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Measurement of the Ar(e,e^prime p) and Ti(e,e^prime p) cross sections in Jefferson Lab Hall A

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arxiv 2012.11466 v2 pith:U7BBQMKL submitted 2020-12-21 nucl-ex nucl-th

Measurement of the Ar(e,e^prime p) and Ti(e,e^prime p) cross sections in Jefferson Lab Hall A

L. Gu , D. Abrams , A. M. Ankowski , L. Jiang , B. Aljawrneh , S. Alsalmi , J. Bane , A. Batz
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S. Barcus M. Barroso O. Benhar V. Bellini J. Bericic D. Biswas A. Camsonne J. Castellanos J.-P. Chen M. E. Christy K. Craycraft R. Cruz-Torres H. Dai D. Day S.-C. Dusa E. Fuchey T. Gautam C. Giusti J. Gomez C. Gu T. Hague J.-O. Hansen F. Hauenstein D. W. Higinbotham C. Hyde C. Keppel S. Li R. Lindgren H. Liu C. Mariani R. E. McClellan D. Meekins R. Michaels M. Mihovilovic M. Murphy D. Nguyen M. Nycz L. Ou B. Pandey V. Pandey K. Park G. Perera A. J. R. Puckett S. N. Santiesteban S. \v{S}irca T. Su L. Tang Y. Tian N. Ton B. Wojtsekhowski S. Wood Z. Ye J. Zhang (The Jefferson Lab Hall A Collaboration)
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The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scattering data (e,e$^\prime$p) in parallel kinematics using natural argon and natural titanium targets. Here, we report the first results of the analysis of the data set corresponding to beam energy of 2,222 MeV, electron scattering angle 21.5 deg, and proton emission angle -50 deg. The differential cross sections, measured with $\sim$4% uncertainty, have been studied as a function of missing energy and missing momentum, and compared to the results of Monte Carlo simulations, obtained from a model based on the Distorted Wave Impulse Approximation.

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