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Assembly of Targets for RPA by Compression Waves

This study investigates the production of thin pure hydrogen targets using a laser-driven hydrodynamic approach for Radiation Pressure Acceleration (RPA). The goal is to find the laser-target configuration that produces the highest energy per nucleon. The study explores the physical principles, key problems, and experimental motivations for generating suitable targets for RPA.

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Assembly of Targets for RPA by Compression Waves

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  1. Assembly of Targets for RPA by Compression Waves A.P.L.Robinson Plasma Physics Group, Central Laser Facility, STFC Rutherford-Appleton Lab.

  2. Acknowledgements J.Pasley and I.Bush, University of York, UK R.Kumar, S.Mondal, and whole TIFR team, Tata Institute for Fundamental Research, Mumbai, India A.R.Bell, P.A.Norreys, D.Symes, Central Laser Facility, UK

  3. Summary A HEDP technique for generating pure H targets for RPA.

  4. Background RPA = Radiation Pressure Acceleration

  5. Challenge • Great interest in Radiation Pressure Acceleration. • Early experimental demonstrations of RPA have been reported. • Want to find laser-target configuration that produces highest energy per nucleon. • Here we investigate the production of thin pure hydrogen targets via a laser-driven hydrodynamic approach

  6. Why Pure H targets? • Classic Light-Sail analysis shows that momentum or energy per ion defined by • Energy per nucleon is then 1/A of this energy per ion. • For a given we are therefore always better off with a pure H target. • Mixed targets don’t efficiently accelerate protons. • Therefore we need suitable pure H targets. Robinson et al., NJP (2008)

  7. Problem • Solid H only available under cryogenic conditions (but a low density form of H). • Producing sub-micron foils not yet demonstrated. • Producing foils less than 10 microns not demonstrated. • NIF/ ICF targets : 10s of microns of DT ice on solid material. 10µm 100µm 1µm

  8. Physical Principle 1.Imagine a hot spot being created in a uniform plasma or fluid 3.Cavity expands as compression wave propagates outward. 2.Overpressure region cavitates region and creates a thin shell of dense plasma at edge

  9. Key Problems • Creation of a hot spot at a sufficiently high temperature. • Hydrodynamic evolution of compression wave on multi-ps timescale. • Suitability of final structure for RPA.

  10. Scheme 1 2.Use short pulse to create hot spot on one side 1.Use small ball of cryogenic H 10 micron diameter 3. Drives compression wave into surrounding plasma 4. Produce a thin shell of dense plasma at far side. 5ps 8ps 12ps

  11. Results 1 Use simple hydrodynamic calculation to obtain a density profile. Density x-y Plot Density Line-out Conclusion : Can produce a potentially suitable target.

  12. Scheme 2 2.Use short pulses to create hot spots in cold plasma on both sides 1.Use small ball of cryogenic H 10 micron diameter 3. Drives 2 compression waves into surrounding plasma 4. Compression Waves collide to create a thin dense region.

  13. Results 2 Density x-y Plot Use simple hydrodynamic calculation to obtain a density profile. Density Line-out 10 microns of low density plasma is problematic.

  14. Suitability for RPA Long shelf of plasma at rear (or front) of target is principal concern. Output from hydrodynamic simulation. Profile considered in PIC sim.

  15. Suitability for RPA 2 Still obtain effective acceleration of narrow bunch to > 100 MeV via RPA 1D PIC result below (80fs pulse at 5 x 1021Wcm-2)

  16. Producing a Hot Spot • Used a 1D PIC with a simple collision model. • Done series of simulations for pure H target at cryogenic H density (40 nc) and step-like density profile. • Allows us to include effects like resistive heating while still generating fast electrons fully self-consistently. • Next step – 2D model

  17. Heating Profiles • Linearly Polarized, 20fs, 0.5µm, 5x1018Wcm-2 Can produce keV temperatures over a few microns. Long gradient to cooler region though.

  18. Effect on Hydro Heating profile based on collisional PIC code results produces similar results to those based on pure assumption. Density line-out Density x-y plot

  19. Experimental Motivation

  20. Experimental Motivation 2 Extracts from Mondal et al. PRL 2010 Can probe the motion of the critical surface by looking at Doppler shift of a probe beam.

  21. Experimental Motivation 3 Extracts from Mondal et al. PRL 2010 Experiment Simulation (Coll. PIC+Hydro) Simulation model reproduces experimental measurements well. Motion of crit. surface due to compression wave in simulation.

  22. Review

  23. Summary A HEDP technique for generating pure H targets for RPA.

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