18 research outputs found
Characterizing quark gluon plasma by dilepton interferometry
The Hanbury-Brown-Twiss (HBT) radii have been calculated from the two
particle correlation functions with virtual photons produced in the collisions
of two nuclei at ultra-relativistic energies. We show that the variation of the
HBT radii with the invariant mass of the virtual photon can be used to
characterize and distinguish the hadronic as well as the partonic phase that
might have produced initially in the collisions. It has been illustrated that
the non-monotonic variation of the HBT radii with invariant mass provides an
access to the development of collective flow in the system.Comment: Talk presented at icpaqgp 2010, Dec 6-10, 2010, Goa, Indi
Photon interferometry and size of the hot zone in relativistic heavy ion collisions
The parameters obtained from the theoretical analysis of the single photon
spectra observed by the WA98 collaboration at SPS energies have been used to
evaluate the two photon correlation functions. The single photon spectra and
the two photon correlations at RHIC energies have also been evaluated, taking
into account the effects of the possible spectral change of hadrons in a
thermal bath. We find that the ratio for SPS and
for RHIC energy.Comment: text changed, figures adde
(Anti)Proton and Pion Source Sizes and Phase Space Densities in Heavy Ion Collisions
NA44 has measured mid-rapidity deuteron spectra from AA collisions at
sqrt{s}=18GeV/A at the CERN SPS. Combining these spectra with published proton,
antiproton and antideuteron data allows us to calculate, within a coalescence
framework, proton and antiproton source sizes and phase space densities. These
results are compared to pion source sizes and densities, pA results and to
lower energy (AGS) data. The antiproton source is larger than the proton source
at sqrt{s}=18GeV/A. The phase space densities of pions and protons are not
constant but grow with system size. Both pi+ and proton radii decrease with
transverse mass and increase with sqrt{s}. Pions and protons do not freeze-out
independently. The nature of their interaction changes as sqrt{s}, and the
pion/proton ratio increases.Comment: 4 pages, Latex 2.09, 3 eps figures. Changes for January 2001. The
proton source size is now calculated assuming a more realistic Hulthen,
rather than Gaussian, wavefunction. A new figure shows the effect of this
change which is important for small radii. A second new figure shows the
results of RQMD calculations of the proton source size and phase density.
Because of correlations between position and momentum coalesence does not
show the full proton source size. The paper has been streamlined and
readability improve
Journey of a patient with chronic thromboembolic pulmonary hypertension
Right ventricle (RV) dysfunction is a key outcome determinant and a leading cause of death for patients with chronic thromboembolic pulmonary hypertension (CTEPH). In this report, we followed the 5-year clinical journey of a patient with CTEPH. The tricuspid pressure gradient was significantly increased in the early phase of CTEPH and “normalized” at the late phase of this patient’s clinical journey, but this “normalized” gradient is not a positive treatment response but rather an ominous sign of advancing right heart failure owing to an exhaustion of RV contractile function. Thus, appropriate interpretation of the tricuspid pressure gradient change is of importance for assessing RV dysfunction and treatment outcome during follow-up in patients with CTEPH. Besides systolic pulmonary artery pressure (SPAP), other RV functional parameters such as tricuspid annular plane systolic excursion, RV fractional area change, and RV longitudinal strain, together with clinical markers, may provide additional guidance regarding functional improvement or progression in patients with CTEPH
Catalytic Concentration of Alanine Aminotransferase (ALAT) Determined by IFCC Method at 37°C IRMM/IFCC-454.
Abstract not availableJRC.D-Institute for Reference Materials and Measurements (Geel
Catalytic Concentration of Lactate Dehydrogenase Isoenzyme 1 (LD1) Determined by IFCC Method at 37°C IRMM/IFCC-453.
Abstract not availableJRC.D-Institute for Reference Materials and Measurements (Geel