194 research outputs found
Heavy Flavor Probes of Quark Matter
A brief survey of the role of heavy flavors as a probe of the state of matter
produced by high energy heavy ion collisions is presented. Specific examples
include energy loss, initial state gluon saturation, thermalization and flow.
The formation of quarkonium bound states from interactions in which multiple
heavy quark-antiquark pairs are initially produced is examined in general.
Results from statistical hadronization and kinetic models are summarized. New
predictions from the kinetic model for J/Psi at RHIC are presented.Comment: Based on invited plenary talk at Strange Quark Matter 2004, Cape
Town, South Africa, September 15-20, 2004, references completed, published in
J. Phys. G: Nucl. Part. Phys. 31 (2005) S641-S64
An Experimental Overview of Results Presented at SQM 2006
I have been asked to give an critical overview on the experimental results
shown in the conference with a emphasis of what has been learned and the
challenges that are ahead in trying to understand the physics of the strongly
interacting quark-gluon plasma. I will not try to summarize all of the results
presented, rather I will concentrate primarily on RHIC data from this
conference. Throughout this summary, I will periodically review some of the
previous results for those not familiar with the present state of the field.Comment: 15 pages, 12 Figure
Kaon Weak Decays in Chiral Theories
The ten nonleptonic weak decays , , , , , are predicted for a
chiral pole model based on the linear sigma model theory which automatically
satisfies the partial conservation of axial current (PCAC) hypothesis. These
predictions, agreeing with data to the 5% level and containing no or at most
one free parameter, are compared with the results of chiral perturbation theory
(ChPT). The latter ChPT approach to one-loop level is known to contain at least
four free parameters and then predicts a rate
which is 60% shy of the experimental value. This suggests that ChPT is an
unsatisfactory approach towards predicting kaon weak decays.Comment: 12 pages, 8 eps figure
production in PHENIX
Heavy quarkonia production is expected to be sensitive to the formation of a
quark gluon plasma (QGP). The PHENIX experiment has measured
production at ~200 GeV in Au+Au and Cu+Cu collisions, as well
as in reference p+p and d+Au runs. 's were measured both at mid
() and forward () rapidity. In this letter, we present
the A+A preliminary results and compare them to normal cold nuclear matter
expectations derived from PHENIX d+Au and p+p measurements as well as to
theoretical models including various effects (color screening, recombination,
sequential melting...).Comment: 5 pages, 7 figures. To appear in the proceedings of Hot Quarks 2006:
Workshop for Young Scientists on the Physics of Ultrarelativistic
Nucleus-Nucleus Collisions, Villasimius, Italy, 15-20 May 200
Radiative decays of heavy and light mesons in a quark triangle approach
The radiative meson decays and are
analyzed using the quark triangle diagram. Experimental data yield well
determined estimates of the universal quark-antiquark-meson couplings
and for the light meson sector. Also
predictions for the ratios of neutral to charged heavy meson decay coupling
constants are given and await experimental confirmation.Comment: 31 pages of RevTex, 5 figures, Postscript version available at
http://info.utas.edu.au/docs/physics/theory/Publications/9548.html, scheduled
to appear in Phys. Rev. D, vol 53, issue 11, 199
Open Charm Enhancement in Pb+Pb Collisions at SPS
The statistical coalescence model for the production of open and hidden charm
is considered within the canonical ensemble formulation. The data for the
J/\psi multiplicity in Pb+Pb collisions at 158 A GeV are used for the model
prediction of the open charm yield. We find a strong enhancement of the open
charm production, by a factor of about 2--4, over the standard hard-collision
model extrapolation from nucleon-nucleon to nucleus-nucleus collisions. A
possible mechanism of the open charm enhancement in A+A collisions at the SPS
energies is proposed.Comment: 4 pages, Late
Charmonium from Statistical Hadronization of Heavy Quarks -- a Probe for Deconfinement in the Quark-Gluon Plasma
We review the statistical hadronization picture for charmonium production in
ultra-relativistic nuclear collisions. Our starting point is a brief reminder
of the status of the thermal model description of hadron production at high
energy. Within this framework an excellent account is achieved of all data for
hadrons built of (u,d,s) valence quarks using temperature, baryo-chemical
potential and volume as thermal parameters. The large charm quark mass brings
in a new (non-thermal) scale which is explicitely taken into account by fixing
the total number of charm quarks produced in the collision. Emphasis is placed
on the description of the physical basis for the resulting statistical
hadronization model. We discuss the evidence for statistical hadronization of
charmonia by analysis of recent data from the SPS and RHIC accelerators.
