864 research outputs found

    Expectations of fragment decay from highly excited nuclei

    Get PDF
    The statistical model is used to illustrate the consequences of a successive binary decay mechanism as the initial nuclear excitation is pushed towards the limits of stability. The partition of the excitation energy between light and heavy fragments is explicitly calculated, as are the consequences of the decay of the primary light fragments to particle-bound residual nuclei which would be observed experimentally. The test nucleus 100 44 Ru is considered at initial excitations of 100, 200, 400, and 800 MeV. Exit channels of n, p, and α; and 100 clusters of 3 ≀ Z ≀ 20 ≀ 4, 6 ≀ A ≀ 48 are considered from all nuclides in the deexcitation cascade. The total primary and final cluster yields are shown versus Z and initial excitation. The primary versus final yields are also shown individually for 12C, 26Mg, and 48Ca. We show how multifragmentation yields will change with the excitation energy due to a successive binary decay mechanism. Measurements that may be prone to misinterpretation are discussed, as are those that should be representative of initial nucleus excitation

    Dynamical treatment of Fermi motion in a microscopic description of heavy ion collisions

    Get PDF
    A quasiclassical Pauli potential is used to simulate the Fermi motion of nucleons in a molecular dynamical simulation of heavy ion collisions. The thermostatic properties of a Fermi gas with and without interactions are presented. The inclusion of this Pauli potential into the quantum molecular dynamics (QMD) approach yields a model with well defined fermionic ground states, which is therefore also able to give the excitation energies of the emitted fragments. The deexcitation mechanisms (particle evaporation and multifragmentation) of the new model are investigated. The dynamics of the QMD with Pauli potential is tested by a wide range of comparisons of calculated and experimental double-differential cross sections for inclusive p-induced reactions at incident energies of 80 to 160 MeV. Results at 256 and 800 MeV incident proton energy are presented as predictions for completed experiments which are as yet unpublished

    Implementation of GDH model in TALYS-1.7 code

    Get PDF
    The geometry dependent hybrid model proposed by M.Blann and supplied with models for the non-equilibrium cluster emission was implemented in the TALYS-1.74 code. A number of subprograms of ALICE and ALICE/ASH codes after an appropriate modification were added to TALYS. The value of the TALYS input variable preeqmode equal to five is reserved for the use of new approach. The calculated nucleon and light cluster energy distributions are compared with measured data

    Investigation of soluble adhesion molecules in cancer: beneficial approach or expensive toy? The case of intercellular adhesion molecule-1 (sICAM-1)

    Get PDF
    Adhesion molecules are key topobiological components in almost any kind of cell-cell and cell-matrix interaction in both human physiology and pathology. Heterogeneous processes as platelet adhesion to subendothelial matrix components or leukocyte extravasation at sites of tissue damage are at least in part mediated by adhesion molecules and their corresponding receptors (counter receptors). Using a multitude of modem analytical and preparative approaches ranging from "simple" immunohistochemistry to cloning and gene transfer, in vitro studies provided detailed data on a variety of adhesion molecules and their receptors. However, compared to the speedy accumulation of basic knowledge the evaluation of the diagnostic usefulness of adhesion molecules is still in its infancy.Biomedical Reviews 1994; 3: 73-75

    Quasiparticle Lifetime in a Finite System: A Non--Perturbative Approach

    Full text link
    The problem of electron--electron lifetime in a quantum dot is studied beyond perturbation theory by mapping it onto the problem of localization in the Fock space. We identify two regimes, localized and delocalized, corresponding to quasiparticle spectral peaks of zero and finite width, respectively. In the localized regime, quasiparticle states are very close to single particle excitations. In the delocalized state, each eigenstate is a superposition of states with very different quasiparticle content. A transition between the two regimes occurs at the energy ≃Δ(g/ln⁡g)1/2\simeq\Delta(g/\ln g)^{1/2}, where Δ\Delta is the one particle level spacing, and gg is the dimensionless conductance. Near this energy there is a broad critical region in which the states are multifractal, and are not described by the Golden Rule.Comment: 13 pages, LaTeX, one figur

    Study of the nucleon-induced preequilibrium reactions in terms of the Quantum Molecular Dynamics

    Get PDF
    The preequilibrium (nucleon-in, nucleon-out) angular distributions of 27^{27}Al, 58^{58}Ni and 90^{90}Zr have been analyzed in the energy region from 90 to 200 MeV in terms of the Quantum Moleculear Dynamics (QMD) theory. First, we show that the present approach can reproduce the measured (p,xp') and (p,xn) angular distributions leading to continuous final states without adjusing any parameters. Second, we show the results of the detailed study of the preequilibrium reaction processes; the step-wise contribution to the angular distribution, comparison with the quantum-mechanical Feshbach-Kerman-Koonin theory, the effects of momentum distribution and surface refraction/reflection to the quasifree scattering. Finally, the present method was used to assess the importance of multiple preequilibrium particle emission as a function of projectile energy up to 1 GeV.Comment: 22pages, Revex is used, 10 Postscript figures are available by request from [email protected]

    Preequilibrium Neutron Emission in (p, xn) Reactions with 80-160 MeV Projectiles

    Get PDF
    This research was sponsored by the National Science Foundation Grant NSF PHY 87-1440
    • 

    corecore