0000000000264498

AUTHOR

Hannu Holopainen

showing 15 related works from this author

Monte Carlo Simulation for Elastic Energy Loss of Hard Partons in a Hydrodynamical Background

2011

We have developed a Monte Carlo simulation describing the $2 \rightarrow 2$ scatterings of perturbatively produced, non-eikonally propagating high-energy partons with the quarks and gluons of the expanding QCD medium created in ultrarelativistic heavy ion collisions. The partonic scattering rates are computed in leading-order perturbative QCD (pQCD), while three different hydrodynamical scenarios are used to model the strongly interacting medium. We compare our results and tune the model with the neutral pion suppression observed in $\sqrt{s_{NN}}=200$ GeV Au+Au collisions at the BNL-RHIC. We find the incoherent nature of elastic energy loss incompatible with the measured angular dependence…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScatteringMonte Carlo methodNuclear TheoryHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesPartonHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment
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Energy loss in a fluctuating hydrodynamical background

2011

Recently it has become apparent that event-by-event fluctuations in the initial state of hydrodynamical modelling of ultrarelativistic heavy-ion collisions are crucial in order to understand the full centrality dependence of the elliptic flow coefficient v_2. In particular, in central collisions the density fluctuations play a major role in generating the spatial eccentricity in the initial state. This raises the question to what degree high P_T physics, in particular leading-parton energy loss, which takes place in the background of an evolving medium, is sensitive to the presence of the event-by-event density fluctuations in the background. In this work, we report results for the effects …

PhysicsNuclear and High Energy PhysicsParticle physicsta114Degree (graph theory)010308 nuclear & particles physicsPlane (geometry)Elliptic flowOrder (ring theory)FOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transfer010306 general physicsRelativistic Heavy Ion ColliderEccentricity (mathematics)Nuclear ExperimentEvent (particle physics)
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Initial state anisotropies and their uncertainties in ultrarelativistic heavy-ion collisions from the Monte Carlo Glauber model

2011

In hydrodynamical modeling of heavy-ion collisions, the initial-state spatial anisotropies are translated into momentum anisotropies of the final-state particle distributions. Thus, understanding the origin of the initial-state anisotropies and their uncertainties is important before extracting specific QCD matter properties, such as viscosity, from the experimental data. In this work we review the wounded nucleon approach based on the Monte Carlo Glauber model, charting in particular the uncertainties arising from modeling of the nucleon-nucleon interactions between the colliding nucleon pairs and nucleon-nucleon correlations inside the colliding nuclei. We discuss the differences between …

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)Nuclear Theoryta114010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)MomentumNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuark–gluon plasma010306 general physicsNucleonAnisotropyNuclear ExperimentGlauberQCD matterPhysical review C
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Event-by-event hydrodynamics and thermal photon production in ultrarelativistic heavy ion collisions

2011

ydintörmäysfotonitfluktuaatiothydrodynamiikkaalkeishiukkasetultrarelativistic heavy-ion collisions theory
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Elliptic flow from event-by-event hydrodynamics with fluctuating initial state

2011

We develop an event-by-event ideal hydrodynamical framework where initial state density fluctuations are present and where we use a similar flow-analysis method as in the experiments to make a one-to-one $v_2$ comparison with the measured data. Our studies also show that the participant plane is quite a good approximation for the event plane.

