Barak Schmookler
(UCR),
Barak Schmookler
(UC Riverside)
7/18/22, 11:00 AM
Zachary Sweger
(University of California, Davis)
7/19/22, 9:20 AM
Barak Schmookler
(UCR),
Barak Schmookler
(UC Riverside)
7/19/22, 10:00 AM
Wai Kin Lai
(University of California, Los Angeles)
7/19/22, 11:00 AM
Ryan Milton
(UCLA)
7/19/22, 2:30 PM
Bishnu Karki
(University of California, Riverside)
7/19/22, 2:50 PM
Miguel Rodriguez
(UCR)
7/19/22, 3:10 PM
JiaJun Huang
(UCR)
7/19/22, 3:20 PM
Luis Garabito
(lgara004@ucr.edu)
7/19/22, 3:30 PM
Grace Gamire
(Cal Poly SLO/UCLA)
7/19/22, 3:40 PM
Ananya Paul
(University of California, Riverside)
7/19/22, 3:50 PM
Sean Preins
(University of California, Riverside)
7/19/22, 4:00 PM
Owen Long
(UCLA)
7/19/22, 4:40 PM
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...