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Design Considerations of table-top FELs

Design Considerations of table-top FELs. DESY, June 20; recap of FLS 2006, May 15, 2006. LMU: F. Grüner , U. Schramm, S. Becker, R. Sousa, T. Eichner, D. Habs MPQ: S. Karsch, M. Geissler, L. Veisz, J. Meyer-ter-Vehn, F. Krausz UCLA: S. Reiche. laser-plasma accelerators

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Design Considerations of table-top FELs

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  1. Design Considerations of table-top FELs DESY, June 20; recap of FLS 2006, May 15, 2006 LMU: F. Grüner, U. Schramm, S. Becker, R. Sousa, T. Eichner, D. HabsMPQ: S. Karsch, M. Geissler, L. Veisz, J. Meyer-ter-Vehn, F. KrauszUCLA: S. Reiche • laser-plasma accelerators • principal possibility of table-top FELs • possible VUV and X-ray scenarios • new experimental status • critical points review • cooperation with DESY…

  2. Laser-Plasma accelerators: “bubble acceleration” electron bunch: e.g. 170 MeV (LOA), 1.2 GeV (Berkeley) TW laser,5-50 fs

  3. M. Geissler PIC code 5fs, a=5

  4. Discharge capillary ~4 cm 300 µm gas-filled capillary electrodes Leemanslaser-plasma-acceleration * presented at Anomalous Absorpt. Conf., June 6, 2006; submitted to Science MPQ: since two weeks 0.35 J in 37 fs, soon 1-2 J future (~2009): 5 J, 5 fs (=1 PW), 1 kHz

  5. Improvement by capillaries de-phasing • discharge introduces parabolic electron density • laser guiding beyond Rayleigh length → higher energies • de-phasing: reducing energy spread • ion-channel: reducing electron beam diameter and divergence • possible scenario: bubble turns into linear wakefield → GeV- energies with ~0.1% energy spread • started cooperation with Simon Hooker (Oxford)

  6. Important feature: ultra-high current typical length scale = plasma wavelength laser pulse ~ 2 µm only!!~ nC charge ~ 100 kA

  7. Principal possibility for table-top FELs simplest estimate: ideal 1d Pierce parameter (no energy spread, emittance, diffraction, time-dependence) : few 100kA (classical: 5 kA) current und. period : few mm (class. few cm) beam diameter (optimal!)

  8. Constraints for table-top FELs saturation length (Xie Ming)for SASE VUV FEL @ ~28nm Λ (Xie Ming) DESY flash (fs mode):λu= 27 mm (462 MeV)εn = 6 mm·mradΔE/E = 0.04 % MPQ (GENESIS)λu= 3 mm (133 MeV)εn = 1 mm·mradΔE/E = 0.5 % • not only table-top size, but sufficient output power: reduction in λu allows a reduction in γ, but needs ultra-high currentfor keeping ρand also saturation power large enough

  9. Start-to-End Simulations electron bunch transport/focusing/filter FEL undulator laser GPT, Geant CSRTrack, Spur;GENESIS 1.3 own 3d PIC code

  10. A possible first VUV case

  11. International competition and a possible first table-top XFEL case

  12. New Experimental Status undulator:60 periods, 5 mm period, 1.6 mm gap~1 T field on axis few days ago: 40 MeV electrons

  13. Critical Points Review • space charge influence due to ultra-dense bunches • - HOMDYN (L. Serafini): for 1 GeV correlated energy spread 0.5 %, no debunching • GPT/CSRtrack runs (see next talk) • simple analytical estimates in agreement with GPT • linear energy chirp can be compensated with tapering • transverse coherence • valid only for spontaneous source, here: gain guiding • calculate growth rate of next higher mode with GENESIS • transverse coherence important for focusing only? • peak brilliance: 1032@ 5 keV - comparable with LCLS! (1012 phts/0.1%BW, θ=15µrad, σx=30µm, τ=10fs)

  14. Cooperation with you… • verify our GPT results with ASTRA • verify entire feasibility study (publishing a joint paper) • discuss beam features in detail (slice energy spread, etc.) • for experiments: diagnostic methods (FROG) • open questions, such as maximum photon energy • what could you learn from us????

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