161 research outputs found

    Quasi-free (p,2p) and (p,pn) reactions with unstable nuclei

    Get PDF
    We study (p,2p) and (p,pn) reactions at proton energies in the range of 100 MeV -- 1 GeV. Our purpose is to explore the most sensitive observables in unpolarized reactions with inverse kinematics involving radioactive nuclei. We formulate a model based on the eikonal theory to describe total cross sections and momentum distributions of the recoiled residual nucleus. The model is similar to the one adopted for knockout reactions with heavy ions. We show that momentum distributions are sensitive to the angular momentum of the ejected nucleon which can be used as an spectroscopic tool. The total cross sections are sensitive to the nucleon separation energies and to multiple scattering effects. Our calculations also indicate that a beam energy around 500 MeV/nucleon has a smaller dependence on the anisotropy of the nucleon-nucleon elastic scattering.Comment: 17 pages, 12 figures, Accepted for publication in the Physical review

    Two-nucleon knockout contributions to the 12^{12}C(e,ep)(e,e'p) reaction in the dip and {Δ\Delta}(1232) regions

    Full text link
    The contributions from 12^{12}C(e,epn)(e,e'pn) and 12^{12}C(e,epp)(e,e'pp) to the semi-exclusive 12^{12}C(e,ep)(e,e'p) cross section have been calculated in an unfactorized model for two-nucleon emission. We assume direct two-nucleon knockout after virtual photon coupling with the two-body pion-exchange currents in the target nucleus. Results are presented at several kinematical conditions in the dip and Δ\Delta(1232) regions. The calculated two-nucleon knockout strength is observed to account for a large fraction of the measured (e,ep)(e,e'p) strength above the two-nucleon emission threshold.Comment: 12 Revtex pages, 4 postscript figures (available upon request), University of Gent preprint SSF94-02-0

    Inclusive (e,eN)(e,e^\prime N), (e,eNN)(e,e^\prime NN), (e,eπ)(e,e^\prime \pi) ... reactions in nuclei

    Get PDF
    We study the inclusive (e,eN)(e,e^\prime N), (e,eNN)(e,e^\prime NN), (e,eπ)(e,e^\prime \pi), (e,eπN)(e,e^\prime \pi N) reactions in nuclei using a Monte Carlo simulation method to treat the multichannel problem of the final state. The input consists of reaction probabilities for the different steps evaluated using microscopical many body methods. We obtain a good agreement with experiment in some channels where there is data and make predictions for other channels which are presently under investigation in several electron laboratories. The comparison of the theoretical results with experiment for several kinematical conditions and diverse channels can serve to learn about different physical processes ocurring in the reaction. The potential of this theoretical tool to make prospections for possible experiments, aiming at pinning down certain reaction probabilities, is also emphasized.Comment: 21 pages (LaTeX + figure files

    The 2p-2h electromagnetic response in the quasielastic peak and beyond

    Get PDF
    The contribution to the nuclear transverse response function R_T arising from two particle-two hole (2p-2h) states excited through the action of electromagnetic meson exchange currents (MEC) is computed in a fully relativistic framework. The MEC considered are those carried by the pion and by Delta degrees of freedom, the latter being viewed as a virtual nucleonic resonance. The calculation is performed in the relativistic Fermi gas model in which Lorentz covariance can be maintained. All 2p-2h many-body diagrams containing two pionic lines that contribute to R_T are taken into account and the relative impact of the various components of the MEC on R_T is addressed. The non-relativistic limit of the MEC contributions is also discussed and compared with the relativistic results to explore the role played by relativity in obtaining the 2p-2h nuclear response.Comment: 27 pages, 12 figures, revtex4; minor modifications in the discussion of the results, references adde

    Finite-Energy Sum Rules in Eta Photoproduction off the Nucleon

    Get PDF
    The reaction γNηN{\gamma}N \to {\eta}N is studied in the high-energy regime (with photon lab energies Eγlab>4E_{\gamma}^{\textrm{lab}} > 4 GeV) using information from the resonance region through the use of finite-energy sum rules (FESR). We illustrate how analyticity allows one to map the t-dependence of the unknown Regge residue functions. We provide predictions for the energy dependence of the beam asymmetry at high energies.Comment: Joint Physics Analysis Cente

    Two-proton overlap functions in the Jastrow correlation method and cross section of the 16^{16}O(e,epp)14(e,e^{\prime}pp)^{14}Cg.s._{\rm g.s.} reaction

    Full text link
    Using the relationship between the two-particle overlap functions (TOF's) and the two-body density matrix (TDM), the TOF's for the 16^{16}O(e,epp)14(e,e^{\prime}pp)^{14}Cg.s._{\rm g.s.} reaction are calculated on the basis of a TDM obtained within the Jastrow correlation method. The main contributions of the removal of 1S0^1S_0 and 3P1^3P_1 pppp pairs from 16^{16}O are considered in the calculation of the cross section of the 16^{16}O(e,epp)14(e,e^{\prime}pp)^{14}Cg.s._{\rm g.s.} reaction using the Jastrow TOF's which include short-range correlations (SRC). The results are compared with the cross sections calculated with different theoretical treatments of the TOF's.Comment: 10 pages, 8 figures, ReVTeX

    Polarization degrees of freedom in photoinduced two-nucleon knockout from finite nuclei

    Get PDF
    The polarization degrees of freedom in photoinduced two-nucleon knockout from finite nuclei are studied. It is pointed out that they open good perspectives to study the dynamics of dinucleons in the medium in detail. The (γ,pp\gamma,pp) and (γ,pn\gamma,pn) angular cross sections, photon asymmetries and outgoing nucleon polarizations are calculated for the target nuclei 16^{16}O and 12^{12}C and photonenergies ranging from 100 up to 500 MeV. It is investigated to which degree the two-nucleon emission reaction is dominated by photoabsorption on 3S1(T=0)^3S_1(T=0) proton-neutron and 1S0(T=1)^1S_0(T=1) proton-proton pairs in the nuclear medium. The calculations demonstrate that dominance of SS wave photoabsorption in the (γ,pn\gamma,pn) channel does not necessarily imply that the reaction mechanism is similar to what is observed in deuteron photodisintegration.Comment: 27 pages, REVTeX 3.0 with epsf.sty, 11 figures in EPS forma

    Proton recoil polarization in exclusive (e,e'pp) reactions

    Full text link
    The general formalism of nucleon recoil polarization in the (e,eNN{\vec e},e'{\vec N}N) reaction is given. Numerical predictions are presented for the components of the outgoing proton polarization and of the polarization transfer coefficient in the specific case of the exclusive 16^{16}O(e,epp{\vec e},e'{\vec p}p)14^{14}C knockout reaction leading to discrete states in the residual nucleus. Reaction calculations are performed in a direct knockout framework where final-state interactions and one-body and two-body currents are included. The two-nucleon overlap integrals are obtained from a calculation of the two-proton spectral function of 16^{16}O where long-range and short-range correlations are consistently included. The comparison of results obtained in different kinematics confirms that resolution of different final states in the 16^{16}O(e,epp{\vec e},e'{\vec p}p)14^{14}C reaction may act as a filter to disentangle and separately investigate the reaction processes due to short-range correlations and two-body currents and indicates that measurements of the components of the outgoing proton polarization may offer good opportunities to study short-range correlations.Comment: 12 pages, 6 figure

    First measurements of the ^16O(e,e'pn)^14N reaction

    Get PDF
    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
    corecore