Search results for "dynamiikka"

showing 10 items of 232 documents

Signatures of gluon saturation from structure-function measurements

2022

We study experimentally observable signals for nonlinear QCD dynamics in deep inelastic scattering (DIS) at small Bjorken variable $x$ and moderate virtuality $Q^2$, by quantifying differences between the linear Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) evolution and nonlinear evolution with the Balitsky-Kovchegov (BK) equation. To remove the effect of the parametrization freedom in the initial conditions of both equations, we first match the predictions for the DIS structure functions $F_2$ and $F_{\rm L}$ from both frameworks in a region in $x,Q^2$ where both frameworks should provide an accurate description of the relevant physics. The differences in the dynamics are then quanti…

Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::Experimentkvanttiväridynamiikkahiukkasfysiikka114 Physical sciences
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Flow correlations from a hydrodynamics model with dynamical freeze-out and initial conditions based on perturbative QCD and saturation

2022

We extend the applicability of the hydrodynamics, perturbative QCD and saturation -based EKRT (Eskola-Kajantie-Ruuskanen-Tuominen) framework for ultrarelativistic heavy-ion collisions to peripheral collisions by introducing dynamical freeze-out conditions. As a new ingredient compared to the previous EKRT computations we also introduce a non-zero bulk viscosity. We compute various hadronic observables and flow correlations, including normalized symmetric cumulants, mixed harmonic cumulants and flow-transverse momentum correlations, and compare them against measurements from the BNL Relativistic Heavy Ion Collider (RHIC) and the CERN Large Hadron Collider (LHC). We demonstrate that the inclu…

Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear Theorykvarkki-gluoniplasmaFOS: Physical scienceskvanttiväridynamiikkahiukkasfysiikkaNuclear Experiment114 Physical sciences
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Light-front wavefunctions of mesons by design

2022

AbstractWe develop a mechanism to build the light-front wavefunctions (LFWFs) of meson bound states on a small-sized basis function representation. Unlike in a standard Hamiltonian formalism, the Hamiltonian in this method is implicit, and the information of the system is carried directly by the functional form and adjustable parameters of the LFWFs. In this work, we model the LFWFs for four charmonium states, $$\eta _c$$ η c , $$J/\psi $$ J / ψ , $$\psi '$$ ψ ′ , and $$\psi (3770)$$ ψ ( 3770 ) as superpositions of orthonormal basis functions. We choose the basis functions as eigenfunctions of an effective Hamiltonian, which has a longitudinal confining potential in addition to the transver…

Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentkvanttiväridynamiikkahiukkasfysiikkaEngineering (miscellaneous)114 Physical sciences
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The importance of kinematic twists and genuine saturation effects in dijet production at the Electron-Ion Collider

2021

We compute the differential yield for quark anti-quark dijet production in high-energy electron-proton and electron-nucleus collisions at small $x$ as a function of the relative momentum $\boldsymbol{P}_\perp$ and momentum imbalance $\boldsymbol{k}_\perp$ of the dijet system for different photon virtualities $Q^2$, and study the elliptic and quadrangular anisotropies in the relative angle between $\boldsymbol{P}_\perp$ and $\boldsymbol{k}_\perp$. We review and extend the analysis in [1], which compared the results of the Color Glass Condensate (CGC) with those obtained using the transverse momentum dependent (TMD) framework. In particular, we include in our comparison the improved TMD (ITMD…

Nuclear Theoryquark antiquarkQC770-798hiukkasfysiikkaPROTONtransverse momentum dependence01 natural scienceslaw.inventionColor-glass condensateGLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)lawEQUATIONSaturation (graph theory)Wave functionPhysicselectron nucleon: colliding beamsQUARK PAIR PRODUCTIONFLUCTUATIONSQCD PhenomenologyQCD phenomenologyHigh Energy Physics - PhenomenologykinematicstwistPhysics::Space PhysicsProduction (computer science)Quarkdijet: productionCOLLISIONSNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesanisotropy114 Physical sciencesdihadron: angular correlationdeep inelastic scattering (phenomenology)AZIMUTHAL CORRELATIONSMomentumelectron p: scatteringNuclear Theory (nucl-th)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesWAVE-FUNCTIONS010306 general physicsColliderDeep Inelastic Scattering (Phenomenology)010308 nuclear & particles physicselectron nucleus: scatteringHigh Energy Physics::PhenomenologyEVOLUTIONGluon[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]gluon: saturationcolor glass condensateHigh Energy Physics::ExperimentkvanttiväridynamiikkaJournal of High Energy Physics
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Prompt and non-prompt J/ψ production cross sections at midrapidity in proton-proton collisions at √s = 5.02 and 13 TeV

2022

The production of J/ψ is measured at midrapidity (|y| < 0.9) in proton-proton collisions at √s = 5.02 and 13 TeV, through the dielectron decay channel, using the ALICE detector at the Large Hadron Collider. The data sets used for the analyses correspond to integrated luminosities of Lint = 19.4 ± 0.4 nb−1 and Lint = 32.2 ± 0.5 nb−1 at √s = 5.02 and 13 TeV, respectively. The fraction of non-prompt J/ψ mesons, i.e. those originating from the decay of beauty hadrons, is measured down to a transverse momentum pT = 2 GeV/c (1 GeV/c) at √s = 5.02 TeV (13 TeV). The pT and rapidity (y) differential cross sections, as well as the corresponding values integrated over pT and y, are carried out separat…

