High Precision Beam Position Monitor for the TESLA ... · BPM Proposal. TM010 TM110 TM11 TE01. The...
Transcript of High Precision Beam Position Monitor for the TESLA ... · BPM Proposal. TM010 TM110 TM11 TE01. The...
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High High PrecisionPrecision BeamBeam Position Position Monitor Monitor forfor thethe TESLA TESLA
SpectrometerSpectrometer
Alexei Alexei LiapineLiapineTUTU--BerlinBerlin
ZeuthenZeuthen, 17th March 2003, 17th March 2003
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BPM in the SpectrometerBPM in the Spectrometer
•• the resolution of the resolution of BPMsBPMs has to be higher than 1has to be higher than 1µµm (100nm preferred)m (100nm preferred)•• the dynamic range has to be possibly wide to avoid the dynamic range has to be possibly wide to avoid mecanicalmecanical movementmovement•• BPMsBPMs must work with a beam, which is not parallel to zmust work with a beam, which is not parallel to z--axis axis
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BPM ProposalBPM Proposal
The The exitationexitation of the dipole mode in a cylindrical cavity is proportional of the dipole mode in a cylindrical cavity is proportional to the beam offset from the cavity center: Eto the beam offset from the cavity center: �cos)/( 111110 RrjCJ�
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BPM ProposalBPM Proposal
In order to avoid the modes which are stronger than the dipole mIn order to avoid the modes which are stronger than the dipole modeodea modea mode--selective structure of the cavity is proposed.selective structure of the cavity is proposed.
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BPM BPM ProposalProposal
TM010 TM110
TM11 TE01
The dipole mode TM110 couples to the lowest wave The dipole mode TM110 couples to the lowest wave of the waveguide of the waveguide -- TE01, while the monopole modes couple to the TE01, while the monopole modes couple to the
higher wave higher wave –– TM11, which has a higher cutTM11, which has a higher cut--off frequency.off frequency.Therefore the monopole modes don’t propagate in the waveguide.Therefore the monopole modes don’t propagate in the waveguide.
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AngleAngle--dependencedependence
The dipole mode is also exited if the beam is not parallel to z-axis
lTRrjEV tr
offset
211
0110 ��
��
���
���
2cos
211
0110
klTRklijEV tr
angle �
��
���
���
221
110
110 klctgklkri
VV
offset
angle�
Beam Beam
The ratio of two components:
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1.5 GHz 1.5 GHz -- PrototypePrototype
Closed monitor with the waveguidesClosed monitor with the waveguides Opened cavityOpened cavity
AntennaAntenna Contact inside the Contact inside the waveguide
WaveguideWaveguidewaveguide
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1.5 GHz 1.5 GHz -- PrototypePrototype
1.61.6------VVnoisenoise, , µµVV
4.0/mm4.0/mm14501450VVinin, V, V
1620162021102110QQ00
820820→→∞∞QQextext
1518151810101010f, MHzf, MHz
34 34 (0.5mrad, 100nm)(0.5mrad, 100nm)------VVangleangle/V/Voffsetoffset
0.06/100nm of beam 0.06/100nm of beam offsetoffset
9.3(0.005)9.3(0.005)/100/100µµm of m of slot offsetslot offset
VVoutout, mV, mV
115115660660DampingDamping time, nstime, ns
TM110TM110TM010TM010ParameterParameter
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1.5 GHz 1.5 GHz -- PrototypePrototype
The cavity was tested with a network The cavity was tested with a network analyseranalyserin order to check its resonant frequencyin order to check its resonant frequency
and the quality factorand the quality factor
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1.5 GHz 1.5 GHz -- PrototypePrototype
1. Resonant 1. Resonant carecteristiccarecteristic of of two armstwo arms2. 2. LinescanLinescan in wide rangein wide rangeσσ=50nm in =50nm in --0.50.5……+0.5mm+0.5mmσσ=160nm in =160nm in --1…+1mm1…+1mm
3. 3. LinescanLinescan in narrow rangein narrow rangeσσ=400nm, =400nm, VVoutout=8.5=8.5µµV/100nmV/100nm
VCO
P Measurement setupMeasurement setup
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ElectronicsElectronics
TheThe electronicselectronics forfor thethe monitormonitorisis designeddesigned usingusing thethe homodynehomodyne
principle
The The apperanceapperance of the electronicsof the electronics
principle
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ElectronicsElectronics
Characteristic of the position Characteristic of the position channel
CharacteristicCharacteristic of of thethe chargechargechannelchannel channel
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Measurements with ElectronicsMeasurements with Electronics
1. 1. LinescanLinescan in wide range in wide range σσ=180nm=180nm2. 2. LinescanLinescan in narrow range in narrow range σσ=20nm=20nm3. 3. LinescanLinescan after tuning after tuning σσ=200nm in =200nm in --1..+1mm1..+1mm
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ConclusionsConclusions
•• relative resolution is about 200nmrelative resolution is about 200nm++ linear range is linear range is --1mm…+1mm1mm…+1mm+ moderate mechanical tolerances+ moderate mechanical tolerances+ relative simple and cheap electronics+ relative simple and cheap electronics-- strong anglestrong angle--dependent componentdependent component-- large and heavylarge and heavy-- hard to provide high vacuumhard to provide high vacuum
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AlternativesAlternatives5.5 GHz cavity5.5 GHz cavity
+ smaller, easier to handle+ smaller, easier to handle+ weak angle+ weak angle--dependent componentdependent component+ stronger dipole mode signal+ stronger dipole mode signal+ better time resolution+ better time resolution-- critical production tolerancescritical production tolerances-- smaller linear range (250smaller linear range (250µµm)m)-- more complicated electronicsmore complicated electronics
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AlternativesAlternatives
We want to measure not the offset, but the angleWe want to measure not the offset, but the angleProbably TE111Probably TE111--cavity is the right one for that purposecavity is the right one for that purpose