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Linac Lessons Learned from LCLS-I. Franz-Josef Decker 14-Dec-2011 CSR is a big deal limiting performance Tolerance studies beforehand helped a lot Tor’s List Software adaptability helped speed up commissioning . CSR (Coherent Synchrotron Radiation). - PowerPoint PPT Presentation
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Linac Lessons Learned from LCLS-I
Franz-Josef Decker 14-Dec-2011
CSR is a big deal limiting performance Tolerance studies beforehand helped a lot Tor’s List Software adaptability helped speed up commissioning
CSR (Coherent Synchrotron Radiation)FEL intensity [mJ] is suppressed at the shortest
bunchlengths (highest peak current) we canrun under- or over-compressed
Emittance growth due to CSR in BC2(is there a cure?)
Under - compressed
Over -
com
pres
sed
Charge: 1nC 250 pC 150 pCInstead of raising charge (like SLC or PEP-II) LCLS
runs “better” with lower charges, same FEL intensity with lower charge and shorter FEL pulses
1 nC was abandoned early on, emittance growth to Li28
250 pC had (has) double horizontal FEL spot and 150 pC is cleaner and more stable
User are asking for even lower charges (80,) 40, 20 pC for shorter pulses lengths
Tolerance Budgets, e.g.: long. Jitter
L1S: 0.05 need 0.03
DE/E: 0.04%
Need even better for certain experiments
XX--bandband XX--
0.500.50
XX--bandband XX--XX--bandband XX--
0.500.50
Energy jitter bigger than spreadJitter: 4.0E-4 Intensity after
monochromatorSpread: 3.3E-4 varies 100%
Simulated FEL through MonochromatorEnergy spread: 0.02% Mono width:
0.006% hard edge Energy jitter: 0.04% Intensity jitter:
20% (blue)
New jitter compensation ideas
Over-compressed: Stable areaOver-compression cancels L1S
jitter: more negative phase in L2give lower E, but also longer bunch length (less WF) so more E: 0.045-0.050%to 0.030-0.035%
Less taper (by Ops) reduces FEL intensity spikes
under overcompressed
From XPP thru Mono:No FEL intensity and very high
spikes got eliminated
Before
D. Fritz
No intensity
FEL spikes
Always some intensity
Barely FEL spikes
taper
Tor’s ListHe would love to hear about anything that
impacts the design of BC1/BC2, the phase control, klystron com-plement, diagnostics, and beam operational modes.
BC1: Energy change: 250 220 MeV for less L1S jitter (un-SLEDed or lower modulator voltage)
BC2: Energy change: 4.5 4.7 5.0 GeV gives higher end energy (sometimes less chirp possible)
Phase control: new PACs and PADs are good, but not all klystrons have this control. New PACs for each SBST would help some multi-bunch issues
Klystron complement: no issues
Tor’s List cont.Diagnostics: BPMs good, Beam phase somewhat
noisy (online), wire scanner o.k., but slow (except 10 sec version with bumps), (Li24 wires never installed), OTRs in BCs used in linac, BLMs (length) have filter issues (mirco-bunching) are calibrated with TCAV3, BLM after DL2 still missing
Beam operational modes: Energy change (20 min), charge change (1 hr), peak current change(2 min), rate change, … all routine by now with GUIs
CQs (dispersion Correction Quads) in BC1, BC2, DL2 also change the betatron match, absolute DL2 energy is also influenced; dispersive bumps might be better
Software adaptability helped speed up commissioning, e.g. E-Loss GUI
10-April-2009: First Lasing (YAGXRAY max_out)
15-April: 1.3 mJ “possible” energy loss due to FEL
17-April: DL2toDumpEnergyLoss function18-April: DL2 Dump Loss Matlab PV 562 2-May: I_pk correction: 14 MeV/kA24-May: E Loss GUI 8-Aug: Gas detector calibration
Other Linac Issues by RegionEarly Linac (Injector): MCORs jitter near zero, RF
kick jitter at load end if multi-pacting or not (L0A), quads 3% weaker if near other magnets, source of micro-bunching(?), x-band: wakefield + dispersion + rf-kick, lattice good for diagnostic, but (maybe) not for beam (space charge at focus in OTR2?), good BC bend magnets necessary, L1S stability, …
L2: wakefields in early L2 affect emittance, matching VERY critical for FEL performance, BC2 dispersion fix, …
L3: matching in Li26 (?), emittance growth with shorter bunches (Li28), Li30 match into BSY, …
SummaryLinac performs well for FEL operation
Coherent effects limit higher FEL intensity (the beam wants to radiate before reaching the undulator)
Jitter, especially in the longitudinal (30 times shorter), is a real challenge But soon energy jitter reaching levels of intrinsic
SASE FELTor’s List: Leave it flexible, good and enough
diagnostics, new PAC (Phase & Amplitude Control) per sector
Software adaptability is good (inside AD), connections to photon side are a pain