3,257 research outputs found
Spectra and nuclear modification factor of charged hadrons produced in lead-lead collisions at sqrt(s_NN)=2.76TeV with the ATLAS detector at the LHC
The measurement of charged particle spectra in heavy ion collisions is a way
to study properties of hot and dense matter created in these interactions. The
centrality dependence of the spectral shape is an important tool to understand
the energy loss mechanism. The ATLAS detector at the LHC accumulated integrated
luminosity equal to 0.15nb^{-1} of lead-lead data at 2.76TeV per
nucleon-nucleon pair. Due to the excellent capabilities of the ATLAS detector,
and its stable operation in 2010 and 2011 heavy ion physics runs, these data
allow measurements of the charged particle spectra and their ratios in
different centrality bins over a wide range of transverse momenta (0.5-150GeV)
and pseudorapidity (|eta|<2.5). The measured ratio central to peripheral events
shows a suppresion by a factor of 5 at pT=7GeV. At higher pT the ratio
increases
Measurement of the nuclear modification factor for high- charged hadrons in +Pb collisions with the ATLAS detector
The charged hadron spectra in +Pb and collisions at
TeV are measured with the ATLAS experiment at the
LHC. The measurements are performed with +Pb data recorded in 2013 with an
integrated luminosity of 25nb and data recorded in 2015 with an
integrated luminosity of 28pb. The +Pb results are compared to
spectra, presented as a ratio of transverse momentum distributions in the two
systems scaled by the number of binary nucleon-nucleon collisions, the nuclear
modification factor . The study of allows a
detailed comparison of the collision systems in different centrality intervals
and in a wide range of transverse momentum. It is shown that the nuclear
modification factor does not have any significant deviation from unity in the
high transverse momentum region.Comment: 4 pages, 4 figures, presented at Hard Probes 201
Effect of radiation-like solid on CMB anisotropies
We compute the power in the lowest multipoles of CMB anisotropies in the
presence of radiation-like solid, a hypothetical new kind of radiation with
nonzero shear modulus. If only the ordinary Sachs-Wolfe effect is taken into
account, the shear modulus to energy density ratio must be in absolute value of
order or less for the theory to be consistent with observations
within cosmic variance. With the integrated Sachs-Wolfe effect switched on, the
constraint is relaxed almost by two orders of magnitude.Comment: 24 pages, 3 figure
Euclidean action for vacuum decay in a de Sitter universe
The behavior of the action of the instantons describing vacuum decay in a de
Sitter is investigated. For a near-to-limit instanton (a Coleman-de Luccia
instanton close to some Hawking-Moss instanton) we find approximate formulas
for the Euclidean action by expanding the scalar field and the metric of the
instanton in the powers of the scalar field amplitude. The order of the
magnitude of the correction to the Hawking-Moss action depends on the order of
the instanton (the number of crossings of the barrier by the scalar field): for
instantons of odd and even orders the correction is of the fourth and third
order in the scalar field amplitude, respectively. If a near-to-limit instanton
of the first order exists in a potential with the curvature at the top of the
barrier greater than 4 (Hubble constant), which is the case if the
fourth derivative of the potential at the top of the barrier is greater than
some negative limit value, the action of the instanton is less than the
Hawking-Moss action and, consequently, the instanton determines the outcome of
the vacuum decay if no other Coleman-de Luccia instanton is admitted by the
potential. A numerical study shows that for the quartic potential the physical
mode of the vacuum decay is given by the Coleman-de Luccia instanton of the
first order also in the region of parameters in which the potential admits two
instantons of the second order.Comment: 16 pages, 3 figures, references adde
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