28 August 2024
Europe/Zurich timezone

Contribution List

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  1. Daniel Schulte (CERN), Rebecca Taylor (CERN)
    28/08/2024, 14:00
  2. Carissa Joyce Cesarotti (Massachusetts Inst. of Technology (US))
    28/08/2024, 14:15
  3. Daniele Calzolari (Universita e INFN, Padova (IT))
    28/08/2024, 14:40

    Proton Driver, Target & Front-End

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  4. Bernd Michael Stechauner (Vienna University of Technology (AT))
    28/08/2024, 14:55

    6D and Final Cooling

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  5. David Amorim (CERN)
    28/08/2024, 15:10
  6. Marion Vanwelde
    28/08/2024, 15:25
  7. Giuseppe Scarantino (University of Rome "La Sapienza")
    28/08/2024, 15:40
  8. Kiley Elizabeth Kennedy (Princeton University (US))
    28/08/2024, 15:55
  9. Luca Bottura (CERN), Donatella Lucchesi (Universita e INFN, Padova (IT)), Daniel Schulte (CERN)
    28/08/2024, 16:20
  10. Lisa Soubirou
    28/08/2024, 17:35

    Reaching collision energy in a matter of milliseconds is a key challenge for the high-energy acceleration chain. The baseline is to use a chain of pulsed synchrotrons including hybrid synchrotrons, a never-operated configuration, that allows working with a more compact machine. Because of the very fast acceleration, we have to distribute the radiofrequency cavities (the acceleration stations)...

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  11. Katherine Fraser (Harvard University)
    28/08/2024, 17:45

    The strongest current bounds on lepton flavor violation (LFV) come primarily from low energy precision observables. While these experiments are expected to improve substantially in the next decade, there are cases where a muon collider could complement existing searches. In this talk, we utilize a SMEFT approach to explore the complementarity of muon colliders with low energy experiments for...

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  12. Dr Yang Ma (INFN Bologna)
    28/08/2024, 17:55

    As a potential energy frontier machine, a multi-TeV muon collider presents a vast array of physics opportunities, ranging from Higgs and top quark production to W/Z factories, jet studies, and neutrino sources. At energies far exceeding the electroweak scale, radiation effects become crucial and demand careful consideration. I will introduce the electroweak parton framework for high-energy...

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  13. Angira Rastogi (Lawrence Berkeley National Lab. (US))
    28/08/2024, 18:05

    The muon collider stands as one of the most promising prospects for next-generation high-energy particle physics experiments. However, it presents significant challenges, particularly in managing the beam-induced background (BIB) resulting from various muon decay sources. Currently, several mitigation strategies are under investigation, such as leveraging timing information from the innermost...

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  14. Maximilian Loeschner
    28/08/2024, 18:15

    BSM theories extending the Standard Model gauge group are well motivated by grand unification, compositeness or flavor symmetries, and naturally introduce additional gauge bosons. Existing experimental bounds coming from LHC exclude the existence of an additional neutral gauge boson Z' with masses of up to about 5 TeV, depending on the model. The reach could be extended at future lepton...

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  15. Federico Nardi (Universita e INFN, Padova (IT) - LPC Clermont), Shahzaib Abbas (University Of Karachi)
    28/08/2024, 18:25

    In the context of design studies for a new experimental setup, automatic differentiation can play
    an important role in helping to find the optimal configuration which meets specified
    requirements. Setting up a differential pipeline that is able to condensate experimental
    information into a loss, which is subsequently minimized, allows a global approach to a
    configuration study, and can...

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  16. Alexander Herrod (Ion Beam Applications)
    28/08/2024, 18:35

    A summary of the beamline for the Fermilab Muon g-2 Experiment (E989) is presented. Particular focus is given to post-target elements such as the liquid lithium lens, along with momentum-cooling wedges in high-dispersion areas and a brief description of how the experiment storage ring has been optimised over multiple experiments since 1959.

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  17. Rebecca Taylor (CERN)
    28/08/2024, 18:50