no code implementations • 21 Dec 2020 • E. P. Segarra, T. Ježo, A. Accardi, P. Duwentäster, O. Hen, T. J. Hobbs, C. Keppel, M. Klasen, K. Kovařík, A. Kusina, J. G. Morfín, K. F. Muzakka, F. I. Olness, I. Schienbein, J. Y. Yu
We use the nCTEQ analysis framework to investigate nuclear Parton Distribution Functions (nPDFs) in the region of large x and intermediate-to-low $Q$, with special attention to recent JLab Deep Inelastic Scattering data on nuclear targets.
High Energy Physics - Phenomenology Nuclear Theory
no code implementations • 9 Sep 2020 • L. Alvarez-Ruso, A. M. Ankowski, M. Sajjad Athar, C. Bronner, L. Cremonesi, K. Duffy, S. Dytman, A. Friedland, A. P. Furmanski, K. Gallmeister, S. Gardiner, W. T. Giele, N. Jachowicz, H. Haider, M. Kabirnezhad, T. Katori, A. S. Kronfeld, S. W. Li, J. G. Morfín, U. Mosel, M. Muether, A. Norrick, J. Paley, V. Pandey, R. Petti, L. Pickering, B. J. Ramson, M. H. Reno, T. Sato, J. T. Sobczyk, J. Wolcott, C. Wret, T. Yang
In neutrino interactions with nucleons and nuclei, Shallow Inelastic Scattering (SIS) refers to processes, dominated by non-resonant contributions, in the kinematic region where $Q^2$ is small and the invariant mass of the hadronic system, $W$, is above the pion production threshold.
High Energy Physics - Experiment Nuclear Experiment
