Conveners
Diffraction in nuclear collisions (I)
- Leszek Adamczyk (AGH University of Science and Tecnology)
Miguel Arratia
(ATLAS)
07/09/2016, 16:00
Diffraction in nuclear physics
The large equivalent-photon fluxes accompanying Pb ion beams at the LHC initiate photon-photon and photo-nuclear
interactions which dominate when the colliding nuclei have large impact parameter (ultra-peripheral collisions).
These electromagnetically-induced processes are sensitive to the nuclear wave-function and in particular the
nuclear modifications of the nucleon parton distribution...
Guillermo Contreras
(FJFI CVUT Prague)
07/09/2016, 16:25
Diffraction in nuclear physics
The strong electromagnetic fields generated by ultra-relativistic heavy ions offer the possibility to study photoproduction processes at the LHC. In so called ultra-peripheral collisions (UPC), when the impact
parameter of the incoming hadrons is larger than the sum of their
radii, hadronic processes are strongly suppressed and only electromagenetic interactions remain.
ALICE has...
Jaroslav Adam
(Czech Technical University in Prague, Creighton University, Omaha)
07/09/2016, 16:50
Diffraction in nuclear physics
Ultra-relativistic heavy ions generate strong electromagnetic fields, which
offer the possibility to study photon-photon, photon-nucleus and photon-proton
processes at the LHC in ultra-peripheral p-Pb and Pb-Pb collisions (UPC).
Exclusive photoproduction of vector mesons is sensitive to the gluon distribution
of the interacting target (proton or nucleus) whereas exclusive production of...
Alexander Bylinkin
(Moscow Instittue of Physics and Technology)
07/09/2016, 17:10
Diffraction in nuclear physics
Exclusive vector meson (Upsilon and Rho0) photoproduction is studied in ultra-peripheral pPb collisions at √sNN =5.02 TeV with the CMS experiment at the LHC. The cross sections are measured as a function of the photon-proton centre-of-mass energy, extending the energy range explored by H1 and ZEUS Experiments at HERA. In addition, the differential cross sections (dσ/d|t|), where|t|≈ p^2_T is...
