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Gao, J.; Anderson, B.D.; Aniol, K.; Auerbach, L.; Baker, F. T.; Berthot, J.; Bertozzi, W.; Bertin, P.Y.; Bimbot, L.; Boeglin, W.; Brash, E. J.; Breton, Vincent; Breuer, H.; Burtin, E.; Calarco, J. R.; Cardman, L.; Cates, G. D.; Cavata, C.; Cc, Chang; Chen, J.-P.; Cisbani, E.; Dale, D.; Лео, Р. Де; Deur, A.; Diederich, B.; Djawotho, P.; Domingo, J.; Doyle, B.; Ducret, J.E.; Epstein, M. B.; Ewell, L.; Finn, J. M.; Fissum, Kevin; Fonvieille, H.; Frois, B.; Frullani, S.; Garibaldi, F.; Gasparian, A.; Gilad, S.; Gilman, R.; Glamazdin, A.; Glashausser, C.; Gómez, J.; Gorbenko, V.; Gorringe, T. P.; Griffioen, K. A.; Hersman, F. W.; Holmes, R.; Holtrop, M.; d’Hose, N.; Howell, C. R.; Huber, G. M.; Hyde-Wright, C. E.; Iodice, M.; Jager, C. W. de; Jaminion, S.; Jones, M.; Joo, K.; Jutier, C.; Kahl, W.; Kato, S.; Kelly, James; Kerhoas, S.; Khandaker, M.; Khayat, M.; Kino, K.; Korsh, W.; Kramer, L.; Kumar, Krishna; Kumbartzki, G.; Laveissière, G.; Leone, A.; LeRose, J.; Levchuk, L.; Liang, M.; Lindgren, R.; Liyanage, N.; Lolos, G. J.; Lourie, R. W.; Madey, R.; Maeda, K.; Malov, S.; Manley, D. M.; Margaziotis, D. J.; Markowitz, P.; Martino, J.; McCarthy, J.; McCormick, K.; McIntyre, Justin I.; Meer, R. L. J. van der; Meziani, Z. E.; Michaels, R.; Mougey, J.; Nanda, S.; Neyret, D.; Offermann, E.A.J.M.; Papandreou, Z.; Perdrisat, C. F.; Perrino, R.; Petratos, G. G.; Platchkov, S.; Pomatsalyuk, R.; Prout, D. L.; Punjabi, V.; Pussieux, T.; Qúeḿener, G.; Ransome, R. D.; Ravel, O.; Roblin, Y.; Roché, R.; Rowntree, D.; Rutledge, G.; Rutt, P. M.; Saha, A.; Saito, T.; Sarty, A. J.; Serdarevic-Offermann, A.; Smith, T.; Soldi, A.; Sorokin, P.; Souder, P. A.; Suleiman, R.; Templon, J. A.; Terasawa, T.; Todor, L.; Tsubota, H.; Ueno, Hiroaki; Ulmer, P. E.; Urciuoli, G. M.; Vernin, P.; Verst, S. Van; Vlahović, Branislav; Voskanyan, H.; Watson, J. W.; Weinstein, Lawrence; Wijesooriya, K.; Wilson, Richard; Wojtsekhowski, B.; Zainea, D. G.; Zeps, V.; Zhao, J.; Zhou, Zhengfang

doi:10.1103/physrevlett.84.3265

Cited by 69 publications

(60 citation statements)

References 21 publications

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“…[209] these wave functions have been used to analyze low Q 2 data for the 16 O(e,e ′ p) reaction [198]. These very same wave functions produce a good description of the shape of the coincidence cross section for the p-shell quasihole states at high Q 2 [259] using the same spectroscopic factors obtained from the low Q 2 data [198].…”

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

“…[258]. In this paper a study of recently published (e,e ′ p) data for 16 O at Q 2 = 0.8 (GeV/c) 2 [259] has been presented. An unfactorized approach was used, as it is required at low Q 2 [16] and as it has been recently advocated also for high Q 2 reactions in Ref.…”

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

“…In Fig. 52 the same reaction is considered in a very different kinematical regime, namely at constant (q, ω) with Q 2 = 0.8 (GeV/c) 2 [259]. The data here refer to a five-fold differential cross section, avoiding any ambiguity in modelling the half off-shell elementary cross section σ ep .…”

