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E. V. Shuryak

Publications and source records attributed to E. V. Shuryak.

At least 55 records · Page 3Linked to original sources

Resolving the Antibaryon-Production Puzzle in High-Energy Heavy-Ion Collisions

We argue that the observed antiproton production in heavy-ion collisions at CERN-SpS energies can be understood if (contrary to most sequential scattering approaches) the backward direction in the process $p\bar p \leftrightarrow \bar{n}π$ (with $\bar{n}$=5-6) is consistently accounted for within a thermal framework. Employing the standard picture of subsequent chemical and thermal freezeout, which induces an over-saturation of pion number with associated chemical potentials of $μ_π\simeq$~60-80 MeV, enhances the backward reaction substantially. The resulting rates and corresponding cross sections turn out to be large enough to maintain the abundance of antiprotons at chemical freezeout until the decoupling temperature, in accord with the measured $\bar{p}/p$ ratio in Pb(158AGeV)+Pb collisions.

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Are High Energy Heavy Ion Collisions similar to a Little Bang, or just a very nice Firework?

The talk is a brief overview of what we recently learned about excited hadronic matter from heavy ion collisions. The central issue is that the systems produced do exhibit macroscopic behavior, it flows and we start getting some idea about its effective Equation of State (EoS). More specifically, we concentrate on elliptic flow, from SPS to RHIC energies, as well as on particle composition and fluctuations. Note that a pressure and the rate of fluctuation relaxation (discussed at the end) are ultimately a measure of a collision rate in the system we would like to understand.

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Toward the non-perturbative description of high energy processes

General implications of existence of non-perturbative scales and hadronic sub-structure for high energy processes are discussed. We propose that the dependence of the cross section of $\bar q q$ dipoles on their size d should deviate from $d^2$ when d becomes comparable to substructure scale. Then we discuss Kharzeev-Levin pomeron model \cite{KL}, based on ladder-type diagrams with $scalar$ resonances (scalar $ππ$ or $σ$ and the scalar glueball $G_0$). This channel is truly unique, because instanton-induced attractive gg interaction \cite{Shu_82} leads to unusually small sizes and strong coupling constants of these states, supplemented by unusually large mass scale, $M_0\approx 4 GeV$, of the transition boundary to the perturbative regime. As pomeron is a small-size object by itself, these resonances may play a special role in its dynamics. Furthermore, we use more realistic description of the scalar gluonic spectral density without free parameters, and slightly modify the model to get correct chiral limit. We conclude that the non-perturbative part of the scalar contribution to the soft pomeron intercept is $Δ= >.05\pm 0.015$, with comparable contributions from both $σ$ and $G_0$.

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Scales and Phases of Non-Perturbative QCD

This is a short write-up of lectures at UK Theory Institute, Swansea UK, Sept.99; and XVII School ``QCD: Perturbative or Non-perturbative?'' Lisbon,Portugal, Oct.99. The covered topic include (i) discussion of the scales at which perturbative description should be changed by the non-perturbative one. A number of various examples are considered, leading to different scales, related to instantons or confinement effects; (ii) Instanton vacuum as an Instanton Liquid; (iii) The phase diagram of QCD at finite temperature and density, and especially description of a recent progress in Color Superconductivity.

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Probing the Boundary of the Non-Perturbative QCD by Small Size Instantons

The lattice data on the instanton size distribution suggest an additional O($ρ^2)$ action. The small-$ρ$ effect O($ρ^4)$ predicted by the Operator Product Expansion (OPE) is not observed. Similar deviations are also found for non-perturbative response to a small static color dipoles: it is O(r) not O(r$^2$). We suggest that small instanton radii in the QCD vacuum and small radii of the QCD strings (to which this observation relates) are consequences of the same phenomenon: a very robust dual superconductivity in the QCD vacuum, with relatively large Higgs VEV and surprisingly large Higgs mass.

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On the Origin of the Multiplicity Fluctuations in High Energy Heavy Ion Collisions

Multiplicity fluctuations in heavy ion collisions obtain comparable contributions both from initial stage of the collisions, and from final stage interaction. We calculate the former component, using the ``wounded nucleon'' model and standard assumptions about nuclei and NN cross section. Combining it with the second one, calculated previously by Stephanov,Rajagopal and Shuryak, ref.2, we obtain good quantitative description of experimental data (ref.3) from NA49 collaboration at CERN on central PbPb collisions.

nucl-th↗

High Density QCD and Instantons

Instantons generate strong non-perturbative interactions between quarks. In the vacuum, these interactions lead to chiral symmetry breaking and generate constituent quark masses on the order of 300-400 MeV. The observation that the same forces also provide attraction in the scalar diquark channel leads to the prediction that cold quark matter is a color superconductor, with gaps as large as $\sim$~100 MeV. We provide a systematic treatment of color superconductivity in the instanton model. We show that the structure of the superconductor depends on the number of flavors. In the case of two flavors, we verify the standard scenario and provide an improved calculation of the mass gap. For three flavors, we show that the ground state is color-flavor locked and calculate the chiral condensate in the high density phase. We show that as a function of the strange quark mass, there is a sharp transition between the two phases. Finally, we go beyond the mean field approximation and investigate the role of instanton-anti-instanton molecules, which -- besides superconducting gap formation -- provide a competitive mechanism for chiral restoration at finite density.

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An unusual space-time evolution for heavy ion collisions at high energies due to the QCD phase transition

The space-time evolution of high energy non-central heavy ion collisions is studied with relativistic hydrodynamics. The results are very sensitive to the Equation of State(EoS). For an EoS with the QCD phase transition, an unusual matter distribution develops. Before freeze-out, two shells are formed which then physically separate and leave a maximum in the center. We make specific predictions for the azimuthal dependence of the flow and for two-pion interferometry, contrasting our results with a resonance gas EoS.

