Matches in SemOpenAlex for { <https://semopenalex.org/work/W2888329174> ?p ?o ?g. }
- W2888329174 abstract "The reconstruction of the neutrino energy is crucial in oscillation experiments that use interactions with nuclei to detect the neutrino. The common reconstruction procedure is based on the kinematics of the final-state lepton. The interpretation of the reconstructed energy in terms of the real neutrino energy must rely on a model for the neutrino-nucleus interaction. The Relativistic Fermi Gas (RFG) model is frequently used in these analyses. In the Hartree-Fock (HF) model for quasielastic nucleon knockout, the bound nucleon wave functions are obtained using an effective nucleon-nucleon force. The final-state wave function is constructed from continuum states in the same potential which have the correct asymptotic behavior. The Continuum Random Phase Approximation (CRPA) model extends the HF approach taking long range correlations into account in a self-consistent way. Considering only single-nucleon processes, the distributions of reconstructed neutrino energies obtained within the HF-CRPA approach are compared with the results of the RFG, an RPWIA calculation, and the RPA+np-nh model of Martini et al. We find that the distributions of reconstructed energies for a fixed incoming energy in the HF-CRPA display additional strength in the low reconstructed energy tails compared to models without elastic distortion of the outgoing nucleon. This asymmetry redistributes strength from higher to lower values of the reconstructed energy. The mean field description of the nuclear dynamics results in a reshaping of the reconstructed energy distribution that cannot be accounted for in a plane wave impulse approximation model, even by modifying ad hoc parameters such as the binding energy. In particular it is shown that in the RFG calculations there is no value of the binding energy which is able to reproduce the entire T2K $nu_mu$ oscillated spectrum as calculated in HF-CRPA." @default.
- W2888329174 created "2018-08-31" @default.
- W2888329174 creator A5040580561 @default.
- W2888329174 creator A5043394198 @default.
- W2888329174 creator A5053666699 @default.
- W2888329174 creator A5055452165 @default.
- W2888329174 creator A5056046714 @default.
- W2888329174 creator A5073571364 @default.
- W2888329174 date "2018-11-05" @default.
- W2888329174 modified "2023-10-16" @default.
- W2888329174 title "Mean-field approach to reconstructed neutrino energy distributions in accelerator-based experiments" @default.
- W2888329174 cites W1528899469 @default.
- W2888329174 cites W1590237081 @default.
- W2888329174 cites W1652762507 @default.
- W2888329174 cites W1997123809 @default.
- W2888329174 cites W2007935939 @default.
- W2888329174 cites W2009689168 @default.
- W2888329174 cites W2011385462 @default.
- W2888329174 cites W2015873717 @default.
- W2888329174 cites W2020372739 @default.
- W2888329174 cites W2032939415 @default.
- W2888329174 cites W2033418271 @default.
- W2888329174 cites W2047543579 @default.
- W2888329174 cites W2049380746 @default.
- W2888329174 cites W2054281826 @default.
- W2888329174 cites W2057961756 @default.
- W2888329174 cites W2060907290 @default.
- W2888329174 cites W2075049743 @default.
- W2888329174 cites W2075430016 @default.
- W2888329174 cites W2076824831 @default.
- W2888329174 cites W2089122291 @default.
- W2888329174 cites W2103863537 @default.
- W2888329174 cites W2105118134 @default.
- W2888329174 cites W2109217121 @default.
- W2888329174 cites W2115427208 @default.
- W2888329174 cites W2115831339 @default.
- W2888329174 cites W2129807146 @default.
- W2888329174 cites W2225737993 @default.
- W2888329174 cites W2259068844 @default.
- W2888329174 cites W2260238348 @default.
- W2888329174 cites W2335052899 @default.
- W2888329174 cites W2469020134 @default.
- W2888329174 cites W2526984592 @default.
- W2888329174 cites W2556123407 @default.
- W2888329174 cites W2732310250 @default.
- W2888329174 cites W3122937415 @default.
- W2888329174 cites W4232314582 @default.
- W2888329174 doi "https://doi.org/10.1103/physrevc.98.054603" @default.
- W2888329174 hasPublicationYear "2018" @default.
- W2888329174 type Work @default.
- W2888329174 sameAs 2888329174 @default.
- W2888329174 citedByCount "11" @default.
- W2888329174 countsByYear W28883291742019 @default.
- W2888329174 countsByYear W28883291742020 @default.
- W2888329174 countsByYear W28883291742021 @default.
- W2888329174 countsByYear W28883291742022 @default.
- W2888329174 countsByYear W28883291742023 @default.
- W2888329174 crossrefType "journal-article" @default.
- W2888329174 hasAuthorship W2888329174A5040580561 @default.
- W2888329174 hasAuthorship W2888329174A5043394198 @default.
- W2888329174 hasAuthorship W2888329174A5053666699 @default.
- W2888329174 hasAuthorship W2888329174A5055452165 @default.
- W2888329174 hasAuthorship W2888329174A5056046714 @default.
- W2888329174 hasAuthorship W2888329174A5073571364 @default.
- W2888329174 hasBestOaLocation W28883291741 @default.
- W2888329174 hasConcept C109214941 @default.
- W2888329174 hasConcept C121332964 @default.
- W2888329174 hasConcept C138309006 @default.
- W2888329174 hasConcept C172695262 @default.
- W2888329174 hasConcept C185544564 @default.
- W2888329174 hasConcept C186453547 @default.
- W2888329174 hasConcept C62520636 @default.
- W2888329174 hasConceptScore W2888329174C109214941 @default.
- W2888329174 hasConceptScore W2888329174C121332964 @default.
- W2888329174 hasConceptScore W2888329174C138309006 @default.
- W2888329174 hasConceptScore W2888329174C172695262 @default.
- W2888329174 hasConceptScore W2888329174C185544564 @default.
- W2888329174 hasConceptScore W2888329174C186453547 @default.
- W2888329174 hasConceptScore W2888329174C62520636 @default.
- W2888329174 hasFunder F4320313831 @default.
- W2888329174 hasFunder F4320321454 @default.
- W2888329174 hasFunder F4320321730 @default.
- W2888329174 hasFunder F4320322603 @default.
- W2888329174 hasFunder F4320333031 @default.
- W2888329174 hasFunder F4320335227 @default.
- W2888329174 hasIssue "5" @default.
- W2888329174 hasLocation W28883291741 @default.
- W2888329174 hasLocation W28883291742 @default.
- W2888329174 hasLocation W28883291743 @default.
- W2888329174 hasLocation W28883291744 @default.
- W2888329174 hasLocation W28883291745 @default.
- W2888329174 hasLocation W28883291746 @default.
- W2888329174 hasLocation W28883291747 @default.
- W2888329174 hasOpenAccess W2888329174 @default.
- W2888329174 hasPrimaryLocation W28883291741 @default.
- W2888329174 hasRelatedWork W1807381854 @default.
- W2888329174 hasRelatedWork W2005969941 @default.
- W2888329174 hasRelatedWork W2046930511 @default.
- W2888329174 hasRelatedWork W2748952813 @default.
- W2888329174 hasRelatedWork W2951860434 @default.