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Shintake monitor in ATF2: status, performance and prospects. Taikan Suehara (The Univ. of Tokyo). M. Oroku, T. Yamanaka, H. Yoda, Y. Kamiya, S. Komamiya (The Univ. of Tokyo) Y. Honda, T. Kume, T. Tauchi (KEK) T. Sanuki (Tohoku Univ.). Maybe this is my last talk about the Shintake monitorā¦. - PowerPoint PPT Presentation
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Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Shintake monitor in ATF2:Shintake monitor in ATF2:status, performancestatus, performance
and prospectsand prospects
Taikan Suehara (The Univ. of Tokyo)M. Oroku, T. Yamanaka, H. Yoda,
Y. Kamiya, S. Komamiya (The Univ. of Tokyo)Y. Honda, T. Kume, T. Tauchi (KEK)
T. Sanuki (Tohoku Univ.)
Maybe this is my last talk about the Shintake monitorā¦
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
TopicsTopics
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Accelerator Test Facility 2 Accelerator Test Facility 2 (ATF2)(ATF2)
ā¢ ATF2: a final focus test facility for the ILC (2008/End-)ā ATF2 goals:
ā¢ 37 nm beam sizeā¢ 2 nm position stabilization
ATF2
About 110 m
1.3 GeV Linac
Dumping ring(ATF)
ATF2 focusesan ultra low emittance
electron beam produced in ATF
to achieve 37 nmbeam size
āShintake monitor (IP beam size monitor)
āIP-BPM (beam position monitor)
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Goals of the Shintake MonitorGoals of the Shintake MonitorShintake monitor is the most proven
beam size monitor for nanometer beams.Target performance in ATF2:ā¢ Ļy: 25 nm ā 6 m (Shintake method)
ā < 10% RMS statistical error in 1 minute (90 pulses) meas.
ā < 2 nm systematic error at 37 nm (ATF2 design)ā Off-axis carbon wire scanner: 1 m ā
ā¢ Ļx: 2.8 m ā 100 m (Laser-wire)ā < 10% RMS error in 1 minute meas.ā 3.5 m () laser spot size at the IP
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Schematic of Shintake MonitorSchematic of Shintake Monitor
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Schematic of Shintake Monitor (cont.)Schematic of Shintake Monitor (cont.)Narrow beam
Narrow beam
Thick beam
Thick beam
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Modulation depth and Crossing Modulation depth and Crossing anglesangles
Crossing angles
Fringe pitch
Observable beam size
174Ā° 266nm 25 - 100nm
30Ā° 1.0m 100 - 400nm
8Ā° 3.8m 0.4 - 1.5m
2Ā° 15.2m 1.5 - 6.0m
M: modulation depth(amplitude / average)Ļ: crossing angle
2, 8, 30, and 174 degrees arechosen to observe 25 to 6000 nm
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Layout and ComponentsLayout and Components
Laser & electronics hut
Laser transport line
Signal line
Gamma detector Bending magnet
Main optical table
Components:ā¢ Laser
ā 532 nm wavelengthā 40 MW, 8 ns FWHMā Single mode
(90 MHz line width)ā 10 Hz max.
ā¢ Laser transport lineā About 15 m
ā¢ Optical tableā 1.6 by 1.7 mā Independent
support frameā¢ Gamma detector
ā CsI(Tl) multi layersā Gamma collimators
ā¢ Electronics
zoom
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Layout ofLayout ofoptical tableoptical table
174Ā°mode30Ā°mode8Ā°mode2Ā°mode
Laser wire mode
y
x
z
z
x
Beam entrance
95% reflectionmirror
Angle selectionmirrors & a prism
Focal point(é»åćć¼ć ćÆē»é¢ć« )åē“50% splitter
1700
1600
éęć¬ć³Focal lenses
Features:ā¢ Switchable
crossing anglesā Rotation mirrors
ā¢ Alignment equipmentsā Slit and Beam scan
ā¢ Laser positionstabilization / correctionā 6 PSDs
ā¢ Phase stabilizationā Image sensors
with objective lenses
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Laser alignment & position Laser alignment & position stabilizationstabilization
Alignment:ā Z: for perfect overlap
of two laser beams1.7 m accuracy achievable
ā XY: for minimum powerjitter by laser fluctuation
0.6 m accuracy achievable
Laser position jitter/drift:ā Stabilization by an active feedback using laser position s
ensor (PSD)s and mirror movers (for slow drift)ā Correction of a pulse-to-pulse power jitter
caused by laser angular jitterPerformance is estimated by Monte-Carlo simulation
Slit scan (Z) Beam scan (XY)
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Phase stabilizationPhase stabilization
Ima
ge
se
nso
rMicroscope lens
Schematic of the phase monitor:Magnified fringes are captured.
