11-15 September 2017
Mexico/General timezone
- ismd2017@nucleares.unam.mx
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Proton structure, Small and large x physics (I)
Date:
11 Sep 14:55 - 17:00
Conveners
-
- Bruno El‐Bennich, Amir Rezaeian
- Chairperson: Bruno El-Bennich
Timetable | Contribution List
Displaying 5
contributions
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5
We present results on a study of the dynamics of the formation of
nonhomogeneous phases of the chiral transition transition in QCD.
The possibility of the formation of a spatially modulated chiral
condensate in the final stages of a heavy-ion collision is investigated
assuming a Ginzburg-Landau-Langevin time evolution, using a
free energy functional motivated by the Nambu—Jona-Lasinio
mo
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Presented by Prof. Gastao KREIN
on
11/9/2017
at
21:35
The measurements of hadronic form factors using the data samples collected with the BESIII detector at BEPCII collider are presented. The cross section of $e^+e^-\to p\bar{p}$ at 12 energies from $2232.4$ to $3671.0$ MeV are measured, the electromagnetic form factor is deduced, and the ratio $|G_{E}/G_{M}|$ is extracted by fitting the polar angle distribution. The cross section of $e^+e^-\to\pi^+\
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Presented by Prof. Haiming HU
on
11/9/2017
at
20:20
Measurements of the Drell-Yan production of $W$ and $Z/\gamma$ bosons at the LHC provide a benchmark of our understanding of perturbative QCD and probe the proton structure in a unique way. The ATLAS collaboration has performed new high precision measurements at center-of-mass energies of 7 TeV. The measurements are performed for $W^+$, $W^-$ and $Z/\gamma$ bosons integrated and as a function of t
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Presented by Alessandro LAPERTOSA
on
11/9/2017
at
19:55
Meson photoproduction is an important tool in the study of baryon resonances. The spectrum of broad and overlapping nucleon excitations can be greatly clarified by use of polarization observables. The N* program at Jefferson Lab with the CEBAF Large Acceptance Spectrometer (CLAS) includes experimental studies with linearly- and circularly-polarized tagged-photon beams, longitudinally- and transver
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Presented by Prof. Steffen STRAUCH
on
11/9/2017
at
21:10
I discuss the fragmentation region at very high energies. Due to the mismatch of
the saturation momenta of the target
and projectile, there is a parametric difference between the energy density and
multiplicity density of produced particles
dependence upon saturation momenta. This parametric difference allows one to
discriminate between thermalized and
non-thermalized systems by measuring
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Presented by Prof. Larry MCLERRAN
on
11/9/2017
at
20:45