Event calendar file
11-15 September 2017
Mexico/General timezone
- ismd2017@nucleares.unam.mx
Support
Forward physics and diffraction (I)
Date:
14 Sep 14:45 - 16:25
Conveners
-
- Martin Hentschinski, Christophe Royon
- Chairperson: Christophe Royon
Timetable | Contribution List
Displaying 4
contributions
out of
4
Session:
Forward physics and diffraction (I)
Diffractive phenomena at the LHC are being studied by several collaborations at CERN. In this paper we present our recent results on the deviation from the exponential behavior in elastic proton-proton scattering at low |t| as well as central exclusive resonance production. Although the above phenomena occur in different kinematical regions, they are related e.g. by Regge-factorization.
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Presented by Prof. Laszlo JENKVOSZKY
on
14/9/2017
at
21:00
Session:
Forward physics and diffraction (I)
The exclusive photoproduction of upsilon states is investigated in the context of ultra-peripheral collisions at the LHC energies. Predictions are presented for their production in proton-proton, proton-nucleus and nucleus-nucleus collision at the energies available at the LHC run 2. The theoretical framework considered in the analysis is the light-cone color dipole formalism, which includes consi
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Presented by Dr. Magno MACHADO
on
14/9/2017
at
19:45
Session:
Forward physics and diffraction (I)
One of the main goals of the Large Hadron Collider is to find signatures of physics Beyond the Standard Model of particle physics. One way to do this is by studying with high precision the interactions of the Standard Model. In this talk, we address the discovery potential of New Physics in the exclusive channel pp $\rightarrow$ p X p which relies on the general purpose detectors at the Large Hadr
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Presented by Cristian BALDENEGRO BARRERA
on
14/9/2017
at
20:10
Session:
Forward physics and diffraction (I)
We use the spinor helicity formalism to calculate the cross section for production of three partons of a given polarization in Deep Inelastic Scattering (DIS) off proton and nucleus targets at small Bjorken x. The target proton or nucleus is treated as a classical color field (shock wave) from which the produced partons scatter multiple times. The resulting expressions are used to study azimuthal
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Presented by Dr. Martin HENTSCHINSKI
on
14/9/2017
at
20:35
