15–21 Sept 2019
Hotel Hermitage, La Biodola Bay, Isola d'Elba, Italy
Europe/Rome timezone

Session

WG5

17 Sept 2019, 18:00
SB1 (Hotel Hermitage)

SB1

Hotel Hermitage

Presentation materials

There are no materials yet.

  1. Erik Adli (University of Oslo, Norway)
    17/09/2019, 18:00
    WG5 - Plasma devices, plasma and beam diagnostics
    talk

    The Plasma Lens Experiment at CERN is an experiment in active plasma lensing. It consists of a gas-filled sapphire capillary connected to a set of compact Marx banks, which breaks down the gas and drives a large current pulse through it. This generates a magnetic field, which is probed using the CLEAR electron beam and measured using various screens and magnetic elements behind the lens. We...

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  2. Keenan Hunt-Stone (Univ. of Colorado, USA)
    17/09/2019, 18:20
    WG5 - Plasma devices, plasma and beam diagnostics
    talk

    Future beam-driven plasma wakefield accelerator (PWFA) experiments at the Facility for Advanced Accelerator Experimental Tests (FACET-II) will require several detectors monitoring a multitude of plasma and electron bunch parameters. We present simulations demonstrating the ability of an electro-optic sampling beam position monitor (EOS-BPM) to analyze the femtosecond electron bunches that will...

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  3. Spencer Gessner (CERN)
    17/09/2019, 18:40
    WG5 - Plasma devices, plasma and beam diagnostics
    talk

    The AWAKE experiment at CERN is a proof-of-concept proton beam-driven plasma wakefield accelerator. The plasma source is a 10 meter-long Rubidium vapor cell ionized by a high-intensity laser pulse. The proton beam is modulated by the plasma, which results in micro-bunching at the plasma frequency and resonant excitation of the plasma wave. We measure the frequency of the micro-bunching when...

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  4. Michael Litos (University of Colorado Boulder)
    17/09/2019, 19:00
    WG5-WG7 Joint Session
    talk

    Plans for a laser-ionized, beam-driven plasma wakefield accelerator at SLAC’s FACET-II facility are presented. The plasma source is formed by laser ionization of a volume of uniform density gas, and the plasma density profile is therefore determined by the focal pattern of the laser. This offers the advantage of a tunable density profile that can accommodate entrance and exit ramps suitable...

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