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What have we learned and want to learn from heavy ion collisions at CERN SPS?

The talk is a mini-review of the current status of the field, with emphasis on SPS heavy ion program, now and beyond 2000 (as asked by the organizers). The main question is, of course, whether we can convince ourselves and the community at large that the QGP is in fact produced at SPS. We came a long way toward the positive answer, and are definitely on strongly rising part of the learning curve. Still, in few key directions we lack important pieces of evidences.

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High energy collisions of strongly deformed nuclei: An old idea with a new twist

UU collisions can provide about 30% larger densities compared to central PbPb ones. New aspect is generation of rather deformed initial states. We show that those can be effectively used to resolve a number of outstanding issues, from corrections to hard processes, elliptic flow (the QGP push issue), and the mechanism of $J/ψ$ suppression. UU collisions are studied by a simple Monte-Carlo model, and it is shown how selecting two control parameters - the number of participant nuclei and deformation - one can select particular geometry of the collision.

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New phases of QCD, the tricritical point, and RHIC as a ``nutcracker''

Because too many interesting things are going on now, I have tried to squeeze three different subjects into one talk. The first is a brief summary of the color super-conductivity. During the last year we learned that instanton-induced forces can not only break chiral symmetry in the QCD vacuum, but also create correlated scalar diquarks and form new phases,some similar to the Higgs phase of the Standard model. The second issue I discuss is the remnant of the so called $tricritical$ point, which in QCD with physical masses is the endpoint of the first order transition. I will argue that exchange of sigmas (which are massless at this point even with quark masses included) create interesting event-by-event fluctuations, which can be used to locate it. Finally I describe first results on $flow$ calculations for non-central collisions at RHIC. It was found that it is extremely sensitive to Equation of State (EOS). Furthermore, the unusual ``nutcracker'' picture emerges for lattice-motivated EOS, which is formation of two $shells$ which are physically separated $before$ the freeze-out.

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The problem of Chiral Restoration and Dilepton Production in Heavy Ion Collisions

In the lecture we review several issues related to recent development in non-perturbative QCD. The ``instanton liquid model'' reproduces not only the basic vacuum parameters (the condensates), but even hadronic correlators. New information obtained from lattice simulations also confirm it. Meanwhile the model itself was developed into a self-consistent approach, allowing to include 't Hooft interaction to all orders. It was also generalized to non-zero temperatures and high densities. We discuss one issue, displayed by behavior of the pion and rho correlation functions: the former has strong non-perturbative effects at small distances, the latter has none. What happens at $T\sim T_c$ can be answered by dilepton production experiments with heavy ion collisions. The results definitely indicate large changes in spectral density and "melting" of the rho meson peak, possibly reaching the rate corresponding to complete chiral restoration.

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QCD phases at high density and instantons

The talk is an introduction into diquark condensation phenomena which occur in QCD at high energy density. They are driven by instantons and instanton-antiinstanton pairs (or ``molecules''), which generate attraction in some qq channels. A number of phases is possible, with or without restoration of chiral symmetry: the work is not finished and we do not yet know which take place in real QCD. We also emphasize that specific diquark correlations play a significant role in baryon structure, in particular making that of a nucleon very different of a $Δ$ (or other member of a decuplet). This ``small $N_c$'' scenario based on comparison to QCD with two colors is contrasted with the ``large $N_c$'' one.

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Equation of State, Flow, Fluctuations and $J/ψ$ suppression

Radial flow observed at AGS/SPS energies is very strong, with collective velocities of matter reaching about 0.5c for central collisions of the heaviest ions. The lattice-based Equation of State (EOS) is however rather soft, due to the QCD phase transition. We show that both statements are consistent only if proper kinetic-based treatment of the freeze-out is made. In fact chemical and thermal freeze-out happen at quite different conditions, especially at SPS. Event-by-event fluctuations can shed new light on this problem. We also propose new model of "anomalous" $J/ψ$ suppression found for PbPb collisions, related it to prolonged lifetime of dense matter due the "softest point" of the EOS.

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Diquark Bose Condensates in High Density Matter and Instantons

Instantons lead to strong correlations between up and down quarks with spin zero and anti-symmetric color wave functions. In cold and dense matter, $n_b>n_c\simeq 1 fm^{-3}$ and $T $ condensate and restoring chiral symmetry. At high density, the ground state is a color superconductor in which diquarks play the role of Cooper pairs. An interesting toy model is provided by QCD with two colors: it has a particle-anti-particle symmetry which relates $<\bar qq>$ and $< qq>$ condensates.

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Event-by-event analysis of heavy ion collisions and thermodynamical fluctuations

The event-by-event analysis of heavy ions collisions is becoming possible with advent of large acceptance detectors: it can provide dynamical information which cannot be obtained from inclusive spectra. We identify some observables which can be related to standard thermodynamical fluctuations and therefore may provide information about properties of hadronic matter at the freeze-out stage. Among those are fluctuations of ``apparent temperature'' (the $p_t$ slope), as well as the population of different bins of the pion momentum distribution.

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The gluon/charm content of the eta' meson and instantons

Motivated by recent CLEO measurements of the B-->η' K decay, we evaluate gluon/charm content of the eta' meson using the interacting instanton liquid model of the QCD vacuum. Our result is very large due to the strong field of small-size instantons. We show that it provides quantitative explanations of the CLEO data on the B-->η' K decay rate (as well as inclusive process B-->η' X), via a virtual Cabbibo-unsuppressed decay into \bar c c pair which then becomes eta'. If so, a significant charm component should be present in other hadrons also. In particular, we found a large contribution of the charmed quark in the polarised deep-inelastic scattering on a proton.

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