Setup of the phase monitor
1. Phase acquisitionImage sensors w/ lenses, Fourier transf.
2. Phase controlA delay line with a piezo stage(0.2 nm resolution). 10 Hz feedback.
10 nm stability is required ā active stabilization
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Phase stabilization(2)Phase stabilization(2)
Phase controlPhase without stabilization (10 min.)
Phase with stabilization (10 min).
Geometry of the stabilization test
In the test setup,0.24 rad.(10.1 nm) RMS stabilityis achieved in 1 minute window.(Acceptable stability)
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Vacuum chamber with the IP-Vacuum chamber with the IP-BPMBPM
Electron beam position jitterā phase jitter on modulation plot
ā
IP-BPM (8.7 nm resolution demonstrated)is attached to cancel the jitter
Waveguide
X Port
Y Port
SensorCavity
Beam Pipe Slot
Schematic of the IP-BPMattached to the chamberof the Shintake monitor
ā IP-BPM before assembly
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Support FrameSupport FrameFD
table
Specifications:ā¢ Weight: 1950 kg
(Table: 690 kg)ā¢ 250 mm thickness
steel honeycomb tableā¢ Position adjustment
ā Height: insertion platesunder the table
ā Horizontal: by screwsStatus:ā¢ Fabrication ongoingā¢ Arrival at KEK: 12 March
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Status & SummaryStatus & Summaryā¢ New optical table is designed
ā Basic features have almost been checkedā¢ Phase monitor / stabilizationā¢ Laser position monitoring / stabilization / correctionā¢ IP-BPM
ā Design almost fixed, fabrication ongoing
ā¢ Scheduleā Transportation, installation and initial alignment
of the optical system: ~ Jun. 2008ā Control software and its tests: ~ Aug. 2008ā ATF2 Beam on: Oct. 2008ā 37 nm measurement: 2009?
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Overview of the detectorOverview of the detectorBrems. background from the beam l
ine should be subtracted.ā¢ On-Off method
Subtract laser-off data as background
ā¢ Shot-by-Shot methodUsing layer information to separate
background340mm(18.4 X0)
Gamma
CsI(Tl) scintillator4 front layers (5 mm thick each) + 1 bulk layer (290 mm thick) Simulated shower development of
signal and background
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
CalibrationCalibrationā¢ Calibration using laser photons
Voltage-gain relationā High gain (~900V)
for cosmic-ray testā Low gain (~300V)
for operation
ā¢ Calibration by cosmic raysā Front 4 layersā Bulk layersSystematic error remains
between front and bulk layers
Front layers
Bulk layers
Cosmi. sample
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Setup of beam testSetup of beam test
Gamma detector
Layout of Beam test setup
ā¢ ATF extraction line2007 Oct. ā Dec.
ā¢ Wire scanner photonsā similar energy
spectrum to background
ā System checkā Not used in
following analysesā¢ Laser-wire photons
ā Almost the same energy spectrumto signal photons
ā Statistics is very limited(only 30 minutesacquisition time,O(10000) photons)
ā¢ Two subtraction methods are comparedusing laser-wire data.
Detector at exp. site Position alignment using laser
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
On-Off method On-Off method Procedures:ā¢ Acquire 1000
bunches of ālaser-offā data.
ā¢ Acquire 1000 bunches of ālaser-onā data.
ā¢ Acquire 1000 bunches of ālaser-onā data with lower laser intensity.
ā¢ Subtract ālaser-offā data from each ālaser-onā data set.Signals from all layers are summed before subtraction.
Result:ā¢ Apparent excess of ālaser-onā data is observed.ā¢ Laser intensity and signal strength are correlated
(though not proportional due to unspecified effects).
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Shower developmentShower development
ā¢ Gain of the bulk layer is not matched to the front layersbecause of the systematic error of the cosmic ray calibration.
ā¢ Only front 4 layers are used for the current analysis.
For the Shot-by-Shot method, fraction of energy depositat each layer is compared to Geant4 simulation data.
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Shot-by-Shot method (4 layers) Shot-by-Shot method (4 layers)
Result:ā¢ Similar spectrum to the On-Off method is obtained.ā¢ Effectiveness of this method is validated.ā¢ Statistical error is bigger in this method (as expected).