PhysicsNuclear and High Energy PhysicsIdeal (set theory)Nuclear Theoryta114010308 nuclear & particles physicsPlane (geometry)Event (relativity)Elliptic flowFOS: Physical sciencesState (functional analysis)01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)State density0103 physical sciencesStatistical physics010306 general physicsNuclear theory
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A systematic comparison of jet quenching in different fluid-dynamical models

2010

Comparing four different (ideal and viscous) hydrodynamic models for the evolution of the medium created in 200 AGeV Au-Au collisions, combined with two different models for the path length dependence of parton energy loss, we study the effects of jet quenching on the emission-angle dependence of the nuclear suppression factor R_AA(phi) and the away-side per trigger yield I_AA(phi). Each hydrodynamic model was tuned to provide a reasonable description of the single-particle transverse momentum spectra for all collision centralities, and the energy loss models were adjusted to yield the same pion nuclear suppression factor in central Au-Au collisions. We find that the experimentally measured…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonta114010308 nuclear & particles physicsHadronElliptic flowFOS: Physical sciencesElementary particleParton01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsJet quenchingBosonPhysical Review C
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Viskositeetti ja poikittaisvirtaus raskasionitörmäysten hydrodynamiikassa

2008

hiukkasfysiikkahyrodynamiikka
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Event-by-event hydrodynamics and elliptic flow from fluctuating initial states

2010

We develop a framework for event-by-event ideal hydrodynamics to study the differential elliptic flow which is measured at different centralities in Au+Au collisions at Relativistic Heavy Ion Collider (RHIC). Fluctuating initial energy density profiles, which here are the event-by-event analogues of the eWN profiles, are created using a Monte Carlo Glauber model. Using the same event plane method for obtaining $v_2$ as in the data analysis, we can reproduce both the measured centrality dependence and the $p_T$ shape of charged-particle elliptic flow up to $p_T\sim2$~GeV. We also consider the relation of elliptic flow to the initial state eccentricity using different reference planes, and di…

PhysicsNuclear and High Energy Physicsta114Nuclear TheoryMonte Carlo methodElliptic flowFOS: Physical sciencesFluid mechanicsElementary particleComputational physicsNuclear Theory (nucl-th)Nuclear physicsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentNucleonRelativistic Heavy Ion ColliderGlauberPhysical Review C
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Centrality and initial formation time dependence of the emission of thermal photons from fluctuating initial conditions at RHIC and LHC

2013

Abstract Event-by-event fluctuating initial conditions (IC) in the ideal hydrodynamic calculation are known to enhance the production of thermal photons significantly compared to a smooth initial state averaged profile in the range p T > 1 GeV / c for 200A GeV Au+Au collisions at RHIC and 2.76A TeV Pb + Pb collisions at LHC. The ‘hotspots’ or the over-dense regions in the fluctuating IC produce more high p T photons compared to the smooth IC due to the strong temperature dependent emission of the thermal radiation. This enhancement is expected to be more pronounced for peripheral collisions, for lower beam energies, and for larger values of plasma formation time. A suitably normalized ratio…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Large Hadron ColliderPhotonta114010308 nuclear & particles physics01 natural sciences7. Clean energyNuclear physicsThermal radiationYield (chemistry)0103 physical sciencesThermalBoundary value problemAtomic physicsNuclear Experiment010306 general physicsBeam (structure)Nuclear Physics A
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Collision centrality andτ0dependence of the emission of thermal photons from a fluctuating initial state in an ideal hydrodynamic calculation

2012

Fluctuations in the initial QCD matter density distribution are found to enhance the production of thermal photons significantly in the range $2\ensuremath{\leqslant}{p}_{T}\ensuremath{\leqslant}4$ GeV/$c$ compared to a smooth initial state averaged profile in ideal hydrodynamic calculation for $200A$ GeV Au+Au collisions at the Relativistic Heavy Ion Collider (RHIC) and $2.76A$ TeV Pb+Pb collisions at the Large Hadron Collider (LHC). The thermal emission of photons is strongly dependent on the initial temperature of the system where the presence of ``hot spots'' in the initial state translates into enhanced production of photons compared to a smooth profile. The effect of fluctuations in t…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsRange (particle radiation)Photon010308 nuclear & particles physicsPlasma01 natural sciencesSpectral lineNuclear physics0103 physical sciencesProduction (computer science)Atomic physicsNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderQCD matterPhysical Review C
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Enhancement of thermal photon production in event-by-event hydrodynamics

