학술논문

Comparing proton momentum distributions in $A=2$ and 3 nuclei via $^2$H $^3$H and $^3$He $(e, e'p)$ measurements
Document Type
Working Paper
Author
Cruz-Torres, R.Li, S.Hauenstein, F.Schmidt, A.Nguyen, D.Abrams, D.Albataineh, H.Alsalmi, S.Androic, D.Aniol, K.Armstrong, W.Arrington, J.Atac, H.Averett, T.Gayoso, C. AyerbeBai, X.Bane, J.Barcus, S.Beck, A.Bellini, V.Bhatt, H.Bhetuwal, D.Biswas, D.Blyth, D.Boeglin, W.Bulumulla, D.Camsonne, A.Castellanos, J.Chen, J. -P.Cohen, E. O.Covrig, S.Craycraft, K.Dongwi, B.Duer, M.Duran, B.Dutta, D.Fuchey, E.Gal, C.Gautam, T. N.Gilad, S.Gnanvo, K.Gogami, T.Gomez, J.Gu, C.Habarakada, A.Hague, T.Hansen, O.Hattawy, M.Hen, O.Higinbotham, D. W.Hughes, E.Hyde, C.Ibrahim, H.Jian, S.Joosten, S.Karki, A.Karki, B.Katramatou, A. T.Keppel, C.Khachatryan, M.Khachatryan, V.Khanal, A.King, D.King, P.Korover, I.Kutz, T.Lashley-Colthirst, N.Laskaris, G.Li, W.Liu, H.Liyanage, N.Lonardoni, D.Machleidt, R.Marcucci, L. E.Markowitz, P.McClellan, R. E.Meekins, D.Beck, S. Mey-TalMeziani, Z. -E.Michaels, R.Mihovilovic, M.Nelyubin, V.Nuruzzaman, N.Nycz, M.Obrecht, R.Olson, M.Ou, L.Owen, V.Pandey, B.Pandey, V.Papadopoulou, A.Park, S.Patsyuk, M.Paul, S.Petratos, G. G.Piasetzky, E.Pomatsalyuk, R.Premathilake, S.Puckett, A. J. R.Punjabi, V.Ransome, R.Rashad, M. N. H.Reimer, P. E.Riordan, S.Roche, J.Sammarruca, F.Santiesteban, N.Sawatzky, B.Segarra, E. P.Schmookler, B.Shahinyan, A.Širch, S.Sparveris, N.Su, T.Suleiman, R.Szumila-Vance, H.Tadepalli, A. S.Tang, L.Tireman, W.Tortorici, F.Urciuoli, G.Viviani, M.Weinstein, L. B.Wojtsekhowski, B.Wood, S.Ye, Z. H.Ye, Z. Y.Zhang, J.
Source
Physics Letters B 797 (2019) 134890
Subject
Nuclear Experiment
Nuclear Theory
Language
Abstract
We report the first measurement of the $(e,e'p)$ reaction cross-section ratios for Helium-3 ($^3$He), Tritium ($^3$H), and Deuterium ($d$). The measurement covered a missing momentum range of $40 \le p_{miss} \le 550$ MeV$/c$, at large momentum transfer ($\langle Q^2 \rangle \approx 1.9$ (GeV$/c$)$^2$) and $x_B>1$, which minimized contributions from non quasi-elastic (QE) reaction mechanisms. The data is compared with plane-wave impulse approximation (PWIA) calculations using realistic spectral functions and momentum distributions. The measured and PWIA-calculated cross-section ratios for $^3$He$/d$ and $^3$H$/d$ extend to just above the typical nucleon Fermi-momentum ($k_F \approx 250$ MeV$/c$) and differ from each other by $\sim 20\%$, while for $^3$He/$^3$H they agree within the measurement accuracy of about 3\%. At momenta above $k_F$, the measured $^3$He/$^3$H ratios differ from the calculation by $20\% - 50\%$. Final state interaction (FSI) calculations using the generalized Eikonal Approximation indicate that FSI should change the $^3$He/$^3$H cross-section ratio for this measurement by less than 5\%. If these calculations are correct, then the differences at large missing momenta between the $^3$He/$^3$H experimental and calculated ratios could be due to the underlying $NN$ interaction, and thus could provide new constraints on the previously loosely-constrained short-distance parts of the $NN$ interaction.
Comment: 8 pages, 3 figures (4 panels)