Elasticp+12C scattering between 0.3 and 2 MeV

Absolute differential cross-sections ofp+¹²C elastic scattering have been measured at _cm=89.1°, 118.7°, 146.9° for bombarding energies between 0.3 and 2.0 MeV. Revised level parameters of the first three excited states in¹³N have been extracted with aR-matrix analysis. It is shown that the influence of the bound ground-state of¹³N has an appreciable effect on low-energy scattering. Recent predictions concerning Mott-Schwinger polarization are also discussed.     

π+ and π− scattering from 12C at 150 MeV

High-resolution elastic and inelastic data were obtained for π⁺ and π^? scattering ¹²C. Spectra were taken with the SIN pion spectrometer at 148 MeV over a wide angular range.     

Detailed energy dependence of the elastic and inelastic12C +12C scattering between 5 and 10 MeV/nucleon

Excitation functions for¹²C+¹²C elastic and inelastic scattering to 2⁺ level have been measured over the energy range 30–60 MeV (cm) by 250 keV steps using the kinematical coincidence method. The intermediate structure resonances disappear aboveE _cm=35 MeV while the broad and irregular structure becomes a general feature of the interaction at higher energies.     

Observation of the nuclear rainbow scattering for12C+12C atE Lab =300 MeV

The elastic and inelastic scattering of¹²C on¹²C has been measured in the angular range between 2.8° and 70.4° in the c.m. system atE _Lab =300 MeV. Optical model calculations have been performed with Woods-Saxon and folded potentials, the ground state and the first 2⁺-state were coupled in the calculations. The large cross sections of the elastic scattering at large angles is related to the nuclear rainbow scattering, which is centered at about 56°. This requires a potential depth of 100 MeV at a distance of 3 fm, the fit to the data is sensitive down to this region. The calculations with the folded potential show a better agreement with the data than those with the Woods-Saxon shape. The total reaction cross section of 1,420 mb, obtained from the optical model analysis, corresponds to the geometrical value; no transparency is observed.     

Analysis of 12C + 12C Elastic Scattering for Energy between 70 and 1440 MeV

Physics of Atomic Nuclei - In the present work, we reanalysis the 12C + 12C refractive scattering over a wide energy range. The analysis is performed in the framework of optical model with the...     

Elastic and inelastic scattering of 12C by 12C in the energy range between 10 and 37.6 MeV

The elastic and inelastic scattering of ¹²C by ¹²C has been measured over a wide angular range employing a kinematical analysis with the help of position-sensitive detectors. The bombarding energy was varied in 200 keV steps between 10 and 37.6 MeV. The cross sections are analysed in the framework of compound fluctuations and the direct reaction model.     

Interaction of 80 MeV12C with88Sr; Neutron transfer,inelastic scattering and spin alignment of the 2+ State of12C

Level structure of¹⁰²Cd has been studied via both¹⁰²In decay and nuclear reactions. Using⁹²Mo+¹⁴N at 86 MeV, the nucleus¹⁰²In was identified and its decay (T _1/2=24 ±4s) studied with the aid of on-line mass separation techniques. Levels of¹⁰²Cd were also populated with⁹²Mo+¹²C at 50 MeV and¹⁰²Pd+³He at 35 MeV reactions and investigated by means of standard in-beam techniques. A level scheme including states up to 4.5 MeV excitation energy is proposed and then discussed in the frame of available calculations.     

Spin alignment in12C+12C inelastic scattering

The spin alignment P_zz of¹²C(2 ₁ ⁺ ) produced in¹²C+¹²C inelastic scattering at bombarding energies in the region of known resonances between E_cm=18.5 and 32.8 MeV has been determined with a γ-ray detector positioned in the direction of the scattering normal. The values obtained in the centers of three resonances as well as those obtained off-resonance are spread over a range between ?.05 and +.80 with no clear indication in favour of simple pictures of molecular resonances.     

