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16/09/2015, 09:00
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Benjamin Michael Wynne (University of Edinburgh (GB))16/09/2015, 09:15
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Sanjay Kumar Swain (National Institute of Science Education and Research (IN))16/09/2015, 09:50
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Katarzyna Wichmann (Deutsches Elektronen-Synchrotron Hamburg and Zeuthen (DE))16/09/2015, 10:25
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Gagan Mohanty (Tata Inst. of Fundamental Research (IN))16/09/2015, 11:30
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Veronique Boisvert (Royal Holloway, University of London)16/09/2015, 12:00
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Finn O'Neill Rebassoo (Lawrence Livermore Nat. Laboratory (US))16/09/2015, 13:45
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Nils Ruthmann (CERN)16/09/2015, 14:20
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Nicolas Pierre Chanon (Institut Pluridisciplinaire Hubert Curien (FR))16/09/2015, 14:55
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Jahred Adelman (Northern Illinois University)16/09/2015, 15:30
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Constantinos Loizides (Lawrence Berkeley National Lab. (US))17/09/2015, 08:45
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Thomas Nikodem (Ruprecht-Karls-Universitaet Heidelberg (DE))17/09/2015, 09:25
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Gagan Mohanty (Tata Inst. of Fundamental Research (IN))17/09/2015, 10:00
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Valerie Gibson (University of Cambridge (GB))17/09/2015, 11:05
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James Libby (Indian Institute of Technology Madras)17/09/2015, 11:40
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Cristina Lazzeroni (University of Birmingham (GB))17/09/2015, 12:15
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Peng Haiping17/09/2015, 13:50
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Adam West17/09/2015, 14:30
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Christine Davies (University of Glasgow)17/09/2015, 15:05
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Ken Moats17/09/2015, 16:10
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Hongxuan Liu (Baylor University (US))17/09/2015, 16:45
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Joseph Haley (Oklahoma State University (US))17/09/2015, 17:20
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Mark Lancaster (University College London (UK))18/09/2015, 08:30
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Justyna Lagoda (National Centre for Nuclear Research (PL))18/09/2015, 09:05
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Christopher Backhouse18/09/2015, 09:40
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Michael Wurm18/09/2015, 10:10
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Andrea Pocar (University of Massachusetts, Amherst)18/09/2015, 11:10
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Ignacy Leonard Sawicki (University of Geneva), Ignacy Sawicki18/09/2015, 11:45
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18/09/2015, 12:20
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David G. Cerdeno (University of Durham)19/09/2015, 09:00
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Matteo Duranti (Universita e INFN, Perugia (IT)), Vitaly Choutko (Massachusetts Inst. of Technology (US))19/09/2015, 09:35
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Julian Rautenberg (Bergische Universität Wuppertal)19/09/2015, 10:10
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Steven Gratton19/09/2015, 11:10
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Dr Biagio Rossi (INFN)19/09/2015, 11:45
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Hiroki Nagahama (University of Tokyo (JP))19/09/2015, 12:20
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19/09/2015, 12:50
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ATLAS Poster Presenter (ATLAS)In Run I, a search for high mass higgs decaying to two Z bosons has been performed in both ATLAS and CMS experiments. The search in ATLAS consists of 4 channels depending on the Z decays, llll, llvv, llqq and vvqq. This poster will mainly focus on the decay channels where one of the Z decay leptonicly and the other hadronically, meaning the vvqq and llqq channels from ATLAS. The search...Go to contribution page
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DUNE Collaboration (Fermilab)A new International Collaboration (DUNE - Deep Underground Neutrino Experiment) has been formed to pursue an accelerator-based long-baseline neutrino experiment, as well as neutrino astrophysics and nucleon decay, with an approximately 40-kt (fiducial) modular liquid argon TPC (LAr-TPC) detector located deep underground and a high-resolution near detector. Several independent worldwide...Go to contribution page
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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...Go to contribution page
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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.Go to contribution page
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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...Go to contribution page
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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...Go to contribution page
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ATLAS Poster Presenter (ATLAS)The ATLAS experiment measured the differential production cross-section of Drell-Yan lepton pairs in proton-proton collisions versus their transverse momentum and the phi* observable. These measurements allow for a precise test of perturbative and resummed QCD predictions and are the basis for electroweak precision measurements at the LHC, such as the measurement of the W boson mass. In...Go to contribution page
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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...Go to contribution page
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Iain Lamont (T2K)A study of differences in electron neutrino and muon neutrino interactions using the T2K ND280 detector will be performed in this analysis. The low peak energy of the T2K beam is ideal for studying these differences as this is the region with the largest expected difference. To cancel the large beam flux uncertainties, the ratio of the number of CCQE interactions to the number of CC inclusive...Go to contribution page
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Dr Mikhail Barabanov (JINR)The spectroscopy of exotics states with hidden charm together with the spectroscopy of charmed and strange baryons is discussed. It is a good testing tool for the theories of strong interactions, including: QCD in both the perturbative and non-perturbative regimes, LQCD, potential models and phenomenological models [1, 2, 3]. An understanding of the baryon spectrum is one of the primary goals...Go to contribution page
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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...Go to contribution page
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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.Go to contribution page
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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...Go to contribution page
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ATLAS Poster Presenter (ATLAS)In 2012, the ATLAS and CMS experiments at CERN discovered a Higgs-like boson in LHC pp collisions at √s = 7 and 8 TeV with an approximate mass of 125 GeV. More recent experimental results, exploring the complete Run1 dataset, indicate that the observed boson is consistent with the Standard Model Higgs Boson within uncertainties. The results include spin and parity properties and...Go to contribution page
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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...Go to contribution page
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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...Go to contribution page
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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,...Go to contribution page
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DUNE Collaboration (Fermilab)The Deep Underground Neutrino Experiment (DUNE) plans a 34-kton (fiducial mass) liquid argon time projection chamber to be sited at 4850 ft depth at the Sanford Underground Research Facility in South Dakota. The significant overburden at this site gives DUNE significant physics reach for several non-beam physics topics. These include neutrino oscillation studies with atmospheric neutrinos,...Go to contribution page
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