from 28 November 2016 to 2 December 2016
Hotel Rincón del Arco
Mexico/General timezone
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WG1

Place

Location: Hotel Rincón del Arco
Room: Salón Giralda
Date: from 28 Nov 10:00 to 1 Dec 17:50

Conveners

  • 28 Nov 10:00 - 10:50
    • Kumar, Ramandeep (Panjab)
    • Dr. Kar, Deepak (TU Dresden)
  • 28 Nov 11:20 - 13:00 WG1
    • Kumar, Ramandeep (Panjab)
    • Dr. Kar, Deepak (TU Dresden)
  • 1 Dec 17:00 - 17:50 WG1
    • Kumar, Ramandeep (Panjab)
    • Dr. Kar, Deepak (TU Dresden)

Timetable | Contribution List

Displaying 10 contributions out of 10
Session: WG1
Different distributions of charged-particles and leading charged-particle produced in proton-proton collisions at a centre-of-mass energy $\sqrt{s} = 13$ TeV are measured in the pseudorapidity range $|\eta| < 2.4$ for charged-particles with a transverse momentum $p_T~>~0.5$ GeV. Measurements are presented for four event categories. The first two categories correspond to inclusive and inelastic e ... More
Presented by Mr. Juan Manuel GRADOS LUYANDO on 28/11/2016 at 12:00
Session: WG1
Recent measurements, performed with the CMS and TOTEM experiments, of the elastic and inelastic cross section are presented and compared. The inelastic cross section at 13 TeV is measured with CMS in two fiducial regions using information from forward calorimetry, and finally extrapolated to the full inelastic phase space.
Presented by Kumar RAMANDEEP, Juan Manuel GRADOS LUYANDO on 1/12/2016 at 23:00
Session: WG1
Presented by Dr. Deepak KAR
Session: WG1
Presented by Dr. Deepak KAR on 28/11/2016 at 16:00
Session: WG1
The modelling of Minimum Bias (MB) is a crucial ingredient to learn about the description of soft QCD processes. It has also a significant relevance for the simulation of the environment at the LHC with many concurrent pp interactions (“pileup”). The ATLAS collaboration has provided new measurements of the inclusive charged particle multiplicity and its dependence on transverse momentum ... More
Presented by Jiri KVITA on 28/11/2016 at 11:40
Session: WG1
The modelling of the Underlying Event (UE) is a crucial component in the complete description of both soft and hard QCD processes at hadron colliders. The ATLAS collaboration presents new results on the number and transversemomentum sum of charged particles as a function of the leading high pT track in events taken at a center of mass energy of 13 TeV. These results are presented in regions t ... More
Presented by Robert ASTALOS on 28/11/2016 at 16:30
Session: WG1
We present results on the measurement of the underlying event at 13 TeV using leading tracks, jets, and Drell-Yan processes. In addition measurements of forward-backward particle correlations and the rapidity gap fraction are presented. Finally results on charged particle multiplicity and transverse momenta distributions are shown.
Presented by Mr. Juan Manuel GRADOS LUYANDO on 28/11/2016 at 18:20
Session: WG1
Presented by Dr. Deepak KAR on 1/12/2016 at 23:20
Session: WG1
By measuring the substructure of a jet, one can assign it a quark or gluon tag. In this talk, we confront the challenges faced when going beyond this leading-order understanding, using both parton shower generators and first-principles calculations to assess the impact of higher-order perturbative and nonperturbative physics. Working in the idealized context of electron-positron collisions,where ... More
Presented by Dr. Deepak KAR on 28/11/2016 at 12:40
Session: WG1
Underlying-event activity is defined as the soft particle production in proton+proton collisions which is not directly related to the final fragmentation of hard-scattered partons. Underlying-event measurements therefore provide a tool to study non-factorizable and non-perturbative phenomena. Systematic measurements of the relationship between the underlying event and jet processes provide a cruci ... More
Presented by Dr. Li YI on 28/11/2016 at 11:20
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