4.5 Article

Quasielastic lepton scattering and back-to-back nucleons in the short-time approximation

Journal

PHYSICAL REVIEW C
Volume 101, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.101.044612

Keywords

-

Funding

  1. FNAL Intensity Frontier Fellowship
  2. U.S. Department of Energy funds through the Neutrino Theory Network [DE-SC0013617]
  3. U.S. Department of Energy funds through FRIB Theory Alliance grant [DE-SC0013617]
  4. NUclear Computational Low-Energy Initiative (NUCLEI) SciDAC project
  5. U.S. Department of Energy, Office of Science, Office of Nuclear Physics [DE-AC05-06OR23177, DE-AC02-06CH11357, DE-AC52-06NA25396]
  6. Los Alamos LDRD program
  7. DOE Early Career Research Program
  8. U.S. Department of Energy through the Los Alamos National Laboratory
  9. National Nuclear Security Administration of U.S. Department of Energy [89233218CNA000001]
  10. U.S. DOE [DE-AC02-05CH11231]

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Understanding quasielastic electron and neutrino scattering from nuclei has taken on new urgency with current and planned neutrino oscillation experiments, and with electron scattering experiments measuring specific final states, such as those involving nucleon pairs in back-to-back configurations. Accurate many-body methods are available for calculating the response of light (A <= 12) nuclei to electromagnetic and weak probes, but they are computationally intensive and only applicable to the inclusive response. In the present work we introduce a novel approach, based on realistic models of nuclear interactions and currents, to evaluate the short-time (high-energy) inclusive and exclusive response of nuclei. The approach accounts reliably for crucial two-nucleon dynamics, including correlations and currents, and provides information on back-to-back nucleons observed in electron and neutrino scattering experiments. We demonstrate that in the quasielastic regime and at moderate momentum transfers both initial- and final-state correlations and two-nucleon currents are important for a quantitatively successful description of the inclusive response and final-state nucleons. Finally, the approach can be extended to include relativistic-kinematical and dynamical-effects, at least approximately in the two-nucleon sector, and to describe the response in the resonance-excitation region.

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