Nuclear and High Energy PhysicsHadron-Hadron ScatteringAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentkvanttiväridynamiikkahiukkasfysiikkaNuclear Experiment
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New constraints for QCD matter from improved Bayesian parameter estimation in heavy-ion collisions at LHC

2021

The transport properties of quark-gluon plasma created in relativistic heavy-ion collisions are quantified by an improved global Bayesian analysis using the CERN Large Hadron Collider Pb–Pb data at sNN=2.76 and 5.02 TeV. The results show that the uncertainty of the extracted transport coefficients is significantly reduced by including new sophisticated collective flow observables from two collision energies for the first time. This work reveals the stronger temperature dependence of specific shear viscosity, a lower value of specific bulk viscosity, and a higher hadronization switching temperature than in the previous studies. The sensitivity analysis confirms that the precision measurement…

Nuclear and High Energy PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)kvarkki-gluoniplasmaFOS: Physical sciencesHigh Energy Physics::Experimentkvanttiväridynamiikkahep-phhiukkasfysiikkaNuclear Experiment114 Physical sciencesParticle Physics - PhenomenologyPhysics Letters
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Production of muons from heavy-flavour hadron decays at high transverse momentum in Pb–Pb collisions at √sNN = 5.02 and 2.76 TeV

2021

Measurements of the production of muons from heavy-flavour hadron decays in Pb–Pb collisions at √sNN=5.02 and 2.76 TeV using the ALICE detector at the LHC are reported. The nuclear modification factor RAA at √sNN=5.02 TeV is measured at forward rapidity (2.57 GeV/c). The RAA shows an increase of the suppression of the yields of muons from heavy-flavour hadron decays with increasing centrality. A suppression by a factor of about three is observed in the 10% most central collisions. The RAA at √sNN=5.02 TeV is similar to that at √sNN=2.76 TeV. The precise RAA measurements have the potential to distinguish between model predictions implementing different mechanisms of parton energy loss in the…

Nuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentkvanttiväridynamiikkahiukkasfysiikkaNuclear Experiment
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Complete calculation of exclusive heavy vector meson production at next-to-leading order in the dipole picture

2022

Exclusive production of transversely polarized heavy vector mesons in deep inelastic scattering at high energy is calculated at next-to-leading order accuracy in the Color Glass Condensate framework. In addition to the first QCD correction proportional to the strong coupling constant $\alpha_s$, we systematically also include the first relativistic correction proportional to the heavy quark velocity squared $v^2$. When combined with our previously published results for longitudinal vector meson production at next-to-leading order accuracy, these results make phenomenological calculations of heavy vector meson production possible at the order $\mathcal{O}(\alpha_s v^0, \alpha_s^0 v^2)$. When…

Nuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical scienceshiukkasfysiikka114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenologydeep inelastic scattering or small-x physicsHigh Energy Physics - Phenomenology (hep-ph)higher-order perturbative calculationskvanttiväridynamiikkaHigh Energy Physics::Experimentquarkonium
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Theory overview of Heavy Ion collisions

2016

This presentation discusses some recently active topics in the theoretical interpretation of high energy heavy ion collisions at the LHC and at RHIC. We argue that the standard paradigm for understanding the spacetime evolution of the bulk of the matter produced in the collision is provided by viscous relativistic hydrodynamics, which can be used to systematically extract properties of the QCD medium from experimental results. The initial conditions of this hydrodynamical evolution are increasingly well understood in terms of gluon saturation, and can be quantified using Classical Yang-Mills fields and QCD effective kinetic theory. Hard and electromagnetic probes of the plasma provide addit…

Particle physicsNuclear Theorynucleus nucleusNuclear TheoryFOS: Physical sciencesNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)quantum chromodynamicsboundary conditionsYang-Millsheavy ionsNuclear ExperimentBrookhaven RHIC CollplasmaQuantum chromodynamicsPhysicsenergiaLarge Hadron ColliderSpacetimesaturationscatteringviskositeettiPlasmaCollisionGluonHigh Energy Physics - Phenomenologyelectromagneticsspace-timekineticsQuark–gluon plasmaKinetic theory of gasesp nucleushydrodynamiikka
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Distribution and dynamics of transcription-associated proteins during parvovirus infection.

2012

Canine parvovirus (CPV) infection leads to reorganization of nuclear proteinaceous subcompartments. Our studies showed that virus infection causes a time-dependent increase in the amount of viral nonstructural protein NS1 mRNA. Fluorescence recovery after photobleaching showed that the recovery kinetics of nuclear transcription-associated proteins, TATA binding protein (TBP), transcription factor IIB (TFIIB), and poly(A) binding protein nuclear 1 (PABPN1) were different in infected and noninfected cells, pointing to virus-induced alterations in binding dynamics of these proteins. peerReviewed

Parvovirus transkriptioproteiinitvirusesdynamiikka
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