MONALISA David Urner Paul Coe Matthew Warden Armin Reichold Oxford University.
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Transcript of MONALISA David Urner Paul Coe Matthew Warden Armin Reichold Oxford University.
![Page 1: MONALISA David Urner Paul Coe Matthew Warden Armin Reichold Oxford University.](https://reader035.fdocuments.us/reader035/viewer/2022070406/56649e0d5503460f94af767a/html5/thumbnails/1.jpg)
MONALISA
David UrnerPaul Coe
Matthew WardenArmin Reichold
Oxford University
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STATUS: New Design
• More traditional Michelson setup leads to nice results.
• Integration of many interferometer into one node more difficult –
• A compact version is ready and shows promise.
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Parallel Michelson
Originalconcept
Inputbeam
PZT
Mechanical design
PZT
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Michelson : realised in the lab
Stationarymirror
Beam-splitter
PZT sweptmirror
Camera
Launchcollimator
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Michelson :Camera view of mirror sweeping
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Replaced camera with MT connector used 4 nearest neighbour fibres to read out
0 5000 10000 15000
0.0
0.2
0.4
0.6
0.8
1.0
No
rma
lise
d in
ten
sity
/ a
.u.
Time / DAQ cycles
ch 1 ch 2 ch 3 ch 4
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Use modified Carré algorithm to extract4 channel average wrapped phase
0 5000 10000 15000
-3
-2
-1
0
1
2
Ph
ase
/ ra
d
Time / DAQ cycles
UnwrappedWrapped
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9000 10000 11000
-1.0
-0.5
0.0
0.5
1.0
Ext
ract
ph
ase
/
rad
Time / DAQ cycles
Extract independentlyfrom each channelusing 4 points separated equally in time
Here 320 cycles apart
Use modified Carré algorithm to extract
wrapped phase for each channel fit a line
Fit a line to eachstraight sectionaround cycle 10 000and extract residuals
1 ~ 40 mradequivalent 10 nm
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STATUS: New Design
• More traditional Michelson setup leads to nice results.
• Integration of many interferometer into one node more difficult –
• A compact version is ready and shows promise.
![Page 10: MONALISA David Urner Paul Coe Matthew Warden Armin Reichold Oxford University.](https://reader035.fdocuments.us/reader035/viewer/2022070406/56649e0d5503460f94af767a/html5/thumbnails/10.jpg)
Compact Interferometer head
• Shown here using 2cm optics• 1cm optics likely to work. According to
Zemax simulation diffraction should not be a problem. (tests underway)
5cm
4cm
Collimator
Beam splitter
Readout fibres
Input fibre
Retro Reflector
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Status of Subsystems
• Electronics ready for mass production (in use by LiCAS, DC mode integrated for us)
• Temperature measurement system ready for mass production (24 channels built and tested)
• Readout software:– ADC Readout needs adaptation from LiCAS– Binary storage format ready
• FSI data analysis code:– Simple version working and used– In collaboration with LiCAS group implementing advanced object
oriented analysis framework.• Evaluation of Laser to buy for ATF setup finished by end
of January.– New laser available by end of February
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Mass Production of Interferometer
• Full test of present system in air.• Test vacuum system for laboratory:
– Design ready to build vacuum test system– Available in February– Test present setup in vacuum
• Vacuum fibre feedthrough:– Commercial feedthrough too expensive:
• Build own feedtroughs• Jig in production now• First workable feedthroughs by February to be used in test vacuum
system
• Build Jig to place/glue components (beamsplitter and collimator) precisely onto base.– Build first model by March
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• Setup at ATF• Need Scaffolding to hold vacuum tubes• Triangle Nodes Concept
– Drawings ready for base plate – Construction by March
Vacuum system at ATF
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• Triangle Nodes Concept– Drawings ready for base plate – Construction of base plateby March– Construction of instrument platform and dome by May
Vacuum system at ATF
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KEK BPM nodes
• Concept allowing for considerable angle play. • Fixed (or single bellow) attachment to KEK aluminum bar. • Installation early summer 2007
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Move to ATF2
• If 2 nano-BPM setups at ATF2 beam line available:– Within reasonable distance between each other.– Moving experiment to ATF2 beam line can be considered.
