energy spectrometer for the ilc

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Energy Spectrometer Energy Spectrometer for the ILC for the ILC Alexey Lyapin Alexey Lyapin University College London University College London

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Energy Spectrometer for the ILC. Alexey Lyapin University College London. BPM energy spectrometer collaboration. UCL: Filimon Gournarnis, Alexey Lyapin, Matthew Wing Cambridge: Mark Slater, David Ward RHUL: Stewart Boogert DESY-Zeuthen: Heinz-Jeurgen Schreiber, Michele Viti - PowerPoint PPT Presentation

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Page 1: Energy Spectrometer for the ILC

Energy SpectrometerEnergy Spectrometerfor the ILCfor the ILC

Alexey LyapinAlexey Lyapin

University College LondonUniversity College London

Page 2: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 2

BPM energy spectrometer BPM energy spectrometer collaborationcollaboration

UCL: Filimon Gournarnis, Alexey Lyapin, Matthew WingUCL: Filimon Gournarnis, Alexey Lyapin, Matthew Wing

Cambridge: Mark Slater, David WardCambridge: Mark Slater, David Ward

RHUL: Stewart BoogertRHUL: Stewart Boogert

DESY-Zeuthen: Heinz-Jeurgen Schreiber, Michele VitiDESY-Zeuthen: Heinz-Jeurgen Schreiber, Michele Viti

JINR (Dubna): Viktor Duginov, Nikolay MorozovJINR (Dubna): Viktor Duginov, Nikolay Morozov

In collaboration with SLAC, KEK, UC Berkley, LLNL, BINP…In collaboration with SLAC, KEK, UC Berkley, LLNL, BINP…

Page 3: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 3

Luminosity spectrumLuminosity spectrum

Precision threshold scan Precision threshold scan measurements:measurements:

Energy loss effects have to Energy loss effects have to be taken into accountbe taken into account

Absolute beam energy Absolute beam energy measurement of 1 part in 10measurement of 1 part in 1044

Spectrometers up- and Spectrometers up- and downstreamdownstream

Page 4: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 4

BPM spectrometer BPM spectrometer requirementsrequirements

ChicaneChicane 4 magnets 4 magnets 5 mm maximum 5 mm maximum

deflectiondeflection Bipolar operationBipolar operation

Measurement timeMeasurement time Single bunchSingle bunch Bunch trainBunch train 1 hour / 1 day1 hour / 1 day

Dipole magnet

BPM triplet

Mode of operation affects BPM Mode of operation affects BPM designdesign Operation of chicane (frequency Operation of chicane (frequency

of ramping)of ramping) Frequent return to low energy?Frequent return to low energy? Essential design beam energiesEssential design beam energies

50, 175, 250 & 500 GeV50, 175, 250 & 500 GeV Move BPMs to null dipole signalMove BPMs to null dipole signal

Single bunch information useful for Single bunch information useful for machine operation?machine operation?

Page 5: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 5

BPMs in the spectrometerBPMs in the spectrometer

Essential part of diagnosticEssential part of diagnostic 9 BPMs per spectrometer x 4 beam lines 9 BPMs per spectrometer x 4 beam lines

~36 BPMs~36 BPMs Requirements different from Linac BPM Requirements different from Linac BPM

requirementsrequirements Requires detailed design work nowRequires detailed design work now

Page 6: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 6

Spectrometer BPM Spectrometer BPM requirementsrequirements

Spectrometer BPM will probably set Spectrometer BPM will probably set the most stringent requirements on the most stringent requirements on BPM designBPM design ApertureAperture Resolution Resolution Dynamic range (1000:1)Dynamic range (1000:1) Stability (intrinsic and Stability (intrinsic and

electronics)electronics) AccuracyAccuracy CalibrationCalibration BackgroundsBackgrounds

Existing BPM designs are far from Existing BPM designs are far from optimal for an energy spectrometeroptimal for an energy spectrometer Button and strip-line not Button and strip-line not

seriously consideredseriously considered ATF/ATF2 - aperture ATF/ATF2 - aperture Reentrant resolution/stability?Reentrant resolution/stability? Generic pill box cavityGeneric pill box cavity

MachineMachine Bunch angle, position & charge Bunch angle, position & charge

jitterjitter ApertureAperture

SpectrometerSpectrometer Movement rangeMovement range

Stray fieldsStray fields Emittance dilutionEmittance dilution

BPMBPM Resolution already achieved Resolution already achieved

(See ATF results)(See ATF results) Scaling of resolution as function Scaling of resolution as function

of cavity sizeof cavity size Design for stability (monopole Design for stability (monopole

rejection)rejection)

Page 7: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 7

NanoBPM collaboration at NanoBPM collaboration at ATFATFKEK BPMs on flexure piezo moversKEK BPMs on flexure piezo movers BINP BPMs in SLAC/LLNL frameBINP BPMs in SLAC/LLNL frame

Experiment to test the best BPM resolution among with Experiment to test the best BPM resolution among with the other BPM properties, systematics and stabilitythe other BPM properties, systematics and stability

Page 8: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 8

Results from ATFResults from ATF April 2006 dataApril 2006 data

Fitting algorithmFitting algorithm Calibration using hexapod Calibration using hexapod

moversmovers Resolution for the best Resolution for the best

runs ~ 18 nmruns ~ 18 nm Short and long term drifts Short and long term drifts

less than 100 nmless than 100 nm LO sources locking LO sources locking

improvedimproved KEK BPMs coupling to the KEK BPMs coupling to the

reference cavity fixedreference cavity fixed Cross-calibration with Cross-calibration with

corrector magnetscorrector magnets

Page 9: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 9

SLAC ESA spectrometer SLAC ESA spectrometer activitiesactivities

Two more runs next year Two more runs next year with magnets installedwith magnets installed

