Lepton scattering off few-nucleon systems at medium and high energies

The interpretation of recent JLab experimental data on the exclusive process A(e,e′p)B off few-nucleon systems is analyzed in terms of realistic nuclear wave functions and the Glauber multiple scattering theory, both in its original form and within a generalized eikonal approximation. The relevance of the exclusive process ⁴He(e,e′p)³H for possible investigations of QCD effects is illustrated.     

Electron Raman scattering of a two-dimensional pseudodot system

We have carried out the theoretical investigation of the differential cross section for the electron Raman scattering process, which is associated with intersubband transitions in a two-dimensional quantum pseudodot system. The great advantage of our methodology is that it enables confinement regimes by varying two parameters in the model potential. It is found that the differential cross section is affected by the external magnetic field, the geometrical size and the chemical potential of the pseudodot system.     

Optical-model and DWBA application to the few-nucleon problem

An attempt is made to describe p+d elastic scattering in the framework of the optical model. Angular distributions are analyzed in the energy range from 17 to 46.3 MeV. It is found necessary to take into account the contribution of elastic transfer, here calculated by means of DWBA. Total reaction cross section and the angular distribution of the reaction ²H(p, d^∗)p are predicted and compared with experimental data. The success of this attempt suggests the possible use of the optical model and DWBA in few-nucleon problems.     

Electron atomic scattering factors and scattering potentials of crystals

The concepts of complex electron atomic scattering factors and principles for evaluating these factors are discussed and their applicability is examined. Numerical procedures and routines for calculating these factors are described, and for 98 neutron atoms and 109 ions the real part of the electron atomic scattering factors were parameterized using 10 and eight parameters, respectively. Procedures for constructing two and three dimensional scattering potentials using the complex atomic scattering factors are illustrated with examples; effects of thermal vibrations of the crystal lattice are discussed.     

Electron scattering in the dip region

Two-body exchange currents in the noninteracting relativistic Fermi gas model are taken into account with special emphasis put on the role of the delta-isobar to reproduce the transverse response function in the dip region. Due to a resonance behaviour relativistic two-body isobar currents are found to be important for a comparison with the experimental data. Real-pion production is studied within the same framework and the importance and physical implications of the energy dependence of the delta-isobar decay width are stressed. The contents of these lectures have been/will be published in M.J. Dekker, P.J. Brussaard, and J.A. Tjon: Phys. Rev. C49 (1994) 2650–2670 and Phys. Rev. C (1995).Lectures given at the Indian-Summer School on Electron Scattering of Nucleons and Nuclei, Prague (Czech Republic), September 1994.     

Relativistic Hamiltonian dynamics and few-nucleon systems

We present a preliminary calculation of the electromagnetic form factors of ³He and ³H, performed within the light-front Hamiltonian dynamics. Relativistic effects show their relevance even at the static limit, increasing at higher values of momentum transfer, as expected.     

Electron scattering in photoemission

Kane's one-dimensional model of the scattering of photoelectrons as they propagate to the emitting surface is generalized to the three-dimensional case. It is shown that this problem reduces to the Milne problem. An analytic expression is obtained for the probability of an electron's reaching the surface.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 12, pp. 72–75, December, 1980.     

Electron temperature (T e) measurements by Thomson scattering system

Thomson scattering technique based on high power laser has already proved its superoirity in measuring the electron temperature (T _e and density (n _e) in fusion plasma devices like tokamaks. The method is a direct and unambiguous one, widely used for the localised and simultaneous measurements of the above parameters. In Thomson scattering experiment, the light scattered by the plasma electrons is used for the measurements. The plasma electron temperature is measured from the Doppler shifted scattered spectrum and density from the total scattered intensity. A single point Thomson scattering system involving a Q-switched ruby laser and PMTs as the detector is deployed in ADITYA tokamak to give the plasma electron parameters. The system is capable of providing the parameters T _e from 30 eV to 1 keV and n _e from 5 × 10¹²cm⁻³−5 × 10¹³cm⁻³. The system is also able to give the parameter profile from the plasma center (Z=0 cm) to a vertical position of Z=+22 cm to Z=−14 cm, with a spatial resolution of 1 cm on shot to shot basis. This paper discusses the initial measurements of the plasma temperature from ADITYA.     

