01/20/2009Wei, Sawada, Macphee, Mackinnon1 Revised target lists – Focus on shock heating and e-transport in WDM targets – Add electron transport in shocked.

Slides:



Advertisements
Similar presentations
Center for Radiative Shock Hydrodynamics Fall 2011 Review Experimental data from CRASH experiments Carolyn Kuranz.
Advertisements

Grating Phase-Contrast Imaging for Diagnostic of High Energy Density Plasmas D. Stutman, M.P. Valdivia, M. Finkenthal Department of Physics & Astronomy.
1 Monoenergetic proton radiography of laser-plasma interactions and capsule implosions 2.7 mm 15-MeV proton backlighter (imploded D 3 He-filled capsule)
10L Simulations Close to current Titan parameters. Here’s the big picture… electron diagnostic “target planes” every 25  m preplasma L = 5μm (3) LASER.
Self-generated and external magnetic fields in plasmas J. P. Knauer Laboratory for Laser Energetics University of Rochester HEDSA Symposia on High Energy.
Point design and integrated experiments Convenors summary ( M Key, K Tanaka, P Norreys ) What is the status of integrated point designs for the various.
Lawrence Livermore National Laboratory Pravesh Patel 10th Intl. Workshop on Fast Ignition of Fusion Targets June 9-13, 2008, Hersonissos, Crete Experimental.
Independent operations of 3 legs of OMEGA-60 Long-term request: 3 independent legs –Benefits include Overall increased flexibility in beam/driver configuration.
U N C L A S S I F I E D Experiments and Simulations of Ablatively Driven Shock Waves in Gadolinium Richard Kraus, Eric Loomis, Shengnian Luo, Dennis Paisley,
First THz Measurements at FACET Ziran Wu, Alan Fisher, Henrik Loos FACET 2011 Users Meeting
Preliminary Results from Titan Divergence Measurements L. D. Van Woerkom Department of Physics The Ohio State University FSC Special Meeting LLNL 4-6 August.
Measuring E and B fields in Laser-produced Plasmas with Monoenergetic Proton Radiography 9 th International Fast Ignition Workshop C. K. Li MIT Cambridge,
Richard M. Bionta XTOD July 19-21, 2005 UCRL-PRES-xxxxxx X Ray Diagnostics LCLS FAC Meeting Oct. 27, 2005.
Detector Monoenergetic proton backlighting for studying field evolution and areal density in HEDP R. D. Petrasso, MIT 3 MeV DD D 3 He Detector 0.6 ns after.
UNCLASSIFIED Heat Transport Measurements in Foil Targets Irradiated with Picosecond Timescale Laser Pulses D. J. Hoarty 1, S F James 1, C R D Brown 1,
Kodak RAR 2492 Film Same film as above Integrate ~50 shots for good signal X-ray Imaging Spectroscopy of Ti Foils and Pyramidal Targets Gilliss Dyer, Byoung-Ick.
GEOMETRIC EFFECTS ON EUV EMISSIONS IN M. S. Tillack, K. L. University of California San Diego.
ICF Research at York Looking beyond ignition at the NIF John Pasley.
Studies of proton generation and focusing for fast ignition applications Fast Ignition Workshop Nov 4th 2006 Andrew Mackinnon Lawrence Livermore National.
Simulations investigating the effect of a DT-ice-covered cone tip on the implosion of a re-entrant cone-guided ICF capsule J. Pasley - University of California.
FSC 1 Benchmark Modeling of Electron Beam Transport in Nail and Wire Experiments Using Three Independent PIC Codes Mingsheng Wei Annual Fusion Science.
K-Shell Spectroscopy of Au Plasma Generated with a Short Pulse Laser Calvin Zulick [1], Franklin Dollar [1], Hui Chen [2], Katerina Falk [3], Andy Hazi.
Diagnostics for Benchmarking Experiments L. Van Woerkom The Ohio State University University of California, San Diego Center for Energy Research 3rd MEETING.
Modeling the benchmark experiments Mingsheng Wei, Fei He, John Pasley, Farhat Beg,… University of California, San Diego Richard Stephens General Atomics.
Update on LLNL FI activities on the Titan Laser A.J.Mackinnon Feb 28, 2007 Fusion Science Center Meeting Chicago.
ICFT/P PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION 9 th International Fast Ignition Workshop Cambridge, MA 3 November.
Characterization of Inertial Confinement Fusion Capsules Using an X-Pinch Source High Energy Density Physics Summer School Berkeley California, August.
OSU/UCSD/GA Experimental Program J. Pasley, E. Shipton, T. Ma, B. Bucher, S. Chen, F. Beg University of California at San Diego E. Chowdhury, L. Van Woerkom,
DANTE vs. Witness Plate Radiation Temperature Comparison These calculations were performed by undergraduates David S. Conners, & Nate C. Shupe, under the.
Hot Electron Behaviors Relevant to Fast Ignition K. A. Tanaka 1,2, H. Habara 1,2, R. Kodama 1,2, K. Kondo 1,2, G.R. Kumar 1,2,3, A.L. Lei 1,2, K. Mima.
Laser plasma researches in Hungary related to the physics of fast ignitors István B Földes, Ervin Rácz KFKI-Research Institute for Particle and Nuclear.
