Applications of quark-hadron duality in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>structure function

Malace, S.; Adams, G. S.; Ahmidouch, A.; Angelescu, T.; Arrington, J.; Asaturyan, R.; Baker, O. K.; Benmouna, N.; Blok, H.P.; Boeglin, W.; Bosted, P.; Breuer, H.; Christy, M. E.; Cui, Yanou; Dalton, M. M.; Danagoulian, S.; Day, D.; Dunne, J.; Dutta, D.; Ent, R.; Fenker, H.; Gan, L.; Gaskell, D.; Hafidi, K.; Hinton, W.; Holt, R. J.; Horn, T.; Huber, G. M.; Hungerford, E. V.; Jiang, X.; Jones, M.; Joo, K. S.; Kalantarians, N.; Kelly, J. J.; Keppel, C.; Kinney, E.; Kubarovsky, V.; Li, Y.; Liang, Y.; Markowitz, P.; McGrath, Elizabeth J.; McKee, P.; Meekins, D.; Mkrtchyan, H.; Navasardyan, T.; Niculescu, G.; Niculescu, I.; Reimer, P. E.; Reinhold, J.; Roche, J.; Schulte, E.; Segbefia, E.; Smith, C.; Smith, G. R.; Tadevosyan, V.; Tang, L.; Ungaro, M.; Uzzle, A.; Vidakovic, S.; Villano, A. N.; Vulcan, W.; Wesselmann, F. R.; Wojtsekhowski, B.; Wood, S. A.; Yuan, L.; Zheng, X.

doi:10.1103/physrevc.80.035207

Cited by 60 publications

(70 citation statements)

References 58 publications

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“…New information is provided in the region with Q 2 1 GeV 2 and 15 GeV 2 < W 2 < 45 GeV 2 , corresponding to 0.006 < x < 0.04. [19], JLAB [20][21][22][23]) and collider experiments (H1 and ZEUS) [44]. The data are overlaid with new fits to world data, including the data presented here, of inclusive proton (GD11-P) and deuteron (GD11-D) cross sections.…”

Section: Discussion Of the Resultsmentioning

confidence: 99%

“…, JLAB [20,22,23], the HERMES data presented here, and real photon data [45]. In the case of HERA, only data points with Q 2 < 1000 GeV 2 were used in order to minimize contributions from weak processes to the cross section.…”

Section: Bcdms [15]mentioning

confidence: 99%

“…In the case of HERA, only data points with Q 2 < 1000 GeV 2 were used in order to minimize contributions from weak processes to the cross section. The fit to deuteron data includes 2497 data points from the SLAC experiments E49a, E49b, E61, E87, E89a, E89b, E139, E140 [19], NMC [17]; E665 [18]; BCDMS [15]; JLAB [21][22][23]; the HERMES data presented in this paper, and real photon data [45]. Table 3 lists in more detail the data sets, together with their x and Q 2 ranges.…”

Section: Bcdms [15]mentioning

confidence: 99%

“…E665 [18] ( √ s ∼ = 12 − 31 GeV), experiments with electrons at SLAC [19] ( √ s ≤ 7 GeV) and at JLAB [20][21][22][23]) ( √ s ≤ 3.25 GeV). The HERMES experiment [24] at HERA collected a large data set for positron and electron scattering on a variety of nuclear targets, including the proton and deuteron data presented here.…”

Section: The Muon Experiments Bcdms [15] Emc [16] Nmc [17] Andmentioning

confidence: 99%

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Inclusive measurements of inelastic electron and positron scattering from unpolarized hydrogen and deuterium targets

Airapetian¹,

Акопов²,

Akopov³

et al. 2011

J. High Energ. Phys.

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Results of inclusive measurements of inelastic electron and positron scattering from unpolarized protons and deuterons at the HERMES experiment are presented. The structure functions F p 2 and F d 2 are determined using a parameterization of existing data for the longitudinal-to-transverse virtual-photon absorption cross-section ratio. The HERMES results provide data in the ranges 0.006 ≤ x ≤ 0.9 and 0.1 GeV 2 ≤ Q 2 ≤ 20 GeV 2 , covering the transition region between the perturbative and the non-perturbative regimes of QCD in a so-far largely unexplored kinematic region. They are in agreement with existing world data in the region of overlap. The measured cross sections are used, in combination with data from other experiments, to perform fits to the photon-nucleon cross section using the functional form of the ALLM model. The deuteron-to-proton cross-section ratio is also determined.

