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Lasers and Highly-Charged Heavy Ions

Lasers and Highly-Charged Heavy Ions. at. F acility for A ntiproton and I on R esearch. FAIR. Nuclear Structure & Astrophysics (Rare-isotope beams). Hadron Physics (Stored and cooled 14 GeV/c anti-protons). SIS18. p-Linac. SIS100 /300. UNILAC. QCD-Phase Diagram

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Lasers and Highly-Charged Heavy Ions

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  1. Lasers andHighly-Charged Heavy Ions at HZDR Workshop, Rossendorf, 6/9/11

  2. Facility for Antiproton and Ion Research HZDR Workshop, Rossendorf, 6/9/11

  3. FAIR Nuclear Structure & Astrophysics (Rare-isotope beams) Hadron Physics (Stored andcooled 14 GeV/c anti-protons) SIS18 p-Linac SIS100/300 UNILAC QCD-Phase Diagram (HI beams 2 to 45 GeV/u) HESR Rare-Isotope Production Target Fundamental Symmetries & Ultra-High EM Fields (Antiprotons & highly stripped ions) Anti-Proton Production Target Dense Bulk Plasmas (Ion-beam bunchcompression & petawatt-laser) CR &RESR Cryring NESR Materials Science & Radiation Biology (Ion & antiproton beams) 100 m Accelerator Physics HZDR Workshop, Rossendorf, 6/9/11

  4. Parallel Operation HZDR Workshop, Rossendorf, 6/9/11

  5. Experiments CBM APPA Super-FRS PANDA NuSTAR HZDR Workshop, Rossendorf, 6/9/11

  6. PANDA PANDA HZDR Workshop, Rossendorf, 6/9/11

  7. Compressed Baryonic Matter SIS100/300 ALICE @ CERN CBM @ FAIR HZDR Workshop, Rossendorf, 6/9/11

  8. NuSTAR HZDR Workshop, Rossendorf, 6/9/11

  9. APPA • Atomic Physics, Fundamental Interactions,High EM Field Physics (SPARC) • Weak interactions in parity-violating atomic transitions • High field QED in bound system • Pair production • Plasma Physics, Planetary Astrophysics • Warm Dense Matter (WDM) &High Energy Density Matter (HEDgeHOB) • Plasma astrophysics in the lab • Nuclear Physics • Measurement of nuclear moments • Nuclear excitation by laser excitation (NEET) • Applied Physics, Accelerator Science • Integrated concept for laser-acceleration applications HZDR Workshop, Rossendorf, 6/9/11

  10. Staging 2017/18 HZDR Workshop, Rossendorf, 6/9/11

  11. Modularised Start Version M0 M3 M1 M3 M2 CBM/HADES APPA Experiments M1: APPA M1: CBM/HADES M2: NuSTAR M3: PANDA PANDA NuSTAR HZDR Workshop, Rossendorf, 6/9/11

  12. Timelines 2011 2012 2013 2014 2015 2016 2017 2018 2019 9 11 12 6 7 8 10 Building permits Site preparation Civil construction contracts Building of accelerator & detector components Completion of civil construction work Installation of accelerators and detectors Data taking 10 6 7 12 8 9 11 HZDR Workshop, Rossendorf, 6/9/11

  13. Lasers & HI Accelerators Novel lasers: Vulcan, POLARIS, DRACO, PHELIX, ELI Free electron lasers (e.g. LCLS @ SLAC) Advanced particle accelerators(e.g. @ GSI and FAIR) "... thus the technologies are complementary [intense light sources and ion beams] and both are likely to lead to new insights in high-intensity science." National Research Council, USA, 2008 HZDR Workshop, Rossendorf, 6/9/11

  14. Parity-Violating Transitions in Atoms Energy levels of He-like uranium 2E1 (PNC) g N N N N e e Z e e Mixing coefficient for states with opposite parities: To “compete” with spontaneous decay channels one needs to induce a two-photon PNC transition by polarisedlight with intensity 1020 W/cm2 Select case with small splitting! HZDR Workshop, Rossendorf, 6/9/11

  15. Extreme EM Fields Lasers Heavy ions EquivalenttoI ≥ 1028 W/cm2 (adapted from Mourou, Tajima, Bulanov, RMP 78, 2006) Sub-femtosecond pulses Large EM fields, zeptosecond pulses HZDR Workshop, Rossendorf, 6/9/11

  16. Relativistic HI EM Fields E U92+ B Parameters of the “pulse”: @ FAIR: The electric field produced by a moving charge (g>>1) is nearly transverse (linearly polarised) and is accompanied by a transverse magnetic field of almost equal strength. HZDR Workshop, Rossendorf, 6/9/11

  17. Plasmas Inertial Fusion Energy Magnetic Fusion Temperature [eV] XFEL Sun Core PHELIX SIS 100 Laser Heating FLASH Ideal plasmas Ion Beam Heating Strongly coupled plasmas SIS 18 Jupiter solid state density Sun Surface Particles / cm-3 HZDR Workshop, Rossendorf, 6/9/11

  18. WDM & HEDgeHOB @ FAIR High-brilliance XUV photon sources (FLASH@DESY) Intense, energetic beams of heavy ions (GSI & FAIR) 65 mm Ne10+300 MeV/u; Kr crystal small sample volume (100 m3) high gradients low-Z target material short time scales (100 fs) large sample volume (mm3) uniform physical conditions any target material long time scales (50 ns) Heavy-Ion beams at FAIR and novel XUV photon sourcesprovide complementary tools: Specific energy ~ kJ/g Temperature up to 1 eV Pressure multi-kbar range HZDR Workshop, Rossendorf, 6/9/11

  19. Laser-generated X-ray or proton diagnostics @ FAIR X-rays coherent (XRL) or incoherent Laser beam back-lighter target Laser-accelerated protons Laser beam HZDR Workshop, Rossendorf, 6/9/11

  20. SpectroscopyofLithium-likeIons 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 13,9nm/89eV (Ag) 14,7nm/84eV (Pd) 0 18,9nm/66eV (Mo) 50 60 70 80 90 22,0nm/56eV (Zr) ESR-Magnets (10 Tm) Electron Cooler (240 kV) Steerer-Magnets (7,2 Tm) Nuclear Charge Z 2P3/2 ...allowsforprecisiontestsof QED, atomicphysicsandnuclearmodels... 2P1/2 2S1/2 HZDR Workshop, Rossendorf, 6/9/11

  21. Larger Doppler-Boost @ HESR, =5 Back-scattered laser radiation from a compact electron ring (e.g. semi-commercial „Lyncean Compact Light Source“ would reach well above 100 keV. HZDR Workshop, Rossendorf, 6/9/11

  22. Laser-Accelerated Protons & Conventional Accelerators Joint research project @ GSI Helmholtz Institute Jena: Project coordination, 100TW compressor, short laser pulse and ion beam diagnostics GSI: PHELIX Laser, timing, control system, beamlines, accelerator structures, beam diagnostics FZ Dresden-Rossendorf: Solenoid for collimation & PSU TU Darmstadt: Acceleration experiments, collimation simulations, target development Univ. Frankfurt: Accelerator structure development HZDR Workshop, Rossendorf, 6/9/11

  23. Thank you very much! HZDR Workshop, Rossendorf, 6/9/11

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