The pseudorapidity density of charged particles, dNch / d η , at midrapidity in Pb-Pb collisions has been measured at a center-of-mass energy per nucleon pair of √ s N N = 5.02 TeV . For the 5% ...most central collisions, we measure a value of 1943 ± 54 . The rise in dNch / d η as a function of √ s N N is steeper than that observed in proton-proton collisions and follows the trend established by measurements at lower energy. The increase of dNch / d η as a function of the average number of participant nucleons, ⟨ N part ⟩ , calculated in a Glauber model, is compared with the previous measurement at √ s N N = 2.76 TeV . A constant factor of about 1.2 describes the increase in dNch / d η from √ s N N = 2.76 to 5.02 TeV for all centrality classes, within the measured range of 0%–80% centrality. The results are also compared to models based on different mechanisms for particle production in nuclear collisions.
The multi-strange baryon yields in Pbsingle bond Pb collisions have been shown to exhibit an enhancement relative to pp reactions. In this work, Xi and Omega production rates have been measured with ...the ALICE experiment as a function of transverse momentum, p sub(T)pT, in psingle bond Pb collisions at a centre-of-mass energy of View the MathML source sNN=5.02 TeV. The results cover the kinematic ranges 0.6 GeV/c<p sub(T)<7.2 GeV/c0.6 GeV/c<pT<7.2 GeV/c and 0.8 GeV/c<p sub(T)<5 GeV/c0.8 GeV/c<pT<5 GeV/c, for Xi and Omega respectively, in the common rapidity interval -0.5<y sub(CMS)<0-0.5<yCMS<0. Multi-strange baryons have been identified by reconstructing their weak decays into charged particles. The p sub(T)pT spectra are analysed as a function of event charged-particle multiplicity, which in psingle bond Pb collisions ranges over one order of magnitude and lies between those observed in pp and Pbsingle bond Pb collisions. The measured p sub(T)pT distributions are compared to the expectations from a Blast-Wave model. The parameters which describe the production of lighter hadron species also describe the hyperon spectra in high multiplicity psingle bond Pb collisions. The yield of hyperons relative to charged pions is studied and compared with results from pp and Pbsingle bond Pb collisions. A continuous increase in the yield ratios as a function of multiplicity is observed in psingle bond Pb data, the values of which range from those measured in minimum bias pp to the ones in Pbsingle bond Pb collisions. A statistical model qualitatively describes this multiplicity dependence using a canonical suppression mechanism, in which the small volume causes a relative reduction of hadron production dependent on the strangeness content of the hyperon.
The azimuthal anisotropy coefficient v2 of prompt D0, D+, D∗+, and Ds+ mesons was measured in midcentral (30%-50% centrality class) Pb-Pb collisions at a center-of-mass energy per nucleon pair ...sNN=5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at midrapidity, |y|
Here, transverse momentum (pT) spectra of pions, kaons, and protons up to pT = 20GeV/c have been measured in Pb-Pb collisions at √sNN = 2.76TeV using the ALICE detector for six different centrality ...classes covering 0%–80%. The proton-to-pion and the kaon-to-pion ratios both show a distinct peak at pT ≈ 3GeV/c in central Pb-Pb collisions that decreases for more peripheral collisions. For pT > 10GeV/c, the nuclear modification factor is found to be the same for all three particle species in each centrality interval within systematic uncertainties of 10%–20%. This suggests there is no direct interplay between the energy loss in the medium and the particle species composition in the hard core of the quenched jet. For pT < 10GeV/c, the data provide important constraints for models aimed at describing the transition from soft to hard physics.
Invariant differential yields of deuterons and antideuterons in pp collisions at s = 0.9, 2.76 and 7 TeV and the yields of tritons, He3 nuclei, and their antinuclei at s = 7 TeV have been measured ...with the ALICE detector at the CERN Large Hadron Collider. The measurements cover a wide transverse momentum (pT) range in the rapidity interval |y|
A
bstract
The production of prompt charmed mesons D
0
, D
+
and D
∗+
, and their antiparticles, was measured with the ALICE detector in Pb-Pb collisions at the centre-of-mass energy per nucleon pair,
...s
N
N
, of 2
.
76 TeV. The production yields for rapidity |
y
|
<
0
.
5 are presented as a function of transverse momentum,
p
T
, in the interval 1–36 GeV
/c
for the centrality class 0–10% and in the interval 1–16 GeV
/c
for the centrality class 30–50%. The nuclear modification factor
R
AA
was computed using a proton-proton reference at
s
=
2.76
TeV, based on measurements at
s
=
7
TeV and on theoretical calculations. A maximum suppression by a factor of 5-6 with respect to binary-scaled pp yields is observed for the most central collisions at
p
T
of about 10 GeV
/c
. A suppression by a factor of about 2-3 persists at the highest
p
T
covered by the measurements. At low
p
T
(1-3 GeV
/c
), the
R
AA
has large uncertainties that span the range 0.35 (factor of about 3 suppression) to 1 (no suppression). In all
p
T
intervals, the
R
AA
is larger in the 30-50% centrality class compared to central collisions. The D-meson
R
AA
is also compared with that of charged pions and, at large
p
T
, charged hadrons, and with model calculations.
The first evidence of spin alignment of vector mesons ( K*0 and ϕ ) in heavy-ion collisions at the Large Hadron Collider (LHC) is reported. The spin density matrix element ρ 00 is measured at ...midrapidity ( | y | < 0.5 ) in Pb-Pb collisions at a center-of-mass energy ( √sNN ) of 2.76 TeV with the ALICE detector. ρ 00 values are found to be less than 1/3 (1/3 implies no spin alignment) at low transverse momentum ( p T < 2 GeV / c ) for K*0 and ϕ at a level of 3 σ and 2 σ , respectively. No significant spin alignment is observed for the K0S meson ( spin = 0 ) in Pb-Pb collisions and for the vector mesons in p p collisions. The measured spin alignment is unexpectedly large but qualitatively consistent with the expectation from models which attribute it to a polarization of quarks in the presence of angular momentum in heavy-ion collisions and a subsequent hadronization by the process of recombination.
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