2011

Thermal photon emission is widely believed to reflect properties of the earliest, hottest evolution stage of the medium created in ultra-relativistic heavy-ion collisions. Previous computations of photon emission have been carried out using a hydrodynamical medium description with smooth, averaged initial conditions. Recently, more sophisticated hydrodynamical models which calculate observables by averaging over many evolutions with event-by-event fluctuating initial conditions (IC) have been developed. Given their direct connection to the early time dynamics, thermal photon emission appears an ideal observable to probe fluctuations in the medium initial state. In this work, we demonstrate …

PhysicsNuclear and High Energy PhysicsPhotonPhoton antibunchingta114010308 nuclear & particles physicsFOS: Physical sciencesElementary particleMonte Carlo method for photon transportObservable01 natural sciences7. Clean energyNuclear physicsMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesThermal010306 general physicsEvent (particle physics)
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Elliptic flow from event-by-event hydrodynamics

2011

We present an event-by-event hydrodynamical framework which takes into account the initial density fluctuations arising from a Monte Carlo Glauber model. The elliptic flow is calculated with the event plane method and a one-to-one comparison with the measured event plane $v_2$ is made. Both the centrality- and $p_T$-dependence of the $v_2$ are remarkably well reproduced. We also find that the participant plane is a quite good approximation for the event plane.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsPlane (geometry)Event (relativity)Monte Carlo methodElliptic flowFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStatistical physics010306 general physicsNuclear ExperimentGlauber
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Thermal photons from fluctuating initial conditions

2011

Event-by-event fluctuations of initial QCD-matter density produced in heavy-ion collisions at RHIC enhance the production of thermal photons significantly in the region $2 \le p_T \le 4$ GeV/$c$ compared to a smooth initial-state averaged profile in the ideal hydrodynamic calculation. This enhancement is a an early time effect due to the presence of hotspots or over-dense regions in the fluctuating initial state. The effect of fluctuations is found to be stronger in peripheral than in central collisions.

Time effectPhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesThermalAtomic physicsNuclear Experiment010306 general physicsJournal of Physics G: Nuclear and Particle Physics
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Influence of initial state fluctuations on the production of thermal photons

2012

Inhomogeneities in the initial QCD matter density distribution increase the production of thermal photons significantly compared to a smooth initial-state-averaged profile in the region $p_T > 1$ GeV/$c$ in an ideal hydrodynamic calculation. This relative enhancement is more pronounced for peripheral collisions, for smaller size systems as well as for lower beam energies. A suitably normalized ratio of central-to-peripheral yield of thermal photons reduce the uncertainties in the hydrodynamical initial conditions and can be a useful parameter to study the density fluctuations and their size. The fluctuations in the initial density distribution also lead to a larger elliptic flow of therm…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsPhotonta114Nuclear Theory010308 nuclear & particles physicsHadronElliptic flowFOS: Physical sciences01 natural sciences7. Clean energySpectral lineNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNucleonNuclear ExperimentGlauberQCD matter
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Systematics of parton-medium interaction from RHIC to LHC

2011

Despite a wealth of experimental data for high-P_T processes in heavy-ion collisions, discriminating between different models of hard parton-medium interactions has been difficult. A key reason is that the pQCD parton spectrum at RHIC is falling so steeply that distinguishing even a moderate shift in parton energy from complete parton absorption is essentially impossible. In essence, energy loss models are effectively only probed in the vicinity of zero energy loss and, as a result, at RHIC energies only the pathlength dependence of energy loss offers some discriminating power. At LHC however, this is no longer the case: Due to the much flatter shape of the parton p_T spectra originating fr…

PhysicsNuclear and High Energy PhysicsEnergy lossLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesZero-point energyParton01 natural sciencesSpectral lineModel dynamicsNuclear physicsStrange matterHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsAbsorption (electromagnetic radiation)Nuclear Experiment
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