Precise and Fast Timing Network - a first view -
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Transcript of Precise and Fast Timing Network - a first view -
Precise and Fast Timing Network- a first view -
B. JeanneretCTC , December 2009
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Tolerance on Phase and Gradient• Luminosity and understanding/adjustment of the Beam Delivery and of
the Final Focus, DB vs. MB D.Schulte & R.Tomas, PAC09
Not much margin on these. i.e. σ ϕ = 0.2o ΔL/L = -1% σ ϕ = 0.4o ΔL/L = -4%
Overall cycle DB intertrain (or sector to sector)
Many contributions to : intrinsic + measurement errors, two beams , …
On top : MB vs. MB : twice smaller
1fs = 10-15 s
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e+ injector, 2.4 GeV
e- injector2.4 GeV
CLIC 3 TeV
e+ main linace- main linac , 12 GHz, 100 MV/m, 20.85 km
BC2BC2
BC1
e+ DR365m
e- DR365m
booster linac, 9 GeV, 2 GHz or 4 GHz ?
decelerator, 24 sectors of 868 m
IP1
BDS2.75 km
BDS2.75 km
47.9 km
drive beam accelerator2.38 GeV, 1.0 GHz
combiner rings Circumferences delay loop 72.4 m
CR1 144.8 mCR2 434.3 m
CR1CR2
delayloop
326 klystrons33 MW, 139 ms
1 km
CR2delayloop
drive beam accelerator2.38 GeV, 1.0 GHz
326 klystrons33 MW, 139 ms
1 km
CR1
TAR=120m
TAR=120m
245m 245m
83ps
TOL : 45fs
DB
MB
Feed-back box
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Timing and feed-back strategy in the tunnel• To relax on δφ : feed-forward &
back before entering each DECEL
9 GeV MB as a fast clock
Timing line
TA
MB to IP
DB∆t to:injectors DB & MBDamp. RingsMB TADB TAs@50 Hz
BA
Phase from B, Energy jitter δE from A&B,Phase correction for δE
C
D
C&D, Phase error MB/DB , to synchronizethe injector linacs
Open issue: frequency band of δE correction
E
D.Schulte et al,CLIC Note598A.Andersson & J. SladenEPAC06,TUPCH086PAC07,MOPAN066
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Fast & Precise timing network
…
MBTA
DRe-
Pre-DRe-
MBlinac
DRe+
IPEXP
TADBLinac
DLCR1,2
Source
MBLTL
Fbackbox
24 x
9Gev LTL
DECEL
Main Linac2km
50m
1km
500m
?
2km
100m
1km
20km
50mAll this for σt = 15fs
Here σt = 7.5fs to synchronizethe two complex
Here relaxed, tol must be set for full capture and match to damping timeBootLinac
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Long distance Cabling Issues
• Thermal expansion of copper :– dL/L =αΔT= 1.7 10⋅ -5 ΔT
• L = 100m , dL = δz = 5 mum ΔT = δz/α/L = 3 10⋅ -3 K
• XFEL approach– Move to optical fibers, with continuous length
measurement (reflect signal to the emitter)– Lasers and special fibers to produce soliton waves
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Precise timing network• Little (or no) expertise on site as of today.• Complicated optical systems• Expertise exists at XFEL (DESY,PSI)
• Presentations at CLIC09 : WG3 THURSDAY 11h00-12h30
– Long distance Optical Fibers with fs resolutionF. Oemer Ilday / Bilkent Univ. Ankara
– Overview of the Phase Measurement System at SLS/PSIVladimir Arsov / PSI
– Femtosecond optical synchronization system for FLASHMatthias Felber / DESY
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Open Issues• The whole timing network must afford a time resolution
δt = 15fs (7.5 fs for a part) – to be refined
– Which part must be fast, i.e allow for intra-cycle feedback/correction ?
– Which part need be precise only, i.e. allow for inter-cycle
analysis/diagnostics ?
• In-house expertise to be built-up
• In parallel : explore source of errors
– Measurements proper
– Slow movements
– Vibrations (nearby transformers, pulsed kickers, water turbulences, …)