The line shape in atomic beam laser spectroscopy experiments has been calculated for an atomic beam emitted from an open filament and propagated into the vacuum under collisionless conditions. It is ...shown that the activation energy the atoms have to overcome in order to leave the sample leads to significant deviations from the Voigt line shape. The unreliable application of the Voigt profile under the conditions specified above leads to an overestimate of the line width by up to 70%. A modified Voigt profile is given, which has proved a reliable capability to describe the line shape under the above mentioned conditions.
Experimental data on K
+ meson and proton sideward flow measured with the FOPI detector at SIS/GSI in the reactions Ru+Ru at 1.69
A GeV and Ni+Ni at 1.93
A GeV are presented. The K
+ sideward flow is ...found to be anti-correlated (correlated) with the one of protons at low (high) transverse momenta. When compared to the predictions of a transport model, the data favour the existence of an in-medium repulsive K
+-nucleon potential.
An overview is given over recent measurement of flow and particle production in the energy range from 0.1 to 2 AGeV. Excitation functions for the directed sideward and the azimuthally symmetric ...transverse flow are presented and show the importance of flow phenomena in this incident energy regime. Rapidity density distributions are indicative of a system size dependence of the stopping process. The role of strange particles as a probe for the hot and dense phase of hadronic matter is discussed with respect to the production and propagation. The spectra of Kaons indicate an equilibration with the surrounding baryons during the expansion while their directed flow pattern is different from that of the nucleons.
Directed sideward flow of light charged particles and intermediate mass fragments was measured in different symmetric reactions at bombarding energies from 90 to 800
A MeV. The flow parameter is ...found to increase with the charge of the detected fragment up to
Z = 3–4 and then turns into saturation for heavier fragments. Guided by simple simulations of an anisotropic expanding thermal source, we show that the value at saturation can provide a good estimate of the flow angle, Θ
flow, in the participant region. It is found that Θ
flow depends strongly on the impact parameter. The excitation function of Θ
folw reveals striking deviations from the ideal hydrodynamical scaling. The data exhibit a steep rise of Θ
flow to a maximum at around 250 – 400
A MeV, followed by a moderate decrease as the bombarding energy increases further.
Four different combinations of 9644Ru and 9640Zr nuclei, both as projectile and target, were investigated at the same bombarding energy of 400A MeV using a 4pi detector. The degree of isospin mixing ...between projectile and target nucleons is mapped across a large portion of the phase space using two different isospin-tracer observables, the number of measured protons and the tritium to 3He yield ratio. The experimental results show that the global equilibrium is not reached even in the most central collisions. Quantitative measures of stopping and mixing are extracted from the data. They are found to exhibit a quite strong sensitivity to the in-medium ( n,n) cross section used in microscopic transport calculations.
The incident energy at which the azimuthal distributions in semicentral heavy-ion collisions change from in-plane to out-of-plane enhancement —
E
tran is studied as a function of mass of emitted ...particles, their transverse momentum and centrality for Au+Au collisions. The analysis is performed in a reference frame rotated with the sidewards flow angle (
Θ
flow) relative to the beam axis.
A systematic decrease of
E
tran as function of mass of the reaction products, their transverse momentum and collision centrality is evidenced.
The predictions of a microscopic transport model (IQMD) are compared with the experimental results.
Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra ...of pions are well reproduced by adding the pions originating from the Delta-resonance decay to the component of thermal pions, deduced from the high transverse momentum part of the pion spectra. About 10 and 18% of the nucleons are excited to Delta states at freeze-out for beam energies of 1 and 2 AGeV, respectively.
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