- Jiang, L;
- Ankowski, AM;
- 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, ME;
- 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, TJ;
- Hansen, J-O;
- Hauenstein, F;
- Higinbotham, DW;
- Hyde, C;
- Jerzyk, Z;
- Johnson, AM;
- Keppel, C;
- Lanham, C;
- Li, S;
- Lindgren, R;
- Liu, H;
- Mariani, C;
- McClellan, RE;
- Meekins, D;
- Michaels, R;
- Mihovilovic, M;
- Murphy, M;
- Nguyen, D;
- Nycz, M;
- Ou, L;
- Pandey, B;
- Pandey, V;
- Park, K;
- Perera, G;
- Puckett, AJR;
- Santiesteban, SN;
- Širca, S;
- Su, T;
- Tang, L;
- Tian, Y;
- Ton, N;
- Wojtsekhowski, B;
- Wood, S;
- Ye, Z;
- Zhang, J
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. Our Monte Carlo simulation, including both a model spectral function and the effects of final-state interactions, satisfactorily reproduces the data.
