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1.
The observation of refractive effects in 16O+16O and 16O+12C elastic scattering data has definitively established the fact that the optical potential for some light heavy-ion systems is relatively transparent and that its real part is deep. Most of the interpretations of the rainbow features of these data rely on the so-called nearside-farside decomposition of the scattering amplitude. Starting from recent optical model analyses of 16O+16O and 16O+12C elastic scattering around 100 MeV incident energy as an example, we present an alternative interpretation based on the barrier-wave/internal-wave decomposition first proposed by Brink and Takigawa. This method, which complements the nearside-farside approach, demonstrates clearly the exceptional transparency of the 16O+16O, and to a lesser extent 16O+12C, interactions at the investigated energies and makes possible the extraction of the two contributions whose interference explains the Airy oscillations seen in the farside amplitude.  相似文献   

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The real optical potential for 16O+16O system is calculated within a generalized version of the double-folding model with the Pauli knock-on exchange effects between the projectile nucleons and the target nucleons taken into account from first principle. The elastic scattering data at Elab=350 MeV supplemented by the new measurement at larger angles seem to be the first case in heavy-ion scattering where one can test the reliability of different theoretical heavy-ion optical potentials. Predictions are made for the elastic scattering of 16O+16O at laboratory energies of 240–480 MeV to illustrare the energy dependence of the rainbow structure which has been clearly observed in experiment at 350 MeV.  相似文献   

4.
Angular distributions have been measured for the elastic and inelastic scattering of 18O by 16O and 18O at laboratory bombarding energies of 42 and 52 MeV. The inelastic scattering data are analyzed in terms of collective excitations using a coupled channel approach. Deformation parameters are obtained for the strongly excited states. The relationship between the strength of inelastic scattering and the amount of structure in the elastic scattering distributions is discussed.  相似文献   

5.
An investigation of refractive effects in heavy-ion scattering is continued. For the elastic scattering of 16O nuclei on a 13C target at E(16O) = 132 MeV, the differential cross sections are measured for the first time in addition to previous measurements for targets from the carbon isotopes 12C and 14C. Airy structures that are similar for all isotopes and which have close cross sections are observed and are found to be consistent with the energy systematics of Airy minima that were obtained previously. The volume integrals of the real and imaginary parts of the optical potentials found in the present study are nearly identical for all of the isotopes considered here and are also in good agreement with the systematics obtained previously.  相似文献   

6.
《Nuclear Physics A》1988,481(1):94-108
We explain qualitatively the oscillations seen in the total fusion excitation function of 16O on 12C by using an optical model potential containing a parity dependence which accounts for elastic α-particle transfer. We show that it is possible to achieve this while simultaneously obtaining a reasonable fit to the elastic angular distributions. In particular the anomalous large angle scattering is consistent with the parity dependence required to fit the fusion oscillations.  相似文献   

7.
The direct search with pattern search technique of Hooke and Jeeves has been programmed to search for heavy-ion optical model parameters and the results of unconstrained searches using this method for 16O + 11B elastic scattering are presented.  相似文献   

8.
《Nuclear Physics A》1998,628(1):1-16
High precision fusion excitation functions have been measured for the 16O+58Ni and 16O+62Ni systems from which fusion barrier distributions have been evaluated. Coupled-reaction-channels (CRC) calculations, which describe elastic and quasi-elastic scattering, also satisfactorily reproduce the fusion cross sections and barrier distributions. The small value of Z1Z2 in this case leads to barrier distributions with relatively little structure. However, in conjunction with the detailed elastic scattering data for these systems, this allows us to elucidate the role of previously ignored states in 16O in pushing the entire distribution to lower energies. These shifts are consistent with derived magnitudes of polarization potentials for both systems.  相似文献   

9.
Elastic and inelastic quantal scattering is described by a theory in which the contribution of a range of impact parameters to the scattering amplitude is determined by a phase integral (“eikonal”) which is integrated along a real curved “quantal” trajectory. This amplitude reduces to the Glauber expression in the high-energy, forward-angle limit, and to the usual semiclassical amplitude in the classical limit. The formulation can be applied to the study of heavy-ion scattering. The quantal trajectories are investigated analytically for the case of Coulomb scattering. A numerical analysis of elastic 16O16O scattering is carried out. The results show appreciable improvement as compared with the Glauber approximation.  相似文献   