Furthermore we discuss an extension of this model towards lower beam energies
and develop arguments about the prospects to observe medium modifications of
open and hidden charm hadrons. With the imminent start of the LHC accelerator
at CERN, exciting prospects for charmonium production studies at the very high
energy frontier come into reach. We present arguments that, at such energies,
charmonium production becomes a fingerprint of deconfinement: even if no
charmonia survive in the quark-gluon plasma, statistical hadronization at the
QCD phase boundary of the many tens of charm quarks expected in a single
central Pb-Pb collision could lead to an enhanced, rather than suppressed
production probability when compared to results for nucleon-nucleon reactions
scaled by the number of hard collisions in the Pb-Pb system.Comment: review article, 27 pages, Landoldt review volume "Relativistic Heavy
Ion Physics", Reinhard Stock, edito
On the Distribution of 's Produced in Heavy Ion Collisions
Thermal production of in the quark gluon plasma is reconsidered. We
show that if screening effects are not strong enough, the ``in-plasma born''
's would generate a peak in the Feynman momentum distribution at .Comment: 18 pages, RevTex, 7 eps figures. Comments, references and (2) tables
added. Results and conclusions unchanged. Accepted for publication in
Physical Review
Recent results in relativistic heavy ion collisions: from ``a new state of matter'' to "the perfect fluid"
Experimental Physics with Relativistic Heavy Ions dates from 1992 when a beam
of 197Au of energy greater than 10A GeV/c first became available at the
Alternating Gradient Synchrotron (AGS) at Brookhaven National Laboratory (BNL)
soon followed in 1994 by a 208Pb beam of 158A GeV/c at the Super Proton
Synchrotron (SPS) at CERN (European Center for Nuclear Research). Previous
pioneering measurements at the Berkeley Bevalac in the late 1970's and early
1980's were at much lower bombarding energies (~ 1 A GeV/c) where nuclear
breakup rather than particle production is the dominant inelastic process in
A+A collisions. More recently, starting in 2000, the Relativistic Heavy Ion
Collider (RHIC) at BNL has produced head-on collisions of two 100A GeV beams of
fully stripped Au ions, corresponding to nucleon-nucleon center-of-mass energy,
sqrt(sNN)=200 GeV, total c.m. energy 200A GeV. The objective of this research
program is to produce nuclear matter with extreme density and temperature,
possibly resulting in a state of matter where the quarks and gluons normally
confined inside individual nucleons (r < 1 fm) are free to act over distances
an order of magnitude larger. Progress from the period 1992 to the present will
be reviewed, with reference to previous results from light ion and
proton-proton collisions where appropriate. Emphasis will be placed on the
measurements which formed the basis for the announcements by the two major
laboratories: "A new state of matter", by CERN on Feb 10, 2000 and "The perfect
fluid", by BNL on April 19, 2005.Comment: 62 pages, 39 figures. Review article published in Reports on Progress
in Physics on June 23, 2006. In this published version, mistakes,
typographical errors, and citations have been corrected and a subsection has
been adde
Chiral Lagrangians for Radiative Decays of Heavy Hadrons
The radiative decays of heavy mesons and heavy baryons are studied in a
formalism which incorporates both the heavy quark symmetry and the chiral
symmetry. The chiral Lagrangians for the electromagnetic interactions of heavy
hadrons consist of two pieces: one from gauging electromagnetically the
strong-interaction chiral Lagrangian, and the other from the anomalous magnetic
moment interactions of the heavy baryons and mesons. Due to the heavy quark
spin symmetry, the latter contains only one independent coupling constant in
the meson sector and two in the baryon sector. These coupling constants only
depend on the light quarks and can be calculated in the nonrelativistic quark
model. However, the charm quark is not heavy enough and the contribution from
its magnetic moment must be included. Applications to the radiative decays
and are given. Together with our previous results
on the strong decay rates of and , predictions are obtained for the total widths and
branching ratios of and . The decays and are discussed to illustrate the important roles played by both the heavy
quark symmetry and the chiral symmetry.Comment: 30 pages (one figure, available on request), CLNS 92/1158 and
IP-ASTP-13-9
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