Assembly of Targets for RPA by Compression Waves A.P.L.Robinson Plasma Physics Group, Central Laser Facility, STFC Rutherford-Appleton Lab.
Imploding cone-in-shell capsule 2.7 mm 15-MeV proton backlighter Imaging detector Protons per unit area on detector protons Proton Radiography of Electromagnetic.
GA workplan Primary: design and build the complex targets needed for experiments. –targets that can be accurately modeled in simulation codes. –targets.
October 19, 2003 Fusion Power Associates Status of Fast Ignition-High Energy Density Physics Joe Kilkenny Director Inertial Fusion Technology General Atomics.
Measurement of Magnetic field in intense laser-matter interaction via Relativistic electron deflectometry Osaka University *N. Nakanii, H. Habara, K. A.
This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Security, LLC, Lawrence Livermore National Laboratory.
Data acquisition system for experiments at GSI HHT experimental area. A. Kantsyrev 1, D. Varentsov 2, A. Hug 2, S. Udrea 2, L. Shestov 1, V. Turtikov 1.
Great feeling Walking Ifen without machines Sunday Jan 26, 2007.
Lawrence Livermore National Laboratory Andrew G. MacPhee 17 th Topical Conference on High Temperature Plasma Diagnostics Albuquerque, NMWed 14 th May 2008.
Intense Laser Plasma Interactions on the Road to Fast Ignition Linn D. Van Woerkom The Ohio State University APS DPP Orlando, FL 14 November 2007 FSC.
COST Meeting Krakow May 2010 Temperature and K  -Yield radial distributions of laser-produced solid-density plasmas Ulf Zastrau X-ray Optics Group - IOQ.
1 Multiphase code development for simulation of PHELIX experiments M.E. Povarnitsyn, N.E. Andreev, O.F. Kostenko, K.V. Khischenko and P.R. Levashov Joint.
Angular distribution of fast electrons and
This work was performed under the auspices of the U.S. Department of Energy by the University of California Lawrence Livermore National Laboratory under.
1 Development and testing of a pulsed helium ion source for probing materials and warm dense matter studies Qing Ji a, Peter Seidl a, Will Waldron a, Jeff.
IAEA Chengdu, Oct 2006 Andrew MacKinnon This work was performed under the auspices of the U.S. Department of Energy by University of California Lawrence.
LSP modeling of the electron beam propagation in the nail/wire targets Mingsheng Wei, Andrey Solodov, John Pasley, Farhat Beg and Richard Stephens Center.
Fast Electron Temperature Scaling and Conversion Efficiency Measurements using a Bremsstrahlung Spectrometer Brad Westover US-Japan Workshop San Diego,
Multi-colour sctintillator-based ion beam profiler James Green, Oliver Ettlinger, David Neely (CLF / STFC) 2 nd Ion diagnostic workshop June 7-8 th.
1. Fast ignition by hydrodynamic flow
Lawrence Livermore National Laboratory Titan June 2008 Experiment Planning January 31, 2016.
[1] AstroShk-13A : February 28, 2013 Shock reflection phenomena relevant to astrophysical jets P Hartigan J M Foster, D Martinez K Yirak, B H Wilde, P.
Opacity Correction (1/20/09) Schumacher, Ovchinnikov Materials: Copper (1/e absoption length taken as 22  ), Aluminum (72.4  ). Targets: Slab sandwich,
FSC 1 Electron Transport Experiments Farhat Beg Fusion Science Center Meeting Feb. 28, 2007 FSC RAC.
Shock ignition of thermonuclear fuel with high areal density R. Betti Fusion Science Center Laboratory for Laser Energetics University of Rochester FSC.
SL_THOMSON C. Vaccarezza on behalf of the SL_Thomson team.
Munib Amin Institute for Laser and Plasma Physics Heinrich Heine University Düsseldorf Laser ion acceleration and applications A bouquet of flowers.
International Conference on Science and Technology for FAIR in Europe 2014 APPA Cave Instrumentation for Plasma Physics Vincent Bagnoud, GSI and Helmholtz.
Time-Resolved X-ray Absorption Spectroscopy of Warm Dense Matter J.W. Lee 1,2,6, L.J. Bae 1,2, K. Engelhorn 3, B. Barbel 3, P. Heimann 4, Y. Ping 5, A.
Wide-range Multiphase Equations of State and Radiative Opacity of Substances at High Energy Densities Konstantin V. Khishchenko, Nikolay Yu. Orlov Joint.
1 Radiation Environment at Final Optics of HAPL Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI HAPL Meeting ORNL March.
Experiments at LCLS wavelength: 0.62 nm (2 keV)
Generation of high-pressure shocks in the LICPA-driven collider
E3 Hall layout L4f/1.5kJ/150 fs L4p/150J/150 fs – 10 ps L4n/
LSP Modeling of Ultra-Intense Lasers on Cone-Coupled Wire Targets:
Heating in short-pulse laser-driven cone- and nail-capped wire targets
Short focal length target area: X-ray & ion sources and applications
Diagnosis of a High Harmonic Beam Using
X-Ray Transport, Optics, and Diagnostics WBS Alan J
Presentation transcript:

01/20/2009Wei, Sawada, Macphee, Mackinnon1 Revised target lists – Focus on shock heating and e-transport in WDM targets – Add electron transport in shocked Au targets (~2 day shots) – Add some proton hemisphere + foil targets for proton heating shots (~1 day shots) – Electron source targets postponed to April (2 weeks) Targets requested from LLNL ( Walter has all the information) Al target supports requested from GA (total 70 supports) Beams and diagnostics layout defined Hydro simulations have been performed for shock velocity, timing and warm dense plasmas creation In the process defining laser specs for each shot group, and priority/order of shots. Need to define laser (SP+LP) alignment procedure Need to define target alignment procedure Discuss data logging/shot sheet/real-time analysis, participants’ responsibilities Need LSP simulations for transport study Titan Feb./March 2009 Experiment planning Status: Jan. 20, 2009

01/20/2009Wei, Sawada, Macphee, Mackinnon2 Titan Feb./March 2009 Campaign  Dates: Feb 9 - March 13 (5 weeks) [ will likely be delayed due to the Callisto accident]  Expect ~ _75 shots  Goals Create and characterize WDM targets using LP driven shock compression and heating of low density foams using side-on radiography and SOP SP produced electron transport in such WDM targets by measuring Ka yield and angular distribution and compare with cold targets Electron beam transport in shocked gold targets (CH/Cu/Au) – Relevant to shocked Au cone tip physics in FI Create and characterize WDM targets using SP produced protons  Test the emission spectroscopy technique for EP proton heating experiment SHCCD Axis to Cu crystal And HOPG 16° 20° Target normal 17 °

01/20/2009Wei, Sawada, Macphee, Mackinnon3 The electron transport target will be irradiated with the long and short pulse in nearly opposite direction Axis to Cu crystal And HOPG 16° 20° Target normal 17 ° Long pulse beam (from Door A) East-West axis Short pulse beam 17.71° 18.5° Target normal Beam axis Long pulse beam parameter f# = um spot with phase plate tcc Au Target view from front (short pulse beam side) Target view from behind (long pulse beam side) 45 degree bevel all around

01/20/2009Wei, Sawada, Macphee, Mackinnon4 Cu imager 1 (primary dia.) To TL3 To TL2 DC-HOPG Cu (primary dia.) FROG Cu imager 2 (primary dia.) SOP (primary dia.) Diagnostics and beam layout for the WDM experiment (Jan. 20, 2009) Beam axis LP Through Door A Reentrant HOPG can be moved to various port as needed Streaked HOPG Secondary diagnostics IP for Ti Ka radiography in point projection (primary dia.)

01/20/2009Wei, Sawada, Macphee, Mackinnon5 VSG Titan short pulse BN Si? D = 400  m (ROC = 250  m) X = 375  m Create 100micron wide ? eV and solid density Use VSG (has been developed for use on Titan) to diagnose spectral lines from Nitrogen k - shell ( He-like to H like lines at eV) target Grating Detector Plane 3.8° to 7.8 ° ~ 325 eV to 1700 eV VSG = variable separation grating = XUV spectrometer Warm dense plasma creation via proton isochoric heating and characterization by emission spectroscopy

01/20/2009Wei, Sawada, Macphee, Mackinnon6 Diagnostics

01/20/2009Wei, Sawada, Macphee, Mackinnon7 Targets requested from LLNL Target typesSpecs (in unit of µm)NumberLaser beams Heated transport0.1Al/25CH/5Cu/138CRF/3.9Au26LP+SP on the package target heated point projection radiography 0.1Al/25CH/5Cu/138CRF/5.1Au6LP on the package, Ti disk, 250 µm dia, 10 µm thick12SP on Ti foil 20Al/5Cu/138CRF/3.9Au4 Unheated transport20Al/5Cu/15CH/3.9Au6 SP only 20Al/5Cu/3.9Au6 SOP calibrationAl steps 20/40 µm thick3LP only CRF shock velocity targets CRF steps with Al flash on step side 0.1Al/25CH/CRF step(150/160)/0.1Al 3LP only Transport in shocked Au target 0.1Al/25CH/5Cu/25Au10LP+SP 0.1Al/25CH/5Cu/12.5Au5 Proton heating targetsHollow hemi with grid(2), hemi + Si(?) with Boron Nitride coating on side (specs to be added)(5) 7SP only