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

“…[258]. Figure 52: Cross section for the 16 O(e,e ′ p) 15 N reaction at Q 2 = 0.8 (GeV/c) 2 in perpendicular kinematics [259]. Data for the p1/2 state have been multiplied by 20.…”

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

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Self-consistent Green's function method for nuclei and nuclear matter

Dickhoff

Barbieri

2004

Progress in Particle and Nuclear Physics

486

599

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Recent results obtained by applying the method of self-consistent Green's functions to nuclei and nuclear matter are reviewed. Particular attention is given to the description of experimental data obtained from the (e,e ′ p) and (e,e ′ 2N) reactions that determine one and two-nucleon removal probabilities in nuclei since the corresponding amplitudes are directly related to the imaginary parts of the single-particle and two-particle propagators. For this reason and the fact that these amplitudes can now be calculated with the inclusion of all the relevant physical processes, it is useful to explore the efficacy of the method of self-consistent Green's functions in describing these experimental data. Results for both finite nuclei and nuclear matter are discussed with particular emphasis on clarifying the role of short-range correlations in determining various experimental quantities. The important role of long-range correlations in determining the structure of lowenergy correlations is also documented. For a complete understanding of nuclear phenomena it is therefore essential to include both types of physical correlations. We demonstrate that recent experimental results for these reactions combined with the reported theoretical calculations yield a very clear understanding of the properties of all protons in the nucleus. We propose that this knowledge of the properties of constituent fermions in a correlated many-body system is a unique feature of nuclear physics.

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Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

“…[258]. Figure 52: Cross section for the 16 O(e,e ′ p) 15 N reaction at Q 2 = 0.8 (GeV/c) 2 in perpendicular kinematics [259]. Data for the p1/2 state have been multiplied by 20.…”

Section: Extraction Of Spectroscopic Information Frommentioning

confidence: 99%

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Self-consistent Green's function method for nuclei and nuclear matter

Dickhoff

Barbieri

2004

Progress in Particle and Nuclear Physics

486

599

View full text Add to dashboard Cite

show abstract

“…[25] to give the same results as the relativistic Fermi gas for the electromagnetic inclusive responses in nuclear matter. Moreover, the present model was compared in [26] with a fully relativistic DWIA model of the reaction for |Q 2 | = 0.8 (GeV/c) 2 , giving a reasonable description of the A T L asymmetries recently measured in 16 O [27].…”

Section: Introductionmentioning

confidence: 99%

Effects of short-range correlations in(e,e′p)reactions and nuclear overlap functions

2002

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A study of the effects of short-range correlations over the (e, e ′ p) reaction for low missing energy in closed shell nuclei is presented. We use correlated, quasi-hole overlap functions extracted from the asymptotic behavior of the one-body density matrix, containing central correlations of Jastrow type, up to first-order in a cluster expansion, and computed in the very high asymptotic region, up to 100 fm. The method to extract the overlap functions is checked in a simple shell model, where the exact results are known. We find that the single-particle wave functions of the valence shells are shifted to the right due to the short-range repulsion by the nuclear core. The corresponding spectroscopic factors are reduced only a few percent with respect to the shell model. However, the (e, e ′ p) response functions and cross sections are enhanced in the region of the maximum of the missing momentum distribution due to short-range correlations.

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Testing the Limits of the Single Particle Model in 16O(E,E’P)

Weinstein

Electron Scattering

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Dynamical Relativistic Effects in Quasielastic1p-Shell Proton Knockout fromO16

Abstract: We have measured the cross section for quasielastic 1p-shell proton knockout in the 16O(e,e(')p) reaction at omega = 0.439 GeV and Q2 = 0.8 (GeV/c)(2) for missing momentum P(miss) Show more

Cited by 69 publications

References 21 publications

Self-consistent Green's function method for nuclei and nuclear matter

Self-consistent Green's function method for nuclei and nuclear matter

Effects of short-range correlations in(e,e′p)reactions and nuclear overlap functions

Testing the Limits of the Single Particle Model in 16O(E,E’P)

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