• Requirements:– New scaffolding and floor plate– New “flowerpots”
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SLAC/LLBL BPM Node
Here attach vacuum tube for interferometerAttached to BPM.
Holds retro reflector.
Firmconnection
Strain Gauge• Needs bellow to allow
motion of BPM– Vacuum causes a force
order of 100N!
• Develop small force vacuum mount using double bellow system.
• Allows small motion (~1 mm) of BPM-system (we still can measure)
• Large motion (5-10mm) are possible but we cannot measure anymore
• Test stand to measure remaining (perpendicular) force on BPM frame.
-1mm-3mm 1mm 3mm
1N
2N
-1N
0N
-2N
-3N
-3N
Force exerted on carbon frame (BPM)±1mm: < 0.5N/mm±3mm: < 0.8N/mm
Force exerted by perpendicular motion
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SLAC/LLBL BPM Node• Needs bellow to allow
motion of BPM– Vacuum causes a force
order of 100N!
• Develop small force vacuum mount using double bellow system.
• Allows small motion (~1 mm) of BPM-system (we still can measure)
• Large motion (5-10mm) are possible but we cannot measure anymore
• Test stand to measure remaining (perpendicular) force on BPM frame.
• Next item to design is retro holder object: a small tube with vacuum flanges for both bellows at the end.
• Plan to mount in March
• “Flower pot” design needed by March; built in May– Flower pot attached to
scaffolding not carbon fibre tube!
RetroReflector
Retro Holder
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SLAC/LLBL BPM Node• Needs bellow to allow
motion of BPM– Vacuum causes a force
order of 100N!
• Develop small force vacuum mount using double bellow system.
• Allows small motion (~1 mm) of BPM-system (we still can measure)
• Large motion (5-10mm) are possible but we cannot measure anymore
• Test stand to measure remaining (perpendicular) force on BPM frame.
• Next item to design is retro holder object: a small tube with vacuum flanges for both bellows at the end.
• Plan to mount in March
• Allow for true non-touching setup– More difficult analysis
RetroReflector
Retro Holder
NanoGrid
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Combining all Measurement
• Three systems have to be operated simultaniously:– 3 SLAC-BPMs define beam direction– 1 KEK Q-BPM measures motion with respect to that direction.
This BPM is still present on the original motion stage. It can be correlated to the aluminium bar via a Michelson interferometer.
– MONALISA measures relative motion of two BPM systems.
• Isues to be solved:– Read KEK BPM with SLAC readout system– Align two BPM system that both get optimal measurements
We would like to ask if this can be demonstrate before we install MONALISA.
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ATF2: Measuring Motion of Shintake Monitor with Respect to
Final Doublet • Idea of Compact Straightness Monitor (CSM)
presented in May:
Pointsource
Retro
Mirror
Collimator
Fibre launchand readout
Long arm
Use reflection from fibreend as short arm
Distancemeter
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Binocular Michelson
PZTdrivenmirror
Fibre launchcollimator
Pelliclebeam-splitter
Pelliclebeam-splitter
Photodetector
Photodetector
Target retroreflector
Setup takes shape on our optical table.
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Attaching CSM: Shintake Monitor
Monitor and scanner location
IP(on-axis)
Beam sampler
off-axismonitor(ch1)
Phase scanner
off-axismonitor(ch2)
• What do we want to monitor:• Monitor motion (angular
vibrations) of “intersection mirrors”– Its already a mirror– Has to be done in air (Requires
close distance monitor)– Needs to correlate the motion
measurements of the two mirrors.
• Monitor off-axis camera– Easier setup– Mor indirect measurement
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Attaching CSM: Focusing Magnet
• Unsolved Problem on how to monitor magnetic centre of focusing magnet.– Attach CSM to one point of
magnet– Use several distance metres
to monitor breathing of magnet
– Correlate with temperature measurements Retro Reflectors
CSM