62,436 research outputs found

    Binding-energy independence of reduced spectroscopic strengths derived from (p, 2p) and (p, pn) reactions with nitrogen and oxygen isotopes

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    A campaign of intermediate energy (300-450 MeV/u) proton-induced nucleon knockout measurements in inverse kinematics has been recently undertaken at the R 3 B/LAND setup at GSI. We present a systematic theoretical analysis of these data with the aim of studying the quenching of the single-particle strengths and its binding-energy dependence. For that, the measured semi-inclusive (p, 2p) and (p, pn) cross sections are compared with theoretical predictions based on single-particle cross sections derived from a novel coupled-channels formalism and shell-model spectroscopic factors. A systematic reduction of about 20-30% is found, with a very limited dependence on proton-neutron asymmetry.Comment: 8 pages, 3 figure

    Production of thermal photons in viscous fluid dynamics with temperature-dependent shear viscosity

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    We compute the spectrum of thermal photons created in Au+Au collisions at sNN=200\sqrt{s_{NN}}=200 GeV, taking into account dissipative corrections in production processes corresponding to the quark--gluon plasma and hadronic phases. To describe the evolution of the fireball we use a viscous fluid dynamic model with different parametrizations for the temperature--dependence of η/s\eta/s. We find that the spectrum significantly depends on the values of η/s\eta/s in the QGP phase, and is almost insensitive to the values in the hadronic phase. We also compare the influence of the temperature--dependence of η/s\eta/s on the spectrum of thermal photons to that of using different equations of state in the fluid dynamic simulations, finding that both effects are of the same order of magnitude.Comment: 16 pages, 4 figures. Accepted for publication in Mod. Phys. Lett.

    Corrugation of relativistic magnetized shock waves

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    As a shock front interacts with turbulence, it develops corrugation which induces outgoing wave modes in the downstream plasma. For a fast shock wave, the incoming wave modes can either be fast magnetosonic waves originating from downstream, outrunning the shock, or eigenmodes of the upstream plasma drifting through the shock. Using linear perturbation theory in relativistic MHD, this paper provides a general analysis of the corrugation of relativistic magnetized fast shock waves resulting from their interaction with small amplitude disturbances. Transfer functions characterizing the linear response for each of the outgoing modes are calculated as a function of the magnetization of the upstream medium and as a function of the nature of the incoming wave. Interestingly, if the latter is an eigenmode of the upstream plasma, we find that there exists a resonance at which the (linear) response of the shock becomes large or even diverges. This result may have profound consequences on the phenomenology of astrophysical relativistic magnetized shock waves.Comment: 14 pages, 9 figures; to appear in Ap

    Description of the 11^{11}Li(p,d)10(p,d){^{10}}Li transfer reaction using structure overlaps from a full three-body model

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    Recent data on the differential angular distribution for the transfer reaction 11^{11}Li(p,d)10^{10}Li at E/A=5.7E/A=5.7 MeV in inverse kinematics are analysed within the DWBA reaction framework, using the overlap functions calculated within a three-body model of 11^{11}Li. The weight of the different 10^{10}Li configurations in the system's ground state is obtained from the structure calculations unambiguously. The effect of the 9^{9}Li spin in the calculated observables is also investigated. We find that, although all the considered models succeed in reproducing the shape of the data, the magnitude is very sensitive to the content of p1/2p_{1/2} wave in the 11^{11}Li ground-state wave function. Among the considered models, the best agreement with the data is obtained when the 11^{11}Li ground state contains a \sim31\% of p1/2p_{1/2} wave in the nn-9^9Li subsystem. Although this model takes into account explicitly the splitting of the 1+1^+ and 2+2^+ resonances due to the coupling of the p1/2p_{1/2} wave to the 3/23/2^- spin of the core, a similar degree of agreement can be achieved with a model in which the 9^{9}Li spin is ignored, provided that it contains a similar p-wave content.Comment: 8 pages, 3 figures. Final versio

    Linking structure and dynamics in (p,pn)(p,pn) reactions with Borromean nuclei: the 11^{11}Li(p,pn)10(p,pn){^{10}}Li case

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    One-neutron removal (p,pn)(p,pn) reactions induced by two-neutron Borromean nuclei are studied within a Transfer-to-the-Continuum (TC) reaction framework, which incorporates the three-body character of the incident nucleus. The relative energy distribution of the residual unbound two-body subsystem, which is assumed to retain information on the structure of the original three-body projectile, is computed by evaluating the transition amplitude for different neutron-core final states in the continuum. These transition amplitudes depend on the overlaps between the original three-body ground-state wave function and the two-body continuum states populated in the reaction, thus ensuring a consistent description of the incident and final nuclei. By comparing different 11^{11}Li three-body models, it is found that the 11^{11}Li(p,pn)10(p,pn){^{10}}Li relative energy spectrum is very sensitive to the position of the p1/2p_{1/2} and s1/2s_{1/2} states in 10^{10}Li and to the partial wave content of these configurations within the 11^{11}Li ground-state wave function. The possible presence of a low-lying d5/2d_{5/2} resonance is discussed. The coupling of the single particle configurations with the non-zero spin of the 9^{9}Li core, which produces a spin-spin splitting of the states, is also studied. Among the considered models, the best agreement with the available data is obtained with a 11^{11}Li model that incorporates the actual spin of the core and contains \sim31\% of p1/2p_{1/2}-wave content in the nn-9^9Li subsystem, in accord with our previous findings for the 11^{11}Li(p,d)10^{10}Li transfer reaction, and a near-threshold virtual state.Comment: 7 pages, 4 figures, submitted to PL
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