Elastic and inelastic scattering of 185 MeV protons from 12C

The polarization of 185 MeV protons in elastic scattering and in the excitation of the 2⁺ state at 4.44 MeV and the 0⁺ state at 7.65 MeV in ¹²C has been measured in the angular region 2°–60°. Optical model calculations are performed for the elastic scattering. Angular distributions for the inelastic scattering from the 2⁺ state at 4.44 MeV and the 3^? state at 9.64 MeV are calculated in the distorted-wave impulse approximation (DWIA) as well as in the distorted-wave Born approximation (DWBA).     

Them-state population of12C2+ in inelastic scattering

The spin alignment of the¹²C₂ ⁺ state in inelastic scattering of¹²c on⁶⁴zn at E_L=65 MeV has been measured using the γ-recoil-in-flight method. Good agreement with coupled channel calculations are obtained. The sensitivity of the spin alignment to reaction models is discussed.     

Fusion, resonances and scattering in12C+12C reaction

The variation of fusion cross-section (σJ_fus) with energy in the¹²C+¹²C collision is linked to the underlying resonance phenomenon through the behavior of reaction cross-section (σ) of which σ_fus is taken as a part. The calculation of σ_fus is done through an energy-dependent imaginary potential in the optical model potential (OMP). Through dispersion relation, such an imaginary potential gives rise to energy-dependent real potential which is incorporated in the OMP. In our calculation, a form of potential for the nuclear part which has a soft repulsive in-built core is introduced based on similar works done earlier. The calculated results of σ_fus are used to explain the oscillatory structure, astrophysical S-factor and the decreasing trend at higher energies of the experimental σ_fus data in the case of¹²C+¹²C system with remarkable success. The potential used for fusion calculation is tested for fitting elastic scattering data at some energies and is found good in forward angles. Further improvement of the fitting of these data is obtained by incorporating a coupling potential in the surface region. About twenty resonances are observed in our calculation in the specific partial waves and some of them are found close to the experimentally identified resonances in¹²C+¹²C reaction. Thus, we provide an integrated and comprehensive analysis of fusion, resonance and scattering data in the best studied case of¹²C+¹²C reaction within the framework of optical potential model.     

Energy dependence of heavy ion collisions 4He + 12C and 12C + 12C elastic scattering

We have studied the transparency of heavy ion collisions at high energies by using Glauber's multiple scattering theory. The good agreement between our calculation and the existing data available strongly emphasizes the dominance of the nucleon-nucleon interaction in nucleus-nucleus collisions at high energies.     

Elastic scattering of6Li on12C at 20 MeV

The elastic scattering of lithium nuclei from carbon was measured atE _lab=20 MeV. The obtained angular distribution was fitted by an optical model calculation. Parameter sets and the corresponding transmission coefficients are given.     

46.8MeV的(-p)+12C非弹性散射

在Glauber多重散射理论框架下,使用跃迁密度方法和三种NN湮没势,计算了46.8MeV的反质子在12C上的非弹性散射微分截面.理论曲线与实验数据符合得较好.     

Elastic scattering of positive pions from 12C at 29 MeV

The elastic scattering cross section of positive pions at 29 MeV scattered from ¹²C has been measured at scattering angles between 15° and 150°. The cross section drops to a sharp minimum at about 40° and then rises to about 4 mb/sr at back angles.     

One-nucleon transfer reactions in the12C+12C system at 344.5 MeV

Angular distributions of cross sections have been measured for single nucleon transfer reactions induced by 344.5 MeV¹²C ions on a¹²C target. DWBA analyses have been performed for transitions to discrete final states. Spectroscopic information has been derived and is compared with results of other studies.     

Excitation of 15.11 MeV levels in 12C and 13C by inelastic electron scattering

The Ml radiation widths to the ground states of the 15.11 MeV levels in ¹²C and ¹³C have been determined to be 36 ± 3 eV and 25 ± 7 eV, respectively, by the inelastic scattering of 40 to 65 MeV electrons from a solid target enriched to 58% in ¹³C and a comparison ¹²C target. These results are in agreement with the shell model predictions of Cohen and Kurath.