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William M. Fawley

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GINGER Results for the. NEW LCLS Undulator Configuration ... Outline of GINGER Study ... GINGER SASE runs for new LCLS drift space/undulator configuration ... – PowerPoint PPT presentation

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Title: William M. Fawley


1
William M. Fawley Lawrence Berkeley National
Laboratory Presented to LCLS Undulator Parameter
Workshop24 October 2003
2
Outline of GINGER Study
  • First determine best K for peak gain for
    monochromatic cases at l1.5, 0.15, and 0.1 nm
  • Examine taper performance for SASE runs at
    0.15-nm, 11.47 GeV base case
  • SASE performance at 0.1 nm with E14.04 GeV
  • Study of taper sensitivity for 1.5 nm case
  • No wake effects examined --- need ELEGANT
    time-dependent beam parameters
  • Some additional S2E SASE results for ICFA03 study
    envelope reconstruction looks surprisingly good

3
Study Parameters/Bottom-Line Results
SASE results best taper for 0.15, 1.5 nm
4
Effects of Linear K Taper on LCLS SASE Output
Power at ?0.15nm
  • GINGER SASE runs
  • New drift space/undulator configuration
  • Quadrupole strengths Twiss parameters from
    H.-D. Nuhn
  • Taper begins at z75 m simple linear decrease
    with z (including drift spaces)
  • Max power obtained around 0.3 to 0.4 taper
    excessively large tapers appear to lead to rapid
    debunching with z and thus reduced gain

5
Bunching and Inverse Bandwidth vs Z0.15-nm LCLS
6
SASE Results at 0.1-nm Wavelength
  • No taper
  • 1st saturation at 110 m
  • Output power 6 GW
  • No obvious anomalies ---but little margin for any
    beam degradation

7
1.5-nm Taper Results
  • 1.5 nm option is a cake-walk for LCLS
    parameters
  • 1st saturation at 30 m simple linear tapering
    begins at z25 m
  • Tapering increases power over 6-fold to gt 80 GW
  • 60 m of undulator gives most of output power
  • More intelligent tapers probably could increase
    power to gt100 GW

8
New GINGER Results for ICFA03 2nd-Order
Simulation Study
  • Extension of results for ICFA03-Zeuthen S2E study
    for LCLS
  • Full SASE simulation extended over full beam head
    region- results low-pass filtered in time
    (original res-olution 12 attoseconds)
  • In regions where 5D distribution is simple,
    full SASE and envelope reconstruction agree
    surprisingly well
  • Similar runs underway for wake case

(CSR but no wake fields)
Output P for SASE peak P(z) for no slippage
cases
9
Where might we go from here?
  • Need ELEGANT runs with/without CSR effects to
    produce time-dependent 5D distributions at
    undulator entrance
  • Examine temporal sensitivity of P(z) to taper
  • Examine
    to wakes
  • One optimization criterion is maximizing product
    of power times the inverse bandwidth (at least
    for experiments in which monochromatization will
    be done)
  • See if results with taper are more sensitive to
    undulator errors, beam offset/pointing errors
  • Perhaps greater sensitivity to phase jitter but
    does deeper ponderomotive well help?
  • Develop taper algorithm for undulator with drift
    spaces consider effects of spiky SASE P(t)
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