Barak Schmookler
(UCR),
Barak Schmookler
(UC Riverside)
18/07/2022, 11:00
Zachary Sweger
(University of California, Davis)
19/07/2022, 09:20
Barak Schmookler
(UCR),
Barak Schmookler
(UC Riverside)
19/07/2022, 10:00
Wai Kin Lai
(University of California, Los Angeles)
19/07/2022, 11:00
Ryan Milton
(UCLA)
19/07/2022, 14:30
Bishnu Karki
(University of California, Riverside)
19/07/2022, 14:50
Miguel Rodriguez
(UCR)
19/07/2022, 15:10
JiaJun Huang
(UCR)
19/07/2022, 15:20
Luis Garabito
(lgara004@ucr.edu)
19/07/2022, 15:30
Grace Gamire
(Cal Poly SLO/UCLA)
19/07/2022, 15:40
Ananya Paul
(University of California, Riverside)
19/07/2022, 15:50
Sean Preins
(University of California, Riverside)
19/07/2022, 16:00
Owen Long
(UCLA)
19/07/2022, 16:40
Zachary Sweger
(University of California, Davis)
Backward ($u$-channel) production of vector mesons in $ep$ collisions is characterized by a final state consisting of a nearly-stopped proton and a vector meson with a large forward momentum. In conventional (forward, $t$-channel) production, the momentum transfer from the proton to the meson is small and is modeled by pomeron-exchange trajectories. The less well-understood $u$-channel...
