intensity measurements through the stacking cycle
DESCRIPTION
Intensity Measurements through the Stacking Cycle. Recycler/Pbar Beam Physics Meeting Keith Gollwitzer January 14, 2005. What Intensities?. Currently ~5x10 12 protons on target. Secondaries in AP2 and early in the Debuncher ~10 9 particles - PowerPoint PPT PresentationTRANSCRIPT
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Intensity Measurements through the Stacking Cycle
Recycler/Pbar Beam Physics Meeting
Keith Gollwitzer
January 14, 2005
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What Intensities?
• Currently ~5x1012 protons on target.
• Secondaries in AP2 and early in the Debuncher ~109 particles
• Circulating in Debuncher and transferred to Accumulator is ~7.5x107 pbars
• Accumulator core increases up to ~1.5x1012 pbars
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Different Measurements• One pass
– Toroids (Dave P.)– SEMs relative measurements; blows up beam– Ion Chamber small blow up of beam– Gap Monitor INJFLX; first pass in Debuncher
• Circulating in Debuncher – BPM Intensity require bunch/debunch during
stacking cycle– DCCT (Dave P.)– FFT prior to extraction Longitudinal coherence
• Circulating in Accumulator– FFT on injection orbit Longitudinal coherence– BPM Intensity for free during ARF1 ramp– Deposition orbit new stacktail monitor
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One Pass Measurements During Stacking
Toroid SEM Gap Monitor (INJFLX)Ion ChamberSolid – Existing Dashed – FutureDotted – Not Stack
DtoA Transfer
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SEM Intensity measurement from area of fit
Dependent upon being able to subtract noiseWires intercept beam and cause beam blow-up
Shown here is special Debuncher SEM403.
Two vertical peaks are the injection pass and closed orbit.
Beam is completely killed by multiple closed orbit passes.
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Different Measurements• One pass
– Toroids (Dave P.)– SEMs relative measurements; blows up beam– Ion Chamber small blow up of beam– Gap Monitor INJFLX; first pass in Debuncher
• Circulating in Debuncher – BPM Intensity require bunch/debunch during
stacking cycle– DCCT (Dave P.)– FFT prior to extraction Longitudinal coherence
• Circulating in Accumulator– FFT on injection orbit Longitudinal coherence– BPM Intensity for free during ARF1 ramp– Deposition orbit new stacktail monitor
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Flux capacitor (INJFLX) from mixing the gap monitor with the RF signal
Being updated to be a java OAC.
Overhead seems to limit to 3-4sec per update; being worked upon.
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Different Measurements• One pass
– Toroids (Dave P.)– SEMs relative measurements; blows up beam– Ion Chamber small blow up of beam– Gap Monitor INJFLX; first pass in Debuncher
• Circulating in Debuncher – BPM Intensity require bunch/debunch during
stacking cycle– DCCT (Dave P.)– FFT prior to extraction Longitudinal coherence
• Circulating in Accumulator– FFT on injection orbit Longitudinal coherence– BPM Intensity for free during ARF1 ramp– Deposition orbit new stacktail monitor
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DRF1 bunching pbars prior to the end of the stacking cycle in the Debunchers
P2 curve design ; time is with respect to $80
Beam Injection
Beam Extraction
Sample BPMduring 20ms
flat top
Sample timefor ACNET DAQ
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Switching plate BPM signal sent through a SA at zero span and small resolution bandwidth (averaging) and its video
output sent to an oscilloscope input triggered via D:TBT ($83)
Injection of secondaries and
debunching
Bunch and Debunch beam for intensity sampling
Not the same P2 curve as previous slide
Blow-up time scale and pull trace of “flat-top” signal and process height for ACNET variable
In the future, SA and scope setup will be replaced by Ashmanskas board
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Simple comparison of Intensities
TOR109 (10^12 protons)
BPM Intensity (arb)
IC728 (10^8 secondaries)
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Histogramming of Intensities
BPM Intensity
IC728 / TOR109
BPM / TOR109
BPM / IC728 ~3% Width
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Different Measurements• One pass
– Toroids (Dave P.)– SEMs relative measurements; blows up beam– Ion Chamber small blow up of beam– Gap Monitor INJFLX; first pass in Debuncher
• Circulating in Debuncher – BPM Intensity require bunch/debunch during
stacking cycle– DCCT (Dave P.)– FFT prior to extraction Longitudinal coherence
• Circulating in Accumulator– FFT on injection orbit Longitudinal coherence– BPM Intensity for free during ARF1 ramp– Deposition orbit new stacktail monitor
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Recent Changes to FFT 1st look at “stability”
Previous version had averaging and history involved.
Coherence would affect signal for awhile.
Also saw periodic behavior.
Now trying to place in OAC
Averaging but no history.
Coherence – What to do
Paul Derwent is investigating
AccumulatorDebuncher
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Different Measurements• One pass
– Toroids (Dave P.)– SEMs relative measurements; blows up beam– Ion Chamber small blow up of beam– Gap Monitor INJFLX; first pass in Debuncher
• Circulating in Debuncher – BPM Intensity require bunch/debunch during
stacking cycle– DCCT (Dave P.)– FFT prior to extraction Longitudinal coherence
• Circulating in Accumulator– FFT on injection orbit Longitudinal coherence– BPM Intensity for free during ARF1 ramp– Deposition orbit new stacktail monitor
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New Stacktail Monitor• Main purpose is to
watch deposition area and monitor how efficiently the stacktail system clears the deposition orbit area (the width of ARF1 bucket).– Essentially measures
power prior and after ARF1 deposits beam.
• Can use as relative measure of beam on deposition orbit(?) To be Seen.
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Comment about Events & Timeline
• It has been noticed that the “stability” of intensity signals during stacking is dependent upon Event and Timeline– There can be a yield difference between pure
$29 slip stacking events and $21 mixed mode stacking + switchyard event: up to 10% for IC728/TOR109
– The TLG does not make it easy for consistent $80 spacing; in general stacking cycle time varies.
– One shots and other study cycles