01/20/2009Wei, Sawada, Macphee, Mackinnon8 Draft List of shots (in the process of refining)  LP only, SOP calibration and shock velocity – SOP alignment with Al step targets (3 shots) – Shock velocity in CRF foam with SOP(3 shots)  LP+SP (Ti Ka backlight), shock timing –Backlight + Au mesh (4 shots) –Backlighting foam package at t=0, before shock breakout(6 shots)  Diagnostic shots with and Cu foil (2 shots)  Short pulse(SP) only, e-beam transport in  Al/Cu/CRF/Au (2 shots with 1ps, 2 shots with 10 ps)  Al/Cu/Au (2 shots with 1ps, 2 shots with 10 ps)  Al/Cu/CH/Au (2 shots with 1ps, 2 shots with 10 ps)  SP/LP on target, e-transport in shocked CRF foam targets – LP only, background shots (2 shots) – At t1, t2, t3 with 1ps SP, maximum energy? (9 shots) – Repeat with 10 ps SP, maximum energy (9 shots)  SP/LP on target, e-transport in shocked Au targets (CH/Cu/Au[25 or 12]) -Unshocked target with SP only (2 shots) -Fully shocked Au with LP and SP (2 shots) -After shock breakout with LP and SP (2 shots) -Partially shocked Au with LP and SP (2 shots) -Repeat unshocked and fully shocked case with 12 um Au (4 shots)  Proton beam production and heating  beam characterization using hemisphere targets (2shots)  Heating in a secondary foil targets (5shots)

01/20/2009Wei, Sawada, Macphee, Mackinnon9 Who will be doing the experiment? (please let us know your interests, suggested responsibilities to be added/modified) Schedule of PeopleSuggested responsibilitiesAdditional comments Andrewfull 5 weeksLead and run the exp. SebastienHelp on SOP setup, +proton shotsIn&out AndyOversee the exp + proton shotsIn & out PravOversee the expIn&out YuanHalf time?FROG? DanHelp setup EPM(?)+ridealong x-ray diagnostics In&out KramerHelp on diagnostics setup?In&out MingshengFull 5 weeksAssist Andrew co-run the exp, Ti Ka radiography? Foreign national HiroshiFull 5 weeksSOP+shot sheetForeign national SugreevFull 5 weeksDC-HOPG + streaked HOPG BradFull 5 weeksKa imagers + target alignment? Bob+student/postdocFull 5 weeks?Prepulse, autocorrelator,help Dan on the ride-along x-ray diag. Foreign nationals Student from OSU??? anybody else??? RichOversee the expIn&out FarhatOversee the expIn&out, Foreign national

01/20/2009Wei, Sawada, Macphee, Mackinnon10 Hydro simulation results of warm dense plasmas in the shocked foam package target (with Hyades code) Shock reaches the gold/CH foam interface at about 5.2 ns Peak compression is achieved at bout 6.3ns with the compressed foam density of ~ 2g/cc, Te~15-20 eV,~ 10 µm in length (not suitable for transport study) Target: 5µmAu/150µmCHfoam(0.15mg/cc)/5µmCu/25µmCH Long pulse laser: Intensity 4e13 W/cm 2 3ns square pulse, green

01/20/2009Wei, Sawada, Macphee, Mackinnon11 Foam plasma condition at later time may be preferred for transport study Compressed foam plasmas relax and expand with time At 10ns, mass density of ~ g/cc, n e ~4  cm -3, Te~5-7 eV, ~ 75 µm in length

01/20/2009Wei, Sawada, Macphee, Mackinnon12 Foam plasma condition at later time may be preferred for transport study Compressed foam plasmas relax and expand with time At 10ns, mass density of ~ g/cc, n e ~(2-3)  cm -3, Te~5-7 eV, ~ 80 µm in length

01/20/2009Wei, Sawada, Macphee, Mackinnon13 Lasnex simulations (M. Foord) show similar trends, but with higher compression At 10ns, mass density of ~ g/cc, Te~5-7 eV, ~ 30 µm in length Higher absorption may lead to this higher compression

01/20/2009Wei, Sawada, Macphee, Mackinnon14 Hyades simulation results for the shocked Au in the CH(25µm)/Cu(5µm)/Au(30 µm) target Shock propagates into 12 µm Au at about 1.8 ns

01/20/2009Wei, Sawada, Macphee, Mackinnon15 Hyades simulation results for the shocked Au in the CH(25µm)/Cu(5µm)/Au(30 µm) target Shock propagates into 25 µm thick Au at about 2.9 ns