Developing Tune Feedback for PEP-II Alan Fisher SLAC e + e – Factories 2003 October 13–16.

Slides:



Advertisements
Similar presentations
Envelope Detector Conventional DSB-AM signals are easily demodulated by an envelope detector It consists of a diode and an RC circuit, which is a simple.
Advertisements

1 Chelmsford Amateur Radio Society Advanced Licence Course Anthony Martin M1FDE Slide Set 12: v1.4, 2-Dec-2012 (4) Receiver Demodulation Chelmsford Amateur.
Beam-based Measurements