Consistent!
Procedures:1. Acquire 1000
bunches of ālaser-onā data.
2. Estimate āsignalā and ābackgroundā using layer information.
ā¢ Pure āsignalā and pure ābackgroundā energy deposit at each layer is derived from the beam test data.ā¢ The amount of ālaser- offā signal is not used. Background amount is estimated only by shape of the shower development.
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
DiscussionDiscussionā¢ Basic ideas of the two methods are validated by the beam
test.ā¢ Exact calibration of the bulk layer is very important for both
methodsFluctuation of the total energy deposit is much smaller than that of
the shower developmentā more exact calibration method is being investigated.
ā¢ Background spectrum varies by experimental conditionsSpectrum differs from simulation ā effects of secondary particlesā spectrum should be checked frequently and we use the obtained
spectrum for the Shot-by-Shot method.
ā¢ Statistics of the laser-wire data are very shortWe obtain only Compton photons of O(10) bunches in real operation.
ā Additional beam tests are highly desired after proper calibration is performed.
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Error factors of the Shintake monitorError factors of the Shintake monitorā¢ Statistical fluctuation
ā Power jitter: 4.4% (after correction/stabilization)ā¢ Electron beam charge, corrected by a current monitor: 1%ā¢ Laser intensity, corrected by power monitors: 3.8%ā¢ Laser direction fluctuation, corrected by position monitors:
1.4%ā¢ etc.
ā Phase jitter: 13.3 nm (after correction/stabilization)ā¢ Phase stabilization fluctuation: 10.1 nmā¢ IP-BPM: 8.7 nm
ā Background fluctuation: 8.3%ā¢ Statistical fluctuation of estimated number of background
photons
ā¢ Systematic errorsā Fringe contrast: measured by < 5% accuracyā etc. ( << 5%)
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Modulation AcquisitionModulation Acquisitionā¢ Fitting Method
ā Phase scan of 45 points (equal interval), fitted by a sine function
ā¢ RMS Methodā Phase scan of 45 points (equal interval), using RMS of the
spectrum
ā¢ Peak Search Methodā Phase scan of 25 points to obtain peak/valley positionsā Average 10 pulses for both peak and valley positions
Fitting Method RMS Method Peak Search Method
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
ā¢ RMS method is the best in M < 40%, and peak search method is the best in M ā§ 40%
ā¢ < 10% statistical fluctuation can be achieved within 25 ā 6000 nm measurement range
ā¢ Systematic error (~5%) is not included
Beam size resolutionBeam size resolution
Statistical fluctuation of the modulation depth Resolution of the beam sizeusing peak search & RMS methods
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Shintake Monitor for the ILCShintake Monitor for the ILCā¢ Modulation depth @ 5.7 nm ILC beam
ā 89.6% with 157 nm F2 laserā 92.9% with 193 nm Excimer laserā 93.9% with 213 nm YAG 5th laserIn current error factors (ATF2), 17% resolution at M=90%
ā¢ Multi bunch operationā Quick accumulation of statistics
ā¢ Improvement of resolution by a factor of 10 at 3940 bunches
ā 1 train measurement ā slow drift suppressedā Need high-repetition laserā Fast phase scan by a Pockels cell
ā¢ Systematic error is similar, 5% can be achieved
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Shintake monitor for the ILC (2)Shintake monitor for the ILC (2)ā¢ Installation at the Interaction Point
in the beam commissioning stageā Assure 5.7 nm beam focusingā Fast tuning without interactionā Must be removed when installing the
detectorsBy push-pull structure??
ā¢ Installation to the second IP for a diagnostic monitorā > 25 nm beam size measurements are
much more realistic using current scheme.
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
1. Overview2. Optical Table and Support Frame3. Beam Test of Gamma Detector4. Performance Estimation &
Extension to the ILC5. Summary
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
SummarySummary
ā¢ Shintake monitor in ATF2 can measure y from 25 nm to 6 m within 10% resolution, 5% systematic error in 1 minute period.
ā¢ Optical table fabrication is ongoing.ā¢ The beam test demonstrates basic signal/ba
ckground separation using two methods.ā¢ 5.7 nm measurement is realistic if we use a
high-repetition deep-UV laser.
Taikan Suehara, TILC08(GDE+ACFA)@Sendai, 2008/03/05
Thank you.Thank you.