- Main
Comparing proton momentum distributions in A = 2 and 3 nuclei via 2H 3H and 3He (e,e′p) measurements
- Collaboration, Jefferson Lab Hall A Tritium;
- 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 Ayerbe;
- Bai, 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, EO;
- Covrig, S;
- Craycraft, K;
- Dongwi, B;
- Duer, M;
- Duran, B;
- Dutta, D;
- Fuchey, E;
- Gal, C;
- Gautam, TN;
- Gilad, S;
- Gnanvo, K;
- Gogami, T;
- Gomez, J;
- Gu, C;
- Habarakada, A;
- Hague, T;
- Hansen, O;
- Hattawy, M;
- Hen, O;
- Higinbotham, DW;
- Hughes, E;
- Hyde, C;
- Ibrahim, H;
- Jian, S;
- Joosten, S;
- Karki, A;
- Karki, B;
- Katramatou, AT;
- 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, LE;
- Markowitz, P;
- McClellan, RE;
- Meekins, D;
- Beck, S Mey-Tal;
- Meziani, Z-E;
- Michaels, R;
- Mihovilovič, 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, GG;
- Piasetzky, E;
- Pomatsalyuk, R;
- Premathilake, S;
- Puckett, AJR;
- Punjabi, V;
- Ransome, R;
- Rashad, MNH;
- Reimer, PE;
- Riordan, S;
- Roche, J;
- Sammarruca, F;
- Santiesteban, N;
- Sawatzky, B;
- Segarra, EP;
- Schmookler, B;
- Shahinyan, A;
- Širca, S;
- Sparveris, N;
- Su, T;
- Suleiman, R;
- Szumila-Vance, H;
- Tadepalli, AS;
- Tang, L;
- Tireman, W;
- Tortorici, F;
- Urciuoli, G;
- Viviani, M;
- Weinstein, LB;
- Wojtsekhowski, B;
- Wood, S;
- Ye, ZH;
- Ye, ZY;
- Zhang, J
- et al.
Published Web Location
https://doi.org/10.1016/j.physletb.2019.134890Abstract
We report the first measurement of the (e,e′p) reaction cross-section ratios for Helium-3 (He3), Tritium (H3), and Deuterium (d). The measurement covered a missing momentum range of 40≤pmiss≤550MeV/c, at large momentum transfer (〈Q2〉≈1.9 (GeV/c)2) and xB>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 He3/d and H3/d extend to just above the typical nucleon Fermi-momentum (kF≈250 MeV/c) and differ from each other by ∼20%, while for He3/H3 they agree within the measurement accuracy of about 3%. At momenta above kF, the measured He3/H3 ratios differ from the calculation by 20%−50%. Final state interaction (FSI) calculations using the generalized Eikonal Approximation indicate that FSI should change the He3/H3 cross-section ratio for this measurement by less than 5%. If these calculations are correct, then the differences at large missing momenta between the He3/H3 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.
Main Content
Enter the password to open this PDF file:
-
-
-
-
-
-
-
-
-
-
-
-
-
-