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91̽»¨
Simulated proton image of magnetic fields in a turbulent laser-plasma
Credit: Adapted from Bott et al., "Proton imaging of stochastic magnetic fields". J. Plasma Phys. 83 (2017)

Dr Archie Bott

UKRI Future Leaders Fellow

Research theme

  • Lasers and high energy density science
  • Plasma physics

Sub department

  • Atomic and Laser Physics

Research groups

  • 91̽»¨ Centre for High Energy Density Science (OxCHEDS)
  • Theoretical astrophysics and plasma physics at RPC
archie.bott@physics.ox.ac.uk
  • About
  • Publications

Field reconstruction from proton radiography of intense laser driven magnetic reconnection

Physics of Plasmas AIP Publishing 26:8 (2019)

Authors:

CAJ Palmer, PT Campbell, Y Ma, L Antonelli, AFA Bott, Gianluca Gregori, J Halliday, Y Katzir, P Kordell, K Krushelnick, SV Lebedev, E Montgomery, M Notley, DC Carroll, CP Ridgers, Alexander Schekochihin, MJV Streeter, AGR Thomas, ER Tubman, N Woolsey, L Willingale

Abstract:

Magnetic reconnection is a process that contributes significantly to plasma dynamics and energy transfer in a wide range of plasma and magnetic field regimes, including inertial confinement fusion experiments, stellar coronae, and compact, highly magnetized objects like neutron stars. Laboratory experiments in different regimes can help refine, expand, and test the applicability of theoretical models to describe reconnection. Laser-plasma experiments exploring magnetic reconnection at a moderate intensity (IL ∼1014 W cm-2) have been performed previously, where the Biermann battery effect self-generates magnetic fields and the field dynamics studied using proton radiography. At high laser intensities (ILλL2>1018 Wcm-2μm2), relativistic surface currents and the time-varying electric sheath fields generate the azimuthal magnetic fields. Numerical modeling of these intensities has shown the conditions that within the magnetic field region can reach the threshold where the magnetic energy can exceed the rest mass energy such that σcold = B2/(μ0nemec2) > 1 [A. E. Raymond et al., Phys. Rev. E 98, 043207 (2018)]. Presented here is the analysis of the proton radiography of a high-intensity (∼1018 W cm-2) laser driven magnetic reconnection geometry. The path integrated magnetic fields are recovered using a "field-reconstruction algorithm" to quantify the field strengths, geometry, and evolution.

Thomson scattering cross section in a magnetized, high-density plasma

Physical Review E American Physical Society 99:6 (2019) 063204

Authors:

Archie FA Bott, Gianluca Gregori

Abstract:

We calculate the Thomson scattering cross section in a nonrelativistic, magnetized, high-density plasma—in a regime where collective excitations can be described by magnetohydrodynamics. We show that, in addition to cyclotron resonances and an elastic peak, the cross section exhibits two pairs of peaks associated with slow and fast magnetosonic waves; by contrast, the cross section arising in pure hydrodynamics possesses just a single pair of Brillouin peaks. Both the position and the width of these magnetosonic-wave peaks depend on the ambient magnetic field and temperature, as well as transport and thermodynamic coefficients, and so can therefore serve as a diagnostic tool for plasma properties that are otherwise challenging to measure.

Retrieving fields from proton radiography without source profiles

(2019)

Authors:

MF Kasim, AFA Bott, P Tzeferacos, DQ Lamb, G Gregori, SM Vinko

Supersonic plasma turbulence in the laboratory

Nature Communications Nature Research 10 (2019) 1758

Authors:

TG White, MT Oliver, P Mabey, AFA Bott, AA Schekochihin, Gianluca Gregori

The Thomson scattering cross section in a magnetized, high density plasma

(2019)

Authors:

Archie FA Bott, Gianluca Gregori

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