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Jiang, L.; Ankowski, A. M.; Abrams, D.; Gu, L.; Aljawrneh, B.; Alsalmi, S.; Bane, J.; Batz, A.; Barcus, S.; Barroso, M.; Bellini, V.; Benhar, O.; Bericic, J.; Biswas, D.; Camsonne, A.; Castellanos, J.; Chen, J.-P.; Christy, M. E.; Craycraft, K.; Cruz-Torres, R.; Dai, H.; Day, D.; Dirican, A.; Dusa, S.-C.; Fuchey, E.; Gautam, T.; Giusti, C.; Gomez, J.; Gu, C.; Hague, T. J.; Hansen, J.-O.; Hauenstein, F.; Higinbotham, D. W.; Hyde, C.; Jerzyk, Z.; Johnson, A. M.; Keppel, C.; Lanham, C.; Li, S.; Lindgren, R.; Liu, H.; Mariani, C.; McClellan, R. E.; Meekins, D.; Michaels, R.; Mihovilovic, M.; Murphy, M.; Nguyen, D.; Nycz, M.; Ou, L.; Pandey, B.; Pandey, V.; Park, K.; Perera, G.; Puckett, A. J. R.; Santiesteban, S. N.; Širca, S.; Su, T.; Tang, L.; Tian, Y.; Ton, N.; Wojtsekhowski, B.; Wood, S.; Ye, Z.; Zhang, J.
Physical review. D, 01/2023, Volume: 107, Issue: 1Journal Article
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has measured the (e, e'p) cross section in parallel kinematics using a natural titanium target. In this paper, we report the analysis of the dataset obtained in different kinematics for our solid natural titanium target. Data were obtained in a range of missing momentum and missing energy between 15 ≲ pm ≲ 250 MeV / c and 12 ≲ Em ≲ 80 MeV, respectively, and using an electron beam energy of 2.2 GeV. We measured the reduced cross section with ~7% accuracy as a function of both missing momentum and missing energy. Furthermore, our Monte Carlo simulation, including both a model spectral function and the effects of final-state interactions, satisfactorily reproduces the data.
