201 research outputs found
Effects of Rescattering in (e,e'p) Reactions within a Semiclassical Model
The contribution of rescattering to final state interactions in (e,e'p) cross
sections is studied for medium and high missing energies using a semiclassical
model. This approach considers two-step processes that lead to the emission of
both nucleons.
The effects of nuclear transparency are accounted for in a Glauber inspired
approach and the dispersion effects of the medium at low energies are included.
It is found that rescattering is strongly reduced in parallel kinematics.
At high missing energy and momenta, the distortion of the short-range
correlated tail of the spectral function is dominated by a rearrangement of
that strength itself. In perpendicular kinematics, a further enhancement of the
experimental yield is due to strength that is originally in the mean field
region.
This contribution becomes negligible at large missing momenta.Comment: 10 pages, 9 figures. Minor corrections: improved figures and few
comments adde
The Transparency of 12C for Protons
Existing cross-section data for 1p-shell knockout in the reaction 12C(e,e'p)
- as obtained under different kinematic conditions - are shown to be mutually
consistent, apart from a recent measurement performed in Mainz. New data have
been collected at the Amsterdam Pulse Stretcher that confirm the normalization
of the older measurements. An analysis of the world's 12C(e,e'p) data has
yielded precise values of the spectroscopic factor for 1p-shell and 1s-shell
knockout from 12C. These values have been used to evaluate the transparency of
the 12C nucleus for 1p-shell and 1s-shell protons separately on the basis of
recent high-energy 12C(e,e'p) data taken at a four-momentum transfer squared of
1.1 GeV/c^2. As the resulting average value of the nuclear transparency,
0.81(0.04), is considerably higher than the value obtained from previous
analyses and theoretical estimates, the high Q^2 data were used instead for an
independent determination of the spectroscopic strength for 1p + 1s knockout.
Combining these results with the low Q^2 data the spectroscopic factors appear
to be momentum-transfer dependent. Possible explanations of these surprising
results in terms of reaction-mechanism effects or a possible breakdown of the
quasi-particle concept at high Q^2 are discussed as well.Comment: 11 pages 8 figure
Signals for black body limit in coherent ultraperipheral heavy ion collisions
We argue that study of total cross section of photoabsorption and coherent
photoproduction of -mesons in ultraperipheral heavy ion
collisions (UPC) is effective method to probe onset of black body limit(BBL) in
the soft and hard QCD interactions. We illustrate the expected features of the
onset of BBL using generalized vector dominance model. We show that this model
describes very well -meson coherent photoproduction at . In the case of -meson production we find a UPC cross
section which is a factor larger than the one found by Klein and
Nystrand. The advantages of the process of coherent dijet production to probe
onset of BBL in hard scattering regime where decomposition over the twists
becomes inapplicable are explained and relative importance of the and mechanisms is estimated.Comment: 17 pages, 7 figure
Many-body effects in 16O(e,e'p)
Effects of nucleon-nucleon correlations on exclusive reactions on
closed-shell nuclei leading to single-hole states are studied using
( MeV, ) as an example. The quasi-hole wave
function, calculated from the overlap of translationally invariant many-body
variational wave functions containing realistic spatial, spin and isospin
correlations, seems to describe the initial state of the struck proton
accurately inside the nucleus, however it is too large at the surface. The
effect of short-range correlations on the final state is found to be largely
cancelled by the increase in the transparency for the struck proton. It is
estimated that the values of the spectroscopic factors obtained with the DWIA
may increase by a few percent due to correlation effects in the final state.Comment: 21 Pages, PHY-7849-TH-9
2s1/2 occupancies in 30Si, 31P, and 32S
Elastic electron scattering off Si-30 and P-31 was studied in an effective momentum-transfer range of 1.8-3.0 fm(-1). The form-factor data were analyzed together with existing data sets for these nuclei and for S-32 in a model-independent Fourier-Bessel expansion. For P-31 the M1 contribution was subtracted following an established parametrization. Results of Hartree-Fock (HF) calculations, performed for these three nuclei in a spherical basis and in an axially deformed basis, are compared to experiment. Occupancies have been determined which, when used in the spherical-basis HF calculations, lead to a good description of the elastic form-factor data. The deformed-basis calculations have been used to study the influence of the deformation on the calculated binding energies and ground-state charge densities. In all calculations the influence of using different effective nucleon-nucleon interactions was investigated. The resulting differences in 2s(1/2) in occupancy are combined with results from previous existing (e,e'p) experiments to yield ''absolute occupancies'' for the 2s(1/2) orbital. The deduced 2s(1/2) occupancies for Si-30 and S-32 are 0.24(4) and 1.35(19), respectively.Peer reviewe
Orthogonality Effects in Relativistic Models of Nucleon Knockout Reactions
We study the effect of wave function orthogonality in the relativistic
treatment of the nucleon removal reactions (gamma, p) and (e, e' p). The
continuum wave function describing the outgoing nucleon is made orthogonal to
the relevant bound states using the Gram-Schmidt procedure. This procedure has
the advantage of preserving the asymptotic character of the continuum wave
function and hence the elastic observables are unaffected. The orthogonality
effects are found to be negligible for (e, e' p) reactions for missing momenta
up to 700 MeV/c. This holds true for both parallel and perpendicular
kinematics. By contrast the orthogonalization of the wave functions appears to
have a more pronounced effect in the case of (gamma, p) reactions. We find that
the orthogonality effect can be significant in this case particularly for large
angles. Polarization of the outgoing protons and photon asymmetry show more
sensitivity than the cross sections. If the orthogonality condition is imposed
solely on this one hole state the effects are usually smaller.Comment: LaTeX, 7 postscript figure
Short-Range Correlations and the One-Body Density Matrix in Finite Nuclei
The effects of short-range correlations derived from a realistic
meson-exchange potential on the single-particle density matrix in finite nuclei
are investigated by analyzing the one-body density in terms of the natural
orbits. Basic features of these natural orbits and their spectral distributions
are discussed. For many observables it seems to be sufficient to approximate
the one-body density matrix in terms of those natural orbits, which exhibit the
largest occupation probabilities. For the investigation of the high-momentum
components in the single-particle density, however, it is important to take
into account natural orbits with small occupation probabilities, originating
from the single-particle Green function at large negative energies.Comment: 13 pages, RevTeX, 5 figures adde
First measurements of the ^16O(e,e'pn)^14N reaction
This paper reports on the first measurement of the ^16O(e,e'pn)^14N reaction.
Data were measured in kinematics centred on a super-parallel geometry at energy
and momentum transfers of 215 MeV and 316 MeV/c. The experimental resolution
was sufficient to distinguish groups of states in the residual nucleus but not
good enough to separate individual states. The data show a strong dependence on
missing momentum and this dependence appears to be different for two groups of
states in the residual nucleus. Theoretical calculations of the reaction using
the Pavia code do not reproduce the shape or the magnitude of the data.Comment: 10 pages, 11 figures, 2 tables, Accepted for publication in EPJ
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