S. Kox

Improved sterile neutrino constraints from the STEREO experiment with 179 days of reactor-on data

H. Almazán, L. Bernard, Adrien Blanchet, A. Bonhomme et autres

The STEREO experiment is a very short baseline reactor antineutrino experiment. It is designed to test the hypothesis of light sterile neutrinos being the cause of a deficit of the observed antineutrino interaction rate at short baselines with respect to the predicted …

de, fr (code pays fourni par la source)

Improved STEREO simulation with a new gamma ray spectrum of excited gadolinium isotopes using FIFRELIN

H. Almazán, L. Bernard, Adrien Blanchet, A. Bonhomme et autres

Abstract. The STEREO experiment measures the electron antineutrino spectrum emitted in a research reactor using the inverse beta decay reaction on H nuclei in a gadolinium loaded liquid scintillator. The detection is based on a signal coincidence of a prompt positron and …

de, fr (code pays fourni par la source)

Sterile Neutrino Constraints from the STEREO Experiment with 66 Days of Reactor-On Data

H. Almazán, P. del Amo Sanchez, L. Bernard, Adrien Blanchet et autres

The reactor antineutrino anomaly might be explained by the oscillation of reactor antineutrinos toward a sterile neutrino of eV mass. In order to explore this hypothesis, the STEREO experiment measures the antineutrino energy spectrum in six different detector cells covering baselines between …

de, fr (code pays fourni par la source)

The STEREO Experiment

N. Allemandou, H. Almazán, P. del Amo Sanchez, L. Bernard et autres

The STEREO experiment is a very short baseline reactor antineutrino experiment aiming at testing the hypothesis of light sterile neutrinos as an explanation of the deficit of the observed neutrino interaction rate with respect to the predicted rate, known as the Reactor …

fr, de, at (code pays fourni par la source)

Sterile neutrino exclusion from the STEREO experiment with 66 days of reactor-on data

H. Almazán, P. del Amo Sanchez, L. Bernard, Adrien Blanchet et autres

Production of light nuclei and anti-nuclei in pp and Pb-Pb collisions at energies available at the CERN Large Hadron Collider

J. Adam, D. Adamová, M. M. Aggarwal, G. Aglieri Rinella et autres

The production of (anti-)deuteron and (anti-)$^{3}\text{He}$ nuclei in Pb-Pb collisions at $\sqrt{{s}_{\mathrm{NN}}}=2.76$ TeV has been studied using the ALICE detector at the LHC. The spectra exhibit a significant hardening with increasing centrality. Combined blast-wave fits of several particles support the interpretation that …

cz, in, ch, it, pk, kr, us, ru, gb, mx, ua, no, de, br, hr, fr, es, hu, cn, pl, dk, nl, jp (code pays fourni par la source)

Production of light nuclei and anti-nuclei in pp and Pb-Pb collisions at energies available at the CERN Large Hadron Collider

J. Adam, D. Adamová, M. M. Aggarwal, G. Aglieri Rinella et autres

Adam, J.; Adamová, D.; Aggarwal, M. M.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahmed, I.; Ahn, S. U.; Aimo, I.; Aiola, S.; Ajaz, M.; Akindinov, A.; Alam, S. N.; Aleksandrov, D.; Alessandro, B.; Alexandre, D.; Alfaro Molina, R.; Alici, …

One-dimensional pion, kaon, and proton femtoscopy in Pb-Pb collisions at sNN=2.76 TeV

J. Adam, D. Adamová, M. M. Aggarwal, G. Aglieri Rinella et autres

The size of the particle emission region in high-energy collisions can be deduced using the femtoscopic correlations of particle pairs at low relative momentum. Such correlations arise due to quantum statistics and Coulomb and strong final state interactions. In this paper, results …

cz, in, ch, it, kr, us, pk, ru, gb, mx, ua, no, de, br, hr, fr, es, hu, cn, pl, dk, nl, jp (code pays fourni par la source)

Coherent ρ 0 photoproduction in ultra-peripheral Pb-Pb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

J. Adam, D. Adamová, M. M. Aggarwal, G. Aglieri Rinella et autres

We report the first measurement at the LHC of coherent photoproduction of ρ 0 mesons in ultra-peripheral Pb-Pb collisions.The invariant mass and transverse momentum distributions for ρ 0 production are studied in the π + π -decay channel at mid-rapidity.The production cross …

cz, in, ch, it, kr, us, pk, ru, gb, mx, ua, no, br, de, hr, fr, es, hu, cn, pl, dk, nl, jp (code pays fourni par la source)

Charged jet cross sections and properties in proton-proton collisions at s=7 TeV

B. Abelev, J. Adam, D. Adamová, M. M. Aggarwal et autres

The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at center-of-mass energy $\sqrt{s}=7\text{ }\text{ }\mathrm{TeV}$ using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the midrapidity …

us, cz, in, ch, it, pk, kr, ru, gb, ua, no, de, br, hr, fr, es, Afrique du Sud, hu, pl, dk, mx, nl, jp (code pays fourni par la source)

Rapidity and transverse-momentum dependence of the inclusive J/ψ nuclear modification factor in p-Pb collisions at s N N $$ \sqrt{s_{N\ N}} $$ = 5.02 TeV

J. Adam, D. Adamová, M. M. Aggarwal, G. Aglieri Rinella et autres

Rapidity and transverse-momentum dependence of the inclusive J/ψ nuclear modification factor in p-Pb collisions at √ sNN = 5.02 TeV

cz, in, ch, it, pk, kr, us, ru, gb, mx, ua, no, br, de, hr, fr, es, hu, cn, pl, dk, nl, jp (code pays fourni par la source)

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

B. I. Abelev, J. Adam, D. Adamová, M. M. Aggarwal et autres

The elliptic flow coefficient (v 2 ) of identified particles in Pb-Pb collisions at √ s NN = 2.76 TeV was measured with the ALICE detector at the Large Hadron Collider (LHC).The results were obtained with the Scalar Product method, a two-particle …

us, cz, in, it, pk, kr, ru, gb, ua, no, br, de, hr, fr, es, ch, Afrique du Sud, hu, pl, dk, mx, nl, jp (code pays fourni par la source)