10.
Based on the potential resonance in heavy-ion collisions and on the optical model,the gross resonant structure appeared in the complete fusion excitation function and the phenomenon of the backward-angle oscillatory rise in the elastic scattering angular distribution for 16O+24Mg system are studied by using a deep opdcal potendal.The calculated results of the opdcal model are compared with those of the nuclear molecular orbital model.The origin of the gross resonant structure is discussed.  相似文献   

11.
The total reaction cross section for 16O + 16O has been measured at six energies between Ec.m. = 6.8 and 11.9 MeV. Cross sections for the production of protons, alphas, neutrons, deuterons, 31S, 30P, 12C(g.s.) + 20Ne(g.s.) and the relative γ-yield were obtained with a variety of experimental methods. No 3H or 3He were found. All cross sections are normalized to 16O + 16O elastic scattering at θc.m. = 90°, which was measured separately with high precision between Ec.m. = 7.3 and 14.4 MeV. The elastic scattering and relative γ-yield of 12C + 12C were measured between Ec.m. = 3.9 and 7.5 MeV. The elastic scattering and neutron yield of 12C + 16O were measured between Ec.m. = 5.4 and 10.1 MeV.  相似文献   

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The European Physical Journal A - Existing data for the 6Li + 16O elastic scattering at $ E_{c.m.}=3.27$ -36.8MeV were analyzed within the optical model and coupled-reaction-channels method. The...  相似文献   

14.
The method presented in a previous paper to study heavy-ion scattering is simplified by the introduction of an approximate form of the matrix element over the external region. The approximation does not affect the accuracy but lowers greatly the computational time. Formulae for energies and widths of resonances are also introduced. Results obtained for α-16O scattering are compared with other theoretical results and with experiment.  相似文献   

15.
Zeitschrift für Physik A Hadrons and nuclei - Excitation functions of the elastic and inelastic scattering cross sections of16O and18O nuclei on70Ge have been measured at angles between...  相似文献   

16.
On the basis of the dispersive alpha-cluster model for target nuclei and the theory of multiple diffractive scattering, differential cross sections and analyzing powers for the elastic scattering of 400 and 700-MeV deuterons on 12C and 16O target nuclei were calculated in the pointlike-deuteron approximation. In these calculations, the amplitude for incident-deuteron scattering on nuclei was constructed with the aid of amplitudes for scattering that were obtained from a fit to data on d 16O scattering. The same features were calculated on the basis of the diffraction approximation with allowance for the internal deuteron structure by using the amplitudes obtained earlier for nucleon scattering on 12C and 16O nuclei within the same dispersive alpha-clustermodel. The latter made it possible to perform calculations without employing adjustable parameters. The observables calculated on the basis of either approach agree with available experimental data.  相似文献   

17.
The elastic scattering of12C+12C and16O+16O has been studied in the framework of an incoming wave boundary condition model. Different logarithmic derivatives for the incoming waves have been tested and their effects investigated with the help of Fourier analyses. It is shown that a logarithmic derivative obtained from a JWKB approximation leads to strong absorption of the low partial waves while a logarithmic derivative constant for all partial waves causes reflections. These reflections are necessary to describe the high energy elastic scattering of12C+12C. The fits thus obtained with shallow real potentials are comparable to those obtained with deep folding potentials. It is shown that not the lowest partial waves, but those within a window just below the grazing angular momentum are most important for the higher energy12C+12C angular distributions.  相似文献   

18.
The 16O + 16O optical potential is obtained by using the folding method together with a previously defined complex effective nucleon-nucleon force closely related with the heavy-ion collision dynamics. This type of force allows the computation of both the real and the imaginary parts of the optical potential. Through the use of the folding method, finite-range effects are correctly incorporated. In that respect, the present results improve upon those obtained with the local density approximation. They also compare favourably with the phenomenologieal optical potentials.  相似文献   

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Calculations are presented of the elastic scattering and fusion cross sections for the astrophysically interesting reactions 12C+12C, 12C+16O and 16O+16O. The calculations are performed using the incoming wave boundary condition (IWB) and a real ion-ion interaction potential. The results are compared with the available experimental data for the energy region near and below the Coulomb barrier. With values of two adjustable potential parameters (the radial position of the l = 0 barrier and the diffuseness) determined by fitting elastic scattering data, good agreement is obtained for the average energy dependence of the 12C+12C and 12C+16O fusion cross sections. In the case of 16O+16O, both the calculated absolute magnitude and the energy dependence of the fusion cross section are inconsistent with the data and this discrepancy is discussed.  相似文献   

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