Transverse electron scattering response function of {sup 3}He

Journal Article · Tue Apr 15 04:00:00 EDT 2008 · Physical Review. C, Nuclear Physics

DOI:https://doi.org/10.1103/PHYSREVC.77.044007· OSTI ID:21189897

Della Monaca, Sara; Yuan, Luping P ^[1]; Efros, Victor D ^[2]; Khugaev, Avas ^[3]; Leidemann, Winfried; Orlandini, Giuseppina ^[1]; Tomusiak, Edward L ^[4]

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1. Dipartimento di Fisica, Universita di Trento, I-38100 Trento (Italy)
2. Russian Research Centre 'Kurchatov Institute', RU-123182 Moscow (Russian Federation)
3. Institute of Nuclear Physics, Uzbekistan Academy of Sciences, Tashkent (Uzbekistan)
4. Department of Physics and Astronomy, University of Victoria, Victoria, British Columbia V8P 1A1 (Canada)

The transverse response function R{sub T}(q,{omega}) for {sup 3}He is calculated using the configuration space BonnA nucleon-nucleon potential, the Tucson-Melbourne three-body force, and the Coulomb potential. Final states are completely taken into account via the Lorentz integral transform technique. Nonrelativistic one-body currents plus two-body {pi} and {rho} meson exchange currents (MECs) as well as the Siegert operator are included. The response R{sub T} is calculated for q=174, 250, 400, and 500 MeV/c and in the threshold region at q=174, 324, and 487 MeV/c. Strong MEC effects are found in low- and high-energy tails, but due to MECs there are also moderate enhancements of the quasielastic peak (6-10%). The calculation is performed both directly and via transformation of electric multipoles to a form that involves the charge operator. The contribution of the latter operator is suppressed in and below the quasielastic peak, while at higher energies the charge operator represents almost the whole MEC contribution at the lowest q value. The effect of the Coulomb force in the final state interaction is investigated for the threshold region at q=174 MeV/c. Its neglect enhances R{sub T} by more than 10% in the range up to 2 MeV above threshold. In a comparison with experimental data, one finds relatively good agreement at q=250 and 400 MeV/c, while at q=500 MeV/c, presumably due to relativistic effects, the theoretical quasielastic peak position is shifted to somewhat higher energies. The strong MEC contributions in the threshold region are nicely confirmed by data at q=324 and 487 MeV/c.

• OSTI ID: 21189897
• Journal Information: Physical Review. C, Nuclear Physics, Journal Name: Physical Review. C, Nuclear Physics Journal Issue: 4 Vol. 77; ISSN 0556-2813; ISSN PRVCAN
• Country of Publication: United States
• Language: English

Related Subjects

73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BOSON-EXCHANGE MODELS
COMPARATIVE EVALUATIONS
CONFIGURATION
COULOMB FIELD
CURRENTS
ELECTRONS
FINAL-STATE INTERACTIONS
HELIUM 3
MEV RANGE 100-1000
MULTIPOLES
NUCLEON-NUCLEON POTENTIAL
Q-VALUE
RELATIVISTIC RANGE
RESPONSE FUNCTIONS
SCATTERING
THREE-BODY PROBLEM
TWO-BODY PROBLEM