Benjamin Michael Wynne
(University of Edinburgh (GB))
16/09/2015, 09:15
Sanjay Kumar Swain
(National Institute of Science Education and Research (IN))
16/09/2015, 09:50
Katarzyna Wichmann
(Deutsches Elektronen-Synchrotron Hamburg and Zeuthen (DE))
16/09/2015, 10:25
Gagan Mohanty
(Tata Inst. of Fundamental Research (IN))
16/09/2015, 11:30
Veronique Boisvert
(Royal Holloway, University of London)
16/09/2015, 12:00
Finn O'Neill Rebassoo
(Lawrence Livermore Nat. Laboratory (US))
16/09/2015, 13:45
Nicolas Pierre Chanon
(Institut Pluridisciplinaire Hubert Curien (FR))
16/09/2015, 14:55
Constantinos Loizides
(Lawrence Berkeley National Lab. (US))
17/09/2015, 08:45
Thomas Nikodem
(Ruprecht-Karls-Universitaet Heidelberg (DE))
17/09/2015, 09:25
Gagan Mohanty
(Tata Inst. of Fundamental Research (IN))
17/09/2015, 10:00
James Libby
(Indian Institute of Technology Madras)
17/09/2015, 11:40
Joseph Haley
(Oklahoma State University (US))
17/09/2015, 17:20
Mark Lancaster
(University College London (UK))
18/09/2015, 08:30
Justyna Lagoda
(National Centre for Nuclear Research (PL))
18/09/2015, 09:05
Andrea Pocar
(University of Massachusetts, Amherst)
18/09/2015, 11:10
Ignacy Leonard Sawicki
(University of Geneva),
Ignacy Sawicki
18/09/2015, 11:45
Matteo Duranti
(Universita e INFN, Perugia (IT)),
Vitaly Choutko
(Massachusetts Inst. of Technology (US))
19/09/2015, 09:35
Julian Rautenberg
(Bergische Universität Wuppertal)
19/09/2015, 10:10
Arno Straessner
(Technische Universitaet Dresden (DE))
The ATLAS detector was designed and built to study proton-proton
collisions produced at the LHC at centre-of-mass energies up to 14 TeV
and instantaneous luminosities up to
$10^{34}~\mathrm{cm^{-2}s^{-1}}$. Liquid argon (LAr) sampling
calorimeters are employed for all electromagnetic calorimetry in the
pseudorapidity region $|\eta|<3.2$, and for hadronic calorimetry in
the region from...
Mengqing Wu
(Centre National de la Recherche Scientifique (FR))
The poster will give an overview of the dark matter searches in ATLAS based on the presence of a high pT object accompanied by large missing transverse momentum. LHC Run-1 results at a centre-of-mass energy of 8 TeV will be shown along with prospects for the ongoing LHC Run-2, including relevant performance studies based on the 13 TeV data.
Dr
Fatemighomi Nasim
(Royal Holloway University of London)
DEAP-3600 is a single phase liquid argon (LAr) dark matter experiment, located 2 km underground at SNOLAB, in Sudbury, Ontario. The detector has 1 tonne fiducial mass of LAr. The target sensitivity to spin-independent scattering of 100 GeV WIMPs is 10$^{-46}$ cm$^{2}$ which gives one order of magnitude improvement over current results. The DEAP-3600 background target is < 1 background...
ALESSANDRA LUCA'
(INFN - National Institute for Nuclear Physics)
The production of photons with large transverse energy in hadronic
collisions is an important testing ground for perturbative Quantum
Chromodynamics (pQCD), enabling to probe parton distribution functions
(PDFs) and the parton-to-photon fragmentation functions (FFs). In
addition, high-ET photons can also constitute an irreducible background
for important searches such as H→γγ, or...
Mr
Arthur Lesage
(CEA/IRFU,Centre d'etude de Saclay Gif-sur-Yvette (FR))
The ATLAS muon reconstruction has been improved for the Run-II of the LHC.
In this presentation, we will discuss the new reconstruction algorithm and its performance
as measured during the early run of the LHC in 2015 at sqrt(s)= 13 TeV
using samples of J/ψ→μμ and Z→μμ decays.
Reconstruction efficiency, transverse momentum resolution and momentum scales are
measured in the various...
Michael David Beattie
(Lancaster University (GB))
The differential cross sections for prompt and non-prompt production
of psi(2S) and X(3872) is measured in the J/psi pi+ pi- decay mode in
pp collisions at sqrt(s)= 8 TeV, using the integrated luminosity of
11.4 fb-1 taken by the ATLAS detector. The non-prompt fraction of
X(3872) production and the ratio of X(3872) and psi(2S) production
cross sections are also measured. Results are...
Annika Vanhoefer
(Hamburg University (DE))
The direct search for the Higgs boson Lepton Flavour Violating decay H -> e tau_mu in the 19.7/fb proton-proton collisions data collected with the CMS detector at 8 TeV centre-of-mass energy is presented. The observed (expected) limit on the Higgs boson branching fraction is discussed and compared with the H-> mu tau_e and H -> e mu Lepton Flavour Violating decay modes.
Joseph Stanford Ennis
(University of Warwick (GB))
Many extensions to the Standard Model predict new particles which couple to the electroweak bosons. Using recently developed jet substructure techniques it is possible to tag jets consistent with hadronically decaying bosons whilst rejecting the QCD background. Studying the all-hadronic final state with this strategy was used in run-1 to perform a search for new high mass resonances. This...
Paolo Franchini
(Universita e INFN, Bologna (IT))
Muon beams of low emittance provide the basis for the intense, well characterised, neutrino beams necessary to elucidate the physics of flavour at the Neutrino Factory and to provide lepton-antilepton collisions up to several TeV at the Muon Collider. The international Muon Ionization Cooling Experiment (MICE) will demonstrate ionization cooling, the technique proposed to reduce the...
Francois Elie Rene Drielsma
(Universite de Geneve (CH))
Muon beams of low emittance provide the basis for the intense, well-characterised neutrino beams of the Neutrino Factory and for lepton-antilepton collisions at energies of up to several TeV at the Muon Collider. The International Muon Ionization Cooling Experiment (MICE) will demonstrate ionization cooling – the technique by which it is proposed to reduce the µ phase-space volume. MICE is...
Ms
Deepanjali Goswami
(Indian Institute of Technology Guwahati)
We investigated the signature of heavy fermionic triplets belonging to Type III seesaw model through their direct production at the International Linear Collider (ILC). In particular we looked into the decay distributions of charged ($\Sigma^{\pm}$) and neutral ($\Sigma^{0}$) triplets in the processes $e^{+} e^{-} \rightarrow \Sigma^{+}\Sigma^{-}, \Sigma^{0} \Sigma^{0}, \Sigma^{0}\nu,...