Electron scattering by atoms and molecules

Recent advances in the scattering of electrons by free atoms and molecules are considered with an emphasis on the interface between experiment and theory. A survey is made of the theory and methods of measurement and their trend towards the perfect scattering experiment. For atomic targets a detailed coverage is given of the various theoretical models and the results compared with experimental data. For elastic and excitation collisions, the low and high energy regions are reasonably well understood. In the medium energy region, extending from a few times the ionization threshold down to about the ionization threshold there are still difficulties arising from the infinite number of open channels. For ionizing collisions, the three body Coulomb interaction still presents unanswered theoretical problems but has inspired some elegant experimental studies. For molecular targets the additional complexities arising from the nuclear motion, the lack of a centre of symmetry and the evaluation of multicentre integrals are considered. A brief discussion of some current problems and possible future developments is given.     

Electron scattering in the interacting boson model

It is suggested that the interacting boson model be used in the analysis of electron scattering data. Qualitative features of the expected behavior of the inelastic excitation of some 2⁺ states in the transitional SmNd region are discussed.     

Electron scattering from transitional nuclei

An electron scattering experiment on ¹⁸⁸Os, ¹⁹⁰Os, ¹⁹²Os, ¹⁹⁴Pt and ¹⁹⁶Pt has been performed at momentum transfers q = 0.6 to 3.2 fm⁻¹. Transition charge densities have been determined for the low-lying 2⁺, 3⁻ and 4⁺ states. The 2⁺ densities are well reproduced within the framework of the interacting boson model 2, where we have determined the boson densities α_ν, α_π, β_νv and β_π. The 4⁺ transition densities could not be reproduced indicating the need for including a g-boson. The ground and transition charge densities of ¹⁸⁸Os, ¹⁹²Os and ¹⁹⁶Pt have been compared with a microscopic calculation. The total binding energies and the intrinsic wave functions have been calculated for different values of β and γ with the constrained triaxial Hartree-Fock-Bogoliubov method using the finite range interaction D1SA. These energies are interpreted as potential energy surfaces and used in the Bohr hamiltonian in order to obtain the total nuclear wave functions. We obtain very good agreement with experiment. The calculated potential energy surfaces show these nuclei to be γ-soft with a shallow minimum for triaxial deformations and rigid in the β direction.     

Electron scattering for exotic nuclei

A brand-new electron scattering facility, the SCRIT Electron Scattering Facility, will soon start its operation at RIKEN RI Beam Factory, Japan. This is the world’s first electron scattering facility dedicated to the structure studies of short-lived nuclei. The goal of this facility is to determine the charge density distributions of short-lived exotic nuclei by elastic electron scattering. The first collision between electrons and exotic nuclei will be observed in the year 2014.     

Electron scattering by polar molecules

Theoretical and experimental studies of electron-polar molecule collisions are reviewed. Principal emphasis is placed on elastic scattering and excitation of rotational states by low-energy (less than about 10 eV) electrons. After a survey of experimental techniques and methods of cross-section calculation, the results are compared with each other. In particular, the dipole-moment dependence of the cross-section is discussed in relation to possible bound states in a dipole field. Examples of applications of the resulting cross-section are demonstrated. Finally future problems are summarized.     

Electron and positron scattering from atomic potassium

The present coupled-channels-optical method (CCO) provides a comprehensive theoretical calculation of electron-potassium atom and positron-potassium atom scattering at intermediate energies. The CCO calculations for various physical observables are compared with the convergent close-coupling method (CCC) and other theoretical results, as well as experimental data where available. The CCO provides good to fair agreement with results from the convergent close coupling calculations, which are considered to be the state of the art for alkali atoms in the electron channel.