Optical Diagnostics of Colliding Laser Produced Plasmas Paddy Hayden National Centre for Plasma Science & Technology (NCPST)/ School of Physical Sciences, Dublin City University EMMI Workshop on Non-Linear Dynamics of Simple Quantum Systems at Extreme Temperatures and Intensities Nov 2nd 2011 Outline • • • • Colliding Plasmas – Orientation Time Resolved Imaging Interferometry Visible Spectroscopy – Density – Temperature • Ion Emission • Summary EMMI NDSQS Workshop 2011 Colliding Plasmas - Orientation EMMI NDSQS Workshop 2011 Colliding Plasmas - Orientation 1 1 0.8 0.8 0.8 0.6 0.4 0.2 Density (n/n0) 1 Density (n/n0) Density (n/n0) Multi-fluid colliding plasma simulations, Rambo and Denavit, J. COMP. PHYS. 98 317 (1992) 0.6 0.4 0.2 0.4 0.2 When plasma plumes collide there are two extreme scenarios: 1. Interpenetration - interactions collisions Distance (x/x ) Distanceare (x/x ) mostly via binary Distance (x/x ) 0 time - plumes decelerated 150 timesteps 300rapid timesteps 2. Stagnation at collision plane, accumulation of material, kinetic energy converted into excitation energy (glow), rapid growth of dense (stagnated) layer,……… 0 0 50 100 150 200 0 0 50 100 0 1 0.8 0.8 0.6 0.4 0.2 100 Distance (x/x0) 50 100 150 200 200 150 200 6 5 0.6 0.4 0 0 150 0 0.2 50 0 0 200 Density (n/n0) 1 0 0 150 0 Density (n/n0) Density (n/n0) 0.6 4 3 2 1 50 100 Distance (x/x0) EMMI NDSQS Workshop 2011 150 200 0 0 50 100 Distance (x/x0) Colliding Plasmas - Orientation • The parameter which determines whether the plumes are likely to interpenetrate or stagnate is the so-called ‘collisionality parameter’ given by: D ii • Where D is the separation between the two plasmas and λii is the ion-ion Mean Free Path (MFP). ii 1 2 m v 2 2 1 12 4e 4 Z 4 n2 ln 12 EMMI NDSQS Workshop 2011 Colliding Plasmas - Orientation From laterally colliding Controllable parameters: 1. Plasma Separation 2. Laser intensity o) 3. Target angle One (0o tocan 180engineer Key point: stagnation layer 4. Laser wavelength/pulse characteristics; ‘hardness’, density, temperature, shape, etc. by varying geometry (D) and laser-target duration. interaction physics (mfp, λii) - application specific….. to counter streaming EMMI NDSQS Workshop 2011 Time Resolved Imaging Resolution of ~4 ns (now 1.5 ns), use filters to isolate emission from a particular ion stage EMMI NDSQS Workshop 2011 Time Resolved Imaging x 10 4.5 Dt = 30 ns Delay = 30 ns Dt = 0 ns 500 4 4 500 1000 3 2.5 1500 2 1.5 2000 Distance (m) Distance (m) 3.5 Delay = 100 ns 16000 Dt = 100 ns 14000 12000 1000 10000 1500 8000 6000 2000 4000 1 2500 2500 2000 0.5 500 1000 1500 2000 500 2500 1000 1500 2000 2500 Distance (m) Distance (m) 12000 Delay = 600 ns Delay = 200 ns Dt = 200 ns 10000 1000 8000 1500 6000 2000 4000 2500 2000 500 1000 1500 2000 Dt = 295 ns 500 Distance (m) Distance (m) 500 1000 Dt = 600 ns 1000 1500 2000 500 2500 500 2500 1500 1000 1500 2000 2500 Distance (m) Distance (m) Seed Plasmas with 1.3 mm separation, each formed with 300 mJ, 1064 nm, 6 ns laser pulses. Spotsize: ca. 100 μm. Time delay measured relative to the peak of the split laser pulse. EMMI NDSQS Workshop 2011 0 Angle Resolved Imaging EMMI NDSQS Workshop 2011 Nomarski Interferometry EMMI NDSQS Workshop 2011 EMMI NDSQS Workshop 2011 Comparison to Imaging EMMI NDSQS Workshop 2011 Visible Spectroscopy Min. gate width ~4 ns Spatial Res. = 70 μm Spectral Res. = <0.2nm EMMI NDSQS Workshop 2011 Visible Spectroscopy Time-Space Density Measurements: Target Delay = 300 ns Wavelength (nm) Voigt profiles fitted and densities determined by Lorentzian width and Stark parameters in C. Colón et al. Phys. Scr. 73 (2006) 410–419. EMMI NDSQS Workshop 2011 Visible Spectroscopy 100o target Experimental Parameters used: 140o wedge target, each seed plasma formed with 200 mJ, 1064 nm, 6 ns pulses. Spotsize: 100 μm, plasma separation: 2.6 mm. Time delay relative to peak of laser pulse. EMMI NDSQS Workshop 2011 Visible Spectroscopy Time-Space Temperature Measurements Target Delay = 300 ns Wavelength (nm) Temperatures from 485.97 nm and 492.57 nm Sn III lines. Spectrum is binned at 0.5 mm intervals. Temperatures were determined from the line ratios. EMMI NDSQS Workshop 2011 Visible Spectroscopy 100o target Distance (mm) Experimental Parameters used: 140o wedge target, each seed plasma was formed with 200 mJ, 1064 nm, 6 ns pulses. Spotsize: 100 μm and plasma separation: 2.6 mm. Time delay relative to peak of laser pulse. EMMI NDSQS Workshop 2011 Ion Emission Angle Resolved Ion Emission Experiment EMMI NDSQS Workshop 2011 Ion Emission We observe quite significant narrowing of the TOF distribution compared to single plasma plumes Plasma ion bunch compression EMMI NDSQS Workshop 2011 Ion Emission As we move the detector off normal emitted ion flux from each (left or right hand side) single plume dominates => weak lateral emission from stagnation layer -fewer damaging fast ions and perhaps less plasma debris? EMMI NDSQS Workshop 2011 Ion Emission One can also tune the width and peak energy of the ‘total ion’ TOF distribution with the laser energy (6ns/1064nm) EMMI NDSQS Workshop 2011 Summary • Strong stagnation in table top colliding plasmas due to large value of the collisionality parameter (ζ) • Degree of confinement/ hardness of the stagnation layer can be controlled by designing the value of ζ • Stagnation layer becomes quite uniform after 100ns • It looks attractive for investigation as alternative injector systems for ion accelerators, pulsed laser materials deposition source, LIBS, laboratoryastrophysical model experiments, X-ray lasers, fusion (Hohlraums) etc. • Real time exploration of t and D to optimise stagnation layer conditions in an application specific manner. EMMI NDSQS Workshop 2011 Acknowledgements DCU: J. Costello, P. Hough, J. Dardis, T. Kelly, C. Fallon and B. Doohan S. S. Harilal. School of Nuclear Engineering, Purdue University N. Gambino, University of Catania, Italy UCD: G. O’Sullivan, P. Dunne, E. Sokell, F. O’Reilly, ... TCD: J. Lunney, I. Tobin Funding: Science Foundation Ireland 07/IN.1/I1771, Irish Research Council for Science Engineering and Technology (Embark Initiative), EU COST MP0601 Action and ERASMUS MUNDUS - EMJD -EXTATIC - FPA 2012-0033 - EACEA programme EMMI NDSQS Workshop 2011
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