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Space and Planets (artistic image)
Credit: hdwallpaperim.com/

Gianluca Gregori

Professor of Physics

Research theme

  • Lasers and high energy density science
  • Plasma physics

Sub department

  • Atomic and Laser Physics

Research groups

  • Laboratory astroparticle physics
  • Oxford Centre for High Energy Density Science (OxCHEDS)
Gianluca.Gregori@physics.ox.ac.uk
Telephone: 01865 (2)82639
Clarendon Laboratory, room 029.8
  • About
  • Publications

Integrated laser-target interaction experiments on the RAL petawatt laser

PLASMA PHYS CONTR F 47 (2005) B833-B840

Authors:

PK Patel, MH Key, AJ Mackinnon, R Berry, M Borghesi, DM Chambers, H Chen, R Clarke, C Damian, R Eagleton, R Freeman, S Glenzer, G Gregori, R Heathcote, D Hey, N Izumi, S Kar, J King, A Nikroo, A Niles, HS Park, J Pasley, N Patel, R Shepherd, RA Snavely, D Steinman, C Stoeckl, M Storm, W Theobald, R Town, R Van Maren, SC Wilks, B Zhang

Abstract:

We review a recent experimental campaign to study the interaction physics of petawatt laser pulses incident at relativistic intensities on solid targets. The campaign was performed on the 500 J sub-picosecond petawatt laser at the Rutherford Appleton Laboratory. An extensive suite of optical, x-ray, and particle diagnostics was employed to characterise the processes of laser absorption, electron generation and transport, thermal and K-alpha x-ray generation, and proton acceleration.
More details from the publisher

Laboratory simulations of supernova shockwaves: Formation of a second shock ahead of a radiative shock

Aip Conference Proceedings 784 (2005) 721-729

Authors:

JF Hansen, MJ Edwards, D Froula, G Gregori, A Edens, T Ditmire

Abstract:

Supernovae launch spherical shocks into the circumstellar medium (CSM). These shocks may interact with both the intergalactic magnetic field (IGM) and local mass accumulations (possibly with their own local magnetic fields). The latter interaction may trigger star formation. The shocks have high Mach numbers and may be radiative. We have created similar shocks in the laboratory by focusing laser pulses onto the tip of a solid pin surrounded by ambient gas; ablated material from the pin rapidly expands and launches a shock through the surrounding gas. The shock may then be allowed to interact with (a) mass accumulations, (b) magnetic fields, or (c) allowed to expand freely. We will present examples of each type of experiment, but mainly discuss a new phenomena observed first in (c); at the edge of the radiatively heated gas ahead of the shock, a second shock forms. The two expanding shocks are simultaneously visible for a time, until the original shock stalls from running into the heated gas. The second shock remains visible and continues to expand. A minimum condition for the formation of the second shock is that the original shock is super-critical, i.e., the temperature distribution ahead of the original shock has an inflexion point. In a non-radiative control experiment the second shock does not form. © 2005 American Institute of Physics.
More details from the publisher

Supersonic propagation of ionization waves in an underdense, laser-produced plasma

Physics of Plasmas 12:6 (2005) 1-8

Authors:

C Constantin, CA Back, KB Fournier, G Gregori, OL Landen, SH Glenzer, EL Dewald, MC Miller

Abstract:

A laser-driven supersonic ionization wave propagating through a millimeter-scale plasma of subcritical density up to 2-3 keV electron temperatures was observed. Propagation velocities initially ten times the sound speed were measured by means of time-resolved x-ray imaging diagnostics. The measured ionization wave trajectory is modeled analytically and by a two-dimensional radiation-hydrodynamics code. The comparison to the modeling suggests that nonlocal heat transport effects may contribute to the attenuation of the heat-wave propagation. © 2005 American Institute of Physics.
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Measurements of Green Laser-Beam Propagation and Backscatter in Long-Scale Length Plasmas

2013 Abstracts IEEE International Conference on Plasma Science (ICOPS) Institute of Electrical and Electronics Engineers (IEEE) (2005) 164-164

Authors:

C Niemann, L Divol, D Froula, S Glenzer, G Gregori, R Kirkwood, A Mackinnon, N Meezan, J Moody, C Sorce, R Bahr, W Seka
More details from the publisher

Laboratory simulations of supernova shockwave propagation

ASTROPHYS SPACE SCI 298:1-2 (2005) 61-67

Authors:

JF Hansen, MJ Edwards, D Froula, G Gregori, A Edens, T Ditmire

Abstract:

Supernovae launch spherical shocks into the circumstellar medium (CSM). These shocks have high Mach numbers and may be radiative. We have created similar shocks in the laboratory by focusing laser pulses onto the tip of a solid pin surrounded by ambient gas; ablated material from the pin rapidly expands and launches a shock through the surrounding gas. Laser pulses were typically 5 ns in duration with ablative energies ranging from 1-150 J. Shocks in ambient gas pressures of similar to 1 kPa were observed at spatial scales of up to 5 cm using optical cameras with schlieren. Emission spectroscopy data were obtained to infer electron temperatures (< 10 eV).In this experiment we have observed a new phenomena; at the edge of the radiatively heated gas ahead of the shock, a second shock forms. The two expanding shocks are simultaneously visible for a time, until the original shock stalls from running into the heated gas. The second shock remains visible and continues to expand. A minimum condition for the formation of the second shock is that the original shock is super-critical, i.e., the temperature distribution ahead of the original shock has an inflexion point. In a non-radiative control experiment the second shock does not form. We hypothesize that a second shock could form in the astrophysical case, possibly in radiative supernova remnants such as SN1993J, or in shock-CSM interaction.
More details from the publisher

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