Planning to add/replace Planning to add/replace BPMs around 2007 with BPMs around 2007 with higher resolution ones higher resolution ones now designed in UCLnow designed in UCL

One of the primary tests is a 4-One of the primary tests is a 4-magnet chicane spectrometermagnet chicane spectrometer

High energy beam testHigh energy beam test Commissioning run in Jan 2006 to Commissioning run in Jan 2006 to

test the BPMs and electronics, other test the BPMs and electronics, other diagnostics installeddiagnostics installed

Preliminary old (not nano-) cavity Preliminary old (not nano-) cavity BPM resolution with the new BPM resolution with the new electronics ~1electronics ~1μμmm

Page 10: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 10

End station A programeEnd station A programe

Plans to test chicane ideas at ESAPlans to test chicane ideas at ESA Using old SLAC cavities Using old SLAC cavities Test of chicane ideas and Test of chicane ideas and

identification of possible identification of possible problems problems

Test system of other general ILC Test system of other general ILC and spectrometer specific BPM and spectrometer specific BPM designs designs

New RF electronicsNew RF electronics Resolution ~1Resolution ~1mm

First tests in January and April 2006, First tests in January and April 2006, chicane tests in 2007…chicane tests in 2007…

Page 11: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 11

Results from ESAResults from ESA Commissioned 2 BPM Commissioned 2 BPM

triplets, including the triplets, including the new Linac BPMsnew Linac BPMs

Resolution dataResolution data Resolutions of <1Resolutions of <1µm µm

were achievedwere achieved Dynamic range Dynamic range

+/- 1 mm+/- 1 mm Resolution of the Resolution of the

Linac BPMs still Linac BPMs still worse (few µm), worse (few µm), should improve should improve significantly with the significantly with the analysis tuned to the analysis tuned to the different decay different decay rate/bandwidthrate/bandwidth

Page 12: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 12

Results from ESAResults from ESA

BPM alignmentBPM alignment 3 sets aligned within +/- 200 3 sets aligned within +/- 200 µmµm Distance between sets ~20 mDistance between sets ~20 m

Page 13: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 13

Need optimized BPM designNeed optimized BPM design

Cavity BPMs, no alternative yetCavity BPMs, no alternative yet Positive experience with ATF/ATF2 cavitiesPositive experience with ATF/ATF2 cavities Need a bigger aperture for machine Need a bigger aperture for machine

protectionprotection Scale ATF2 design to a lower frequencyScale ATF2 design to a lower frequency

Page 14: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 14

ATF2 QBPMsATF2 QBPMs

First nanoBPM for First nanoBPM for serial production! serial production! (~30 units to be (~30 units to be produced for produced for ATF2)ATF2)

Electrical design done by UCLElectrical design done by UCL Several prototypes successfully testedSeveral prototypes successfully tested Good performance observedGood performance observed At least 40 dB isolation between x and At least 40 dB isolation between x and

y channels measured after tuningy channels measured after tuning Successful tests with dedicated Successful tests with dedicated

electronicselectronics

Page 15: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 15

2.8 GHz cavity design in 2.8 GHz cavity design in progressprogress

Robustness vs. high sensitivity and Robustness vs. high sensitivity and compactness optimumcompactness optimum

Tuning to 2876 MHzTuning to 2876 MHz Reduced Q to keep the decay time Reduced Q to keep the decay time

smallsmall Use nanoBPM analysis – keep similar Use nanoBPM analysis – keep similar

processed signal propertiesprocessed signal properties Almost the same sensitivity as for Almost the same sensitivity as for

BPMs in nanoBPM experiment at ATF BPMs in nanoBPM experiment at ATF beam, expect a resolution < 100 nmbeam, expect a resolution < 100 nm

Planning to test in ESAPlanning to test in ESA

Page 16: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 16

Prototype Al modelPrototype Al model

Planning to do cold tests before producing a vacuum prototype, a model is Planning to do cold tests before producing a vacuum prototype, a model is being produced in UCL workshopbeing produced in UCL workshop

Going to introduce an asymmetry (one slot will be off axis), also reduced the Going to introduce an asymmetry (one slot will be off axis), also reduced the waveguide length in order to see the monopole mode coupling; this should waveguide length in order to see the monopole mode coupling; this should allow us to set reasonable tolerances, benchmark the simulation code, and allow us to set reasonable tolerances, benchmark the simulation code, and choose a reasonable waveguide lengthchoose a reasonable waveguide length

Page 17: Energy Spectrometer for the ILC

EUROTeV meeting, LAL,May 2006 17

ILC spectrometerILC spectrometerSpectrometer analysis:Spectrometer analysis: Started with a simulation of Started with a simulation of

systematic effects in the systematic effects in the spectrometer chicanespectrometer chicane

Backgrounds simulationBackgrounds simulation Improving existing analysis of Improving existing analysis of

the impact of the spectrometer the impact of the spectrometer chicane on the beam (energy chicane on the beam (energy bandwidth etc)bandwidth etc)

Joined the efforts with all Joined the efforts with all European institutions involvedEuropean institutions involved