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Tvaskis, V.; Arrington, J.; Asaturyan, R.; Baker, O. K.; Blok, H.P.; Bosted, P.; Boswell, M.; Bruell, A.; Christy, M. E.; Cochran, A.; Ent, R.; Filippone, B. W.; Gasparian, A.; Keppel, C.; Kinney, E.; Lapikás, L.; Lorenzon, W.; Mack, D.; Mammei, J.; Martin, J. W.; Mkrtchyan, H.; Niculescu, I.; Piercey, R. B.; Potterveld, D. H.; Smith, G. R.; Spurlock, K.; Steenhoven, G. van der; Stepanyan, S.; Tadevosian, V.; Wood, S. A.

doi:10.1103/physrevc.81.055207

Cited by 15 publications

(8 citation statements)

References 91 publications

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“…In addition, new high precision inclusive data have, or will shortly become, available from Jefferson Lab on nucleons and nuclei which can be used both to determine the vector contributions to inclusive structure functions, as well as to test the modeling of the nuclear medium. These data include Jefferson Lab Hall C experiments E99-118 (targets p, 2 H) [91,92], E94-110 (p) [93], E02-019 (p, 2 H) [94], E03-103 ( 2 H, 3 He, 4 He, 9 Be and 12 C) [95], E02-109 (p, 2 H) , E06-009 ( 2 H) [96], and E04-001 ( 12 C, 27 Al, 56 Fe, 64 Cu) [97] from the JUPITER collaboration.…”

Section: B Experimental Inputmentioning

confidence: 99%

NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering

Alvarez‐Ruso

Athar

Bárbaro

et al. 2018

Progress in Particle and Nuclear Physics

312

288

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Future high-precision neutrino interaction experiments are needed to extend the current program of GeV-scale neutrino interactions and should include:1. A feasibility study of a high-statistics hydrogen or deuterium scattering experiment to supplement the currently poorly known (anti)neutrino-nucleon cross sections.2. The need for (anti)neutrino Ar scattering data in the energy range relevant for the DUNE experiment.3. The possibility of muon-based neutrino beams providing extremely accurate knowledge of the neutrino flux and an intense electron neutrino beam.• Current and future long-and short-baseline neutrino oscillation programs should evaluate and articulate what additional neutrino-nucleus interaction data is required to meet their ambitious goals and support experiments that provide this data.In addition to these general challenges facing the community, there are more specific concerns for particular topics and interaction channels. These are summarized below in the form of observations, problem description or recommendations. For a deeper insight, the reader is encouraged to consult the subsequent sections of this paper.

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Section: B Experimental Inputmentioning

confidence: 99%

NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering

Alvarez‐Ruso

Athar

Bárbaro

et al. 2018

Progress in Particle and Nuclear Physics

312

288

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“…In our calculation of this contribution by means of MAID we consider that the deuteron structure function F d 2 is determined by (20), what naturally leads to the value of the contribution close to the result (29). Numerous experimental data, including the above-mentioned [26][27][28] show that the approximate equation F d 2 ≈ F p 2 , where F d 2 is determined as the deuteron structure function per nucleon, sufficiently accurately holds in different kinematic regions. Our other calculation of hadronic polarizability contribution on the basis of experimental data for F d 2 (22) gives smaller result 20.2 µeV .…”

mentioning

confidence: 89%

“…The difference is related with different structure functions F p 2 and F d 2 which enter in (7) and the reduced mass dependence. Thus, to obtain the numerical value of the correction on the deuteron polarizability, we can use the experimental data on deuteron structure functions F d 1,2 (ν, k 2 ) and their different parameterizations [26][27][28].…”

mentioning

confidence: 99%

Hadronic deuteron polarizability contribution to the Lamb shift in muonic deuterium

et al. 2016

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Hadronic deuteron polarizability correction to the Lamb shift of muonic deuterium is calculated on the basis of unitary isobar model and modern experimental data on the structure functions of deep inelastic lepton-deuteron scattering and their parametrizations in the resonance and nonresonance regions.Finding more accurate values of the charge radii of the proton and deuteron in experiments of the CREMA collaboration 1-5 requires a comparison of experimental data and theoretical calculations of the Lamb shift. The deuteron structure and polarizability contributions to the Lamb shift (2P -2S) and hyperfine structure in muonic deuterium are among those corrections which are not known at present with the accuracy comparable with pure electromagnetic corrections. 6-10 The deuteron polarizability effect is related with the excitation of particles which enter in its † Corresponding author 1650104-1 Mod. Phys. Lett. A Downloaded from www.worldscientific.com by UNIVERSITY OF CALIFORNIA @ SANTA BARBARA on 06/14/16. For personal use only. A. V. Eskin et al.

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“…Inclusive deep-inelastic scattering (DIS) from the deuteron has for a considerable time been the main source of information on the partonic structure of the neutron [1][2][3][4][5]. Recently there has been growing emphasis placed on such extractions at large values of the momentum fraction x carried by the partons [6][7][8][9][10][11].…”

Section: Introductionmentioning

confidence: 99%

Final-state interactions in inclusive deep-inelastic scattering from the deuteron

2014

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We explore the role of final-state interactions (FSIs) in inclusive deep-inelastic scattering from the deuteron. Relating the inclusive cross section to the deuteron forward virtual Compton scattering amplitude, a general formula for the FSI contribution is derived in the generalized eikonal approximation, utilizing the diffractive nature of the effective hadron-nucleon interaction. The calculation uses a factorized model with a basis of three resonances with mass W < 2 GeV and a continuum contribution for larger W as the relevant set of effective hadron states entering the final-state interaction amplitude. The results show sizeable on-shell FSI contributions for Bjorken x 0.6 and Q 2 10 GeV 2 , increasing in magnitude for lower Q 2 , but vanishing in the high-Q 2 limit because of phase-space constraints. The off-shell rescattering contributes at x 0.8 and is taken as an uncertainty on the on-shell result.

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Proton and deuteronF2structure function at lowQ2

Cited by 15 publications

References 91 publications

NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering

NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering

Hadronic deuteron polarizability contribution to the Lamb shift in muonic deuterium

Final-state interactions in inclusive deep-inelastic scattering from the deuteron

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