton Wigner distributionsEP SCATTERINGSATURATIONPHOTOPRODUCTIONcolor glass condensateImpact parameterNucleonPhysical Review D
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Color glass condensate at next-to-leading order meets HERA data

2020

We perform the first dipole picture fit to HERA inclusive cross section data using the full next-to-leading order (NLO) impact factor combined with an improved Balitsky-Kovchegov evolution including the dominant effects beyond leading logarithmic accuracy at low $x$. We find that three different formulations of the evolution equation that have been proposed in the recent literature result in a very similar description of HERA data, and robust predictions for future deep inelastic scattering experiments. We find evidence pointing towards a significant nonperturbative contribution to the structure function for light quarks, which stresses the need to extend the NLO impact factor calculation t…

QuarkParticle physicsLogarithmNuclear TheoryFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesperturbative QCDColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)HERADeep inelastic scatteringDipoleHigh Energy Physics - PhenomenologyQCD in nuclear reactionsEvolution equationHigh Energy Physics::Experimentydinfysiikka
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Ultrarelativistic quark-nucleus scattering in a light-front Hamiltonian approach

2020

We investigate the scattering of a quark on a heavy nucleus at high energies using the time-dependent basis light-front quantization (tBLFQ) formalism, which is the first application of the tBLFQ formalism in QCD. We present the real-time evolution of the quark wave function in a strong classical color field of the relativistic nucleus, described as the color glass condensate. The quark and the nucleus color field are simulated in the QCD SU(3) color space. We calculate the total and the differential cross sections, and the quark distribution in coordinate and color spaces using the tBLFQ approach. We recover the eikonal cross sections in the eikonal limit. We find that the differential cro…

QuarkParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceshiukkasfysiikka01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Quantization (physics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessironta010306 general physicsWave functionPhysicsQuantum chromodynamics010308 nuclear & particles physicsEikonal equationkvarkitHigh Energy Physics::PhenomenologyDeep inelastic scatteringHigh Energy Physics - PhenomenologysymbolskvanttikenttäteoriaHamiltonian (quantum mechanics)ydinfysiikkaPhysical Review D
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