Start-to-End Simulations
Mikhail Krasilnikov, ASTRA Simulations for the FLASH Injector (Jan. 2009)
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FLASH photo injector has been simulated (re-optimized) using a new ASTRA version (Dec. 2008).
The goal of the optimization is the projected transverse emittance after the first half of ACC1 for different bunch charges:
1nC, 0.5nC, 0.25nC. Obtained photo injector parameters are summarized in the following table:
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Subsystem
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Parameter
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Unit
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1nC
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0.5nC
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0.25nC
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Cathode Laser
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temporal
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profile
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Gaussian
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Gaussian
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Gaussian
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Trms
|
ps
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4.4
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4.4
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4.4
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transverse
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Profile
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rad.hom.
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rad.hom.
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rad.hom.
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XYrms
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mm
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0.516
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0.381
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0.286
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Ek
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eV
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0.55
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0.55
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0.55
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RF Gun
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FB
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1.13
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1.13
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1.13
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Ecath
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MV⁄m
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45
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45
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45
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phase
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deg
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-2
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-2
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-2
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Gun Solenoid
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Bmax
|
T
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0.173188
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0.173456
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0.173314
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zpos
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m
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0.276
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0.276
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0.276
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bucking
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compens.
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compens.
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compens.
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ACC1
1x4TESLA
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Emax
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MV⁄m
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26
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26
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26
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phase
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deg
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7
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4
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-2
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zpos*
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m
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3.3
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3.3
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3.3
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Electron Beam
at z=8.5m
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Charge
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nC
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1
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0.5
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0.25
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kin. energy
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MeV
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59.7
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60.2
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60.6
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Erms
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keV
|
647
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330
|
67
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length
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mm
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2.3
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1.9
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1.6
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XYsize
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mm
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0.41
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0.41
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0.36
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proj. XY emit.
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mm
mrad
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1.58
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1.04
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0.76
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Remarks:
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Cathode laser has Gaussian temporal profile with 4.4ps rms pulse length,
transverse profile is assumed to be radial homogeneous
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Gun cavity is shifter in 30 cm upstream
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The booster contains first 4 TESLA cavities of ACC1,
its gradient fixed (field amplitude 26MV/m), phase tuned for a smaller emittance
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Gun phase was not optimized and taken from 1 nC case (-2deg off-crest)
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Thermal emittance used for these simulations is based on the optimistic theoretical model (Ek=0.55eV),
recent thermal emittance measurements at PITZ shows higher values of Ek
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200000 ASTRA particles have been used
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Electron beam properties along the photo injector:
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Q=1nC
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Q=0.5nC
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Q=0.25nC
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Electron beam properties at z=8.5m (after first half of ACC1)
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Resulting projected emittance and peak current
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Some ASTRA outputs:
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Transverse phase space for the case Q=1nC
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Longitudinal phase space for the case Q=1nC
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Beam views for Q=1nC
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Transverse phase space for the case Q=0.5nC
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Longitudinal phase space for the case Q=0.5nC
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Beam views for Q=0.5nC
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Transverse phase space for the case Q=0.25nC
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Longitudinal phase space for the case Q=0.25nC
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Beam views for Q=0.25nC
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