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Section: Discussion Of the Resultsmentioning

confidence: 99%

Section: Bcdms [15]mentioning

confidence: 99%

Section: Bcdms [15]mentioning

confidence: 99%

Section: The Muon Experiments Bcdms [15] Emc [16] Nmc [17] Andmentioning

confidence: 99%

See 2 more Smart Citations

Inclusive measurements of inelastic electron and positron scattering from unpolarized hydrogen and deuterium targets

Airapetian¹,

Акопов²,

Akopov³

et al. 2011

J. High Energ. Phys.

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“…The target assembly, described in detail in Refs. [24,25], also included an aluminum "dummy target" that was used for background measurements and subtraction. Precise cross-section measurements require accurate knowledge of target thickness and target density.…”

Section: Methodsmentioning

confidence: 99%

Measurements of the separated longitudinal structure function FL from hydrogen and deuterium targets at low Q2

Tvaskis¹,

Tvaskis²,

Niculescu³

et al. 2018

Phys. Rev. C

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Structure functions, as measured in lepton-nucleon scattering, have proven to be very useful in studying the partonic dynamics within the nucleon. However, it is experimentally difficult to separately determine the longitudinal and transverse structure functions, and consequently there are substantially less data available in particular for the longitudinal structure function. Here, we present separated structure functions for hydrogen and deuterium at low four-momentum transfer squared, Q 2 < 1 GeV 2 , and compare them with parton distribution parametrization and k T factorization approaches. While differences are found, the parametrizations generally agree with the data, even at the very low-Q 2 scale of the data. The deuterium data show a smaller longitudinal structure function and a smaller ratio of longitudinal to transverse cross section, R, than the proton. This suggests 2469-9985/2018/97(4)/045204 (11) 045204-1 ©2018 American Physical Society V. TVASKIS et al.PHYSICAL REVIEW C 97, 045204 (2018) either an unexpected difference in R for the proton and the neutron or a suppression of the gluonic distribution in nuclei.

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Polarized Proton Structure in the Resonance Region

Blin

Mokeev

2023

Few-Body Syst

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In view of the precise data available on inclusive polarized electron scattering off polarized proton targets in the nucleon resonance excitation region, we compare these results with the coherent sum of resonant contributions to the polarized structure function $$g_1$$ g 1 and virtual photon asymmetry $$A_1$$ A 1 . To this goal, we employ the nucleon resonance electroexcitation amplitudes determined for photon virtualities $$Q^2$$ Q 2 < 5.0 GeV$$^2$$ 2 from analyses of the CLAS data on exclusive electroproduction off protons in the resonance region. Most of the well established resonances of four star PDG status in the mass range up to 1.75 GeV are included. We find that the resonance-like structures observed in the inclusive $$g_1$$ g 1 data are related to the resonant contributions in the entire range of photon virtuality $$Q^2$$ Q 2 where the data on $$g_1$$ g 1 are available. In the range of invariant mass of the final hadron system W > 1.5 GeV, the data on the asymmetry $$A_1$$ A 1 are well reproduced even when accounting for resonant contributions only, especially for the larger values of $$Q^2$$ Q 2 and energies analysed. This observation offers an interesting hint to quark-hadron duality seen in polarized inclusive electron scattering observables.

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Applications of quark-hadron duality in theF2structure function

Cited by 60 publications

References 58 publications

Inclusive measurements of inelastic electron and positron scattering from unpolarized hydrogen and deuterium targets

Inclusive measurements of inelastic electron and positron scattering from unpolarized hydrogen and deuterium targets

Measurements of the separated longitudinal structure function FL from hydrogen and deuterium targets at low Q2

Polarized Proton Structure in the Resonance Region

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