BPM Energy Spectrometry for ILC Bino Maiheu University College London for LC-ABD WP 4.2 LC-ABD Meeting IPPP Durham, 26 September 2006 LC-ABD Meeting, 26.

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BPM Energy Spectrometry for ILC Bino Maiheu University College London for LC-ABD WP 4.2 LC-ABD Meeting IPPP Durham, 26 September 2006 LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry

Luminosity spectrum, physics case LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Top quark mass scan Uncertainty on beam energy measurement contributes directly to the uncertainty on the ILC physics output... Need for :  energy measurement accuracy  stability and ease of operation  minimal impact on physics data taking Luminosity spectrum Top quark mass scan

BPM based beam energy measurement LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry BPM BPM BPM WP 4.2 mission statement : Study & design magnetic chicane for beam energy measurement using BPMs for a future linear collider Royal Holloway University London: S. Boogert Cambridge : M. Slater, M. Thomson and D. Ward University College London: F. Gournaris, A. Lyapin, B. Maiheu, S. Malton, D. Miller and M. Wing : test resolution, try different analysis methods, BPM stability tests, multi bunch operation, advanced electronics techniques, inclination of beam in BPMs. -> spectrometer aspects of BPMs can be tested : test stability and operational issues with a full implementation of 4 magnet chicane and 3 BPM stations -> test of chicane prototype η ~ 5 mm at center At least δx~ 500 nm needed δE/E ~ 10 -4

NanoBPM at ATF LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Collaboration with LLNL, LBNL, SLAC and KEK KEK BPMs on flexure piezo movers (x,y) BINP BPMs, each on hexapod (x,y,x',y') in SLAC/LLNL frame

BPM signal processing in a nutshell LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry LO RF LO Filters, Amplifier s ADC Filters, Amplifier s Dipole (TM 110 ) : charge + offset + tilt Monopole (TM 010 ) : charge Normalise signal to Ref (Q) Cavity Tilt has π/2 phase difference to position Tilt axis Pos. axis IQ phase Determine Amplitude & Phase Fit waveform : V = V 0 + A e -Г(t-t0) sin[ω(t-t 0 ) + φ]  Fit waveform : V = V 0 + A e -Г(t-t0) sin[ω(t-t 0 ) + φ]  Digital Down Conversion (DDC) :  Multiply waveform with e iωt  Filter out 2ω component  Sample waveform at fixed t0Ref -> A, φ Disentangle charge, offset and tilt :

ATF Results : resolution + systematics LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry  2 stage down mixing, digitizer 14 bit  Precise calibration using hexa-pod movers, cross calibration using corrector magnets  Commissioned nanoGrid system (nm level XY encoder system) to monitor mechanical stability  Best resolution so far :  16 nm  Short and long-term :  drifts < 100 nm  Clear systematic correlation seen Frequency & temperature : ΔT ~ 0.25 K -> Δω ~ 65kHz assuming typical offsets of beam 50 nm systematic scale change

ATF Results : Beam inclination in BPM LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Important for discussion 3 vs. 4 magnet chicane data between and 1000 μrad No significant change in resolution, however : clear change in calibration constants ! IQ Phase Position Scale Probably related to Temp Clear variation with inclination Further investigation ! BPM BPM

ATF Results : multibunch studies LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Cavity BPMs must work with ILC bunch train...  can we measure energy of individual bunches ? ATF multi bunch data: bunch train of 3 bunches (150 ns) proved difficult to steer down -> saturation... Simulation work bunch train: fitting algorithm seems to be performing well  fitting algorithm seems to be performing well  more study needed : phase advance, DDC ?

T474/T491 - LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Collaboration with LBNL ( Y. Kolomensky et al. ), SLAC ( M. Woods et al. ) and Notre Dame ( M. Hildreth et al. ) 20 m SPEAR girder Dipole magnets BPMs 3,4,5 BPMs 9,10,11  January test run 2006 (4 days) : Commissioning of BPMs 31,32 and 1,2 upstream  April run 2006 ( 2 weeks ) :  Commissioning of new ILC prototype linac triplet (BPM 3,4,5), where BPM4 on x,y mover system  Commissioning of old SLAC BPMs (9,10,11)  Digitisation/signal processing optimization  July run 2006 (2 weeks ) :  Commissioning of Zygo interferometer system (BPMs 3,4,5) + energy BPM24 upstream  Further optimisation of hardware (down mixing)  Stability data taking with 10 BPMs, frequent calibrations

BPM systems used in ESA LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry  Rectangular cavities  x and y separated  GHz, high Q ~ 3000  20 mm aperture (0.8 “)  C. Adolphsen, Z. Li  ILC cold linac prototype cavities cavities  36 mm aperture, GHz  low Q (~ 500)  good monopole suppression

ESA Resolution & stability LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Resolution : BPM 3-5: ~ 700 nm in x, BPM 9-11: ~350 nm in x 200 nm 20k pulses ~ 30 min old cavities prototype

Automatic calibration LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Corrector scans / setpoint calibration... lot of manual work needed Automatic setting of correctors with/without  Automatic setting of correctors with/without feedback feedback  Followed by mover scan on BPM4  Set voltage level for each step in ADC  Still need to implement automatic processing Important aspect of future spectrometer operation !

Spectrometer BPM prototype LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Existing BPM designs not optimal for an energy spectrometer  aperture ( machine protection, resolution )  resolution, stability  monopole rejection ( electric center stability )  coupling -> decay time ( multi bunch ) Designed new prototype (A. Lyapin)  30 mm aperture, GHz, 1.3 MHz bandwidth  theoretical resolution ~ 11.2 nm  Al prototype by UCL workshop, Cu vacuum beam prototype by Mullard Space Science Lab (MSSL) prototype by Mullard Space Science Lab (MSSL) Proposed electronics scheme Al prototype

Aluminium prototype for new BPM LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Al prototype is done & ready for measurements at UCL & RHUL Feed through Waveguide structure Cavity (upside down) Front face Fully assembled prototype Alex

Chicane simulation LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Currently most simulation work just generates “sampled waveforms” Developing core library for full simulation :  Uses physical units ( easily portable between e.g. KEK & SLAC )  Portability between platforms, e.g. import into LabVIEW  Simulation of electronics : conversion loss, non linearity, digitization etc...  Contains analysis routines as well -> simulation & real data analysis based upon idential set of routines idential set of routines RealBPM cavityparametersimulation Waveformsimulation reconstructi on libespec analysis Electronic s digitisatio n Electronic s digitizatio n simulation ChicanesimulationGEANT/BDSIM firstimplementation (GdfidL) Already contains a lot of functionality cross check with ESA data production underway

Future plans LC-ABD Meeting, 26 Sep – Bino Maiheu : BPM Energy Spectrometry Plans for ATF :  long term stability studies  multi bunch and additional tilt & spectrometer related tests  use nanoGrid system to monitor mechanical stability of spaceframe  new BPMs are planned to be installed to replace the KEK ones Plans for ESA :  Install 4 old refurbished magnets in beam line to form chicane (Jan. '07)  Install & commission new spectrometer BPM prototype complete with temperature readout and x,y mover system complete with temperature readout and x,y mover system  Commission constant calibration tone system to monitor gain drifts in electronics in electronics  Link BPM stations with interferometer system (M. Hildreth) Plans for LC-ABD 2 :  Develop BPM triplet to be deployed at mid-chicane location  Long term tests of UK designed spectrometer specific BPMs