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Register a new userStudy of dimuon production in Indium-Indium collisions with the NA60 experiment
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The NA60 experiment at the CERN-SPS is devoted to the study of dimuon production in heavy-ion and proton-nucleus collisions. We present preliminary results from the analysis of Indium-Indium collisions at 158 GeV per nucleon. The topics covered are low mass vector meson production, J/psi production and suppression, and the feasibility of the open charm measurement from the dimuon continuum in the mass range below the J/psi peak.
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NA60 is a fixed-target experiment at the CERN SPS which measured dimuon production in nucleus-nucleus and proton-nucleus collisions. In this paper we report on a precision measurement of low-mass muon pairs in 158 AGeV indium-indium collisions. A significant excess of pairs is observed above the yield expected from neutral meson decays. The excess can be isolated by subtraction of expected sources, thanks to the excellent mass resolution and large sample size.
The NA60 experiment studies muon pair production at the CERN SPS. In this letter we report on a precision measurement of J/psi in In-In collisions. We have studied the J/psi centrality distribution, and we have compared it with the one expected if absorption in cold nuclear matter were the only active suppression mechanism. For collisions involving more than ~80 participant nucleons, we find that an extra suppression is present. This result is in qualitative agreement with previous Pb-Pb measurements by the NA50 experiment, but no theoretical explanation is presently able to coherently describe both results.
The NA60 experiment has studied low-mass muon pair production in proton-nucleus collisions with a system of Be, Cu, In, W, Pb and U targets using a 400 GeV/$c$ proton beam at the CERN SPS. The mass spectrum is well described by the superposition of the two-body and Dalitz decays of the light neutral mesons $eta$, $rho$, $omega$, $eta$ and $phi$. A new high-precision measurement of the electromagnetic transition form factors of the $eta$ and $omega$ mesons is presented, complemented with a measurement of the temperature parameter of the $rho$ meson in cold nuclear matter. The $pt$ spectra for the $omega$ and $phi$ mesons are extracted in the full $pt$ range accessible, up to $pt = 2$ GeV/$c$. The nuclear dependence of the production cross sections for the $eta$, $omega$ and $phi$ mesons has been investigated in terms of the power law $sigma_mathrm{pA} propto mathrm{A}^alpha$, and the $alpha$ parameter was studied as a function of $pt$.
The yield of muon pairs in the invariant mass region 1<M<2.5 GeV/c^2 produced in heavy-ion collisions significantly exceeds the sum of the two expected contributions, Drell-Yan dimuons and muon pairs from the decays of D meson pairs. These sources properly account for the dimuons produced in proton-nucleus collisions. In this paper, we show that dimuons are also produced in excess in 158 A GeV In-In collisions. We furthermore observe, by tagging the dimuon vertices, that this excess is not due to enhanced D meson production, but made of prompt muon pairs, as expected from a source of thermal dimuons specific to high-energy nucleus-nucleus collisions. The yield of this excess increases significantly from peripheral to central collisions, both with respect to the Drell-Yan yield and to the number of nucleons participating in the collisions. Furthermore, the transverse mass distributions of the excess dimuons are well described by an exponential function, with inverse slope values around 190 MeV. The values are independent of mass and significantly lower than those found at masses below 1 GeV/c^2, rising there up to 250 MeV due to radial flow. This suggests the emission source of thermal dimuons above 1 GeV/c^2 to be of largely partonic origin, when radial flow has not yet built up.
The NA60 experiment has studied low-mass muon pair production in proton-nucleus collisions with a system of Be, Cu, In, W, Pb and U targets, using a 400 GeV proton beam at the CERN SPS. The transverse momentum spectra of the $rho/omega$ and $phi$ mesons are measured in the full $p_mathrm{T}$ range accessible, from $p_mathrm{T} = 0$ up to 2 GeV/$c$. The nuclear dependence of the production cross sections of the $eta$, $omega$ and $phi$ mesons has been found to be consistent with the power law $sigma_mathrm{pA} propto mathrm{A}^alpha$, with the $alpha$ parameter increasing as a function of $p_mathrm{T}$ for all the particles, and an approximate hierarchy $alpha_eta approx alpha_phi > alpha_omega$. The cross section ratios $sigma_eta/sigma_omega$, $sigma_rho/sigma_omega$ and $sigma_phi/sigma_omega$ have been studied as a function of the size A of the production target, and an increase of the $eta$ and $phi$ yields relative to the $omega$ is observed from p-Be to p-U collisions.
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