Session

Unexplored ideas for ALICE, ATLAS, CMS and LHCb

6 Jul 2021, 14:30

Conveners

Unexplored ideas for ALICE, ATLAS, CMS and LHCb: Block A (Europe / US East)

  • Kristin Lohwasser (University of Sheffield (GB))
  • Jan Fiete Grosse-Oetringhaus (CERN)

Unexplored ideas for ALICE, ATLAS, CMS and LHCb: Block B (US West / Asia)

  • Stathes Paganis (National Taiwan University)
  • Alberto Belloni (University of Maryland (US))

Presentation materials

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  1. Offshell Organisers
    06/07/2021, 14:30
    Admin
  2. Laura Reina (Florida State University (US)), Nathaniel Craig, Nathaniel Craig (UC Santa Barbara), Nathaniel Craig (Stanford University)
    06/07/2021, 14:40
    Keynote

    title to be confirmed

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  3. 06/07/2021, 15:30
    Admin
  4. Karolos Potamianos (University of Oxford (GB))
    06/07/2021, 15:35
    EPJC track

    The production of two same-sign W bosons in association with two jets via vector boson scattering (VBS), ssWWjj, is a key probe of the mechanism of electroweak symmetry breaking, with the Higgs boson unitarising the process' cross-section. Longitu­dinal ssWWjj involves the spin­-0 modes of the gauge bosons arising from EWSB, and is very sensitive to BSM physics.

    With the Run-2 and Run-3...

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  5. Diego Martinez Santos (Universidade de Santiago de Compostela (ES)), Carlos Vazquez Sierra (CERN)
    06/07/2021, 16:05
    EPJC track

    A mechanism accommodating baryonic Dark Matter (DM) has been proposed recently [arXiv:2101.02706,arXiv:1810.00880]. This has the advantage of explaining matter-anti-matter imbalance and DM at once, without requiring the proton to be unstable. The DM particles, carrying baryon number, would be produced in $b$-hadron decays, through a t-channel mediator. In this model, $b$-hadron branching...

    Go to contribution page
  6. Claire Antel (Universite de Geneve (CH))
    06/07/2021, 16:35
    Keynote

    The ATLAS experiment has been in successful operation at the Large Hadron Collider (LHC) since 2009, collecting data from proton-proton collisions of up to $\sqrt{s}$ = 13 TeV. It is now gearing up to collect its majority of data at the high luminosity LHC. For this, upgrades are underway to face the challenge of a significant increase in number of interactions per bunch-crossing (pile-up),...

    Go to contribution page
  7. Gabriele Ferretti (Chalmers University, Gothenburg, Sweden), Tom Flacke (IBS CTPU Daejeon, Korea), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)
    06/07/2021, 17:20
    EPJC track
  8. 07/07/2021, 00:30
    Admin
  9. Nathaniel Craig, Nathaniel Craig (UC Santa Barbara), Nathaniel Craig (Stanford University), Laura Reina (Florida State University (US))
    07/07/2021, 00:40
    Keynote
  10. 07/07/2021, 01:30
    Admin
  11. Karolos Potamianos (University of Oxford (GB))
    07/07/2021, 01:35
    EPJC track

    The production of two same-sign W bosons in association with two jets via vector boson scattering (VBS), ssWWjj, is a key probe of the mechanism of electroweak symmetry breaking, with the Higgs boson unitarising the process' cross-section. Longitu­dinal ssWWjj involves the spin­-0 modes of the gauge bosons arising from EWSB, and is very sensitive to BSM physics.

    With the Run-2 and Run-3...

    Go to contribution page
  12. Diego Martinez Santos (Universidade de Santiago de Compostela (ES)), Carlos Vazquez Sierra (CERN)
    07/07/2021, 02:05
    EPJC track

    A mechanism accommodating baryonic Dark Matter (DM) has been proposed recently [arXiv:2101.02706,arXiv:1810.00880]. This has the advantage of explaining matter-anti-matter imbalance and DM at once, without requiring the proton to be unstable. The DM particles, carrying baryon number, would be produced in $b$-hadron decays, through a t-channel mediator. In this model, $b$-hadron branching...

    Go to contribution page
  13. Claire Antel (Universite de Geneve (CH))
    07/07/2021, 02:35
    Keynote

    The ATLAS experiment has been in successful operation at the Large Hadron Collider (LHC) since 2009, collecting data from proton-proton collisions of up to $\sqrt{s}$ = 13 TeV. It is now gearing up to collect its majority of data at the high luminosity LHC. For this, upgrades are underway to face the challenge of a significant increase in number of interactions per bunch-crossing (pile-up),...

    Go to contribution page
  14. Tom Flacke (IBS CTPU Daejeon, Korea), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)
    07/07/2021, 03:20
    EPJC track
  15. Giancarlo Panizzo (INFN Gruppo collegato di Udine), Simone Amoroso (Deutsches Elektronen-Synchrotron (DE)), Marco Zaro (Università degli Studi e INFN Milano (IT)), Davide Pagani (Deutsches Elektronen-Synchrotron (DE))
    EPJC track
  16. Davide Pagani (Deutsches Elektronen-Synchrotron (DE)), Giancarlo Panizzo (INFN Gruppo collegato di Udine), Marco Zaro (Università degli Studi e INFN Milano (IT)), Simone Amoroso (Deutsches Elektronen-Synchrotron (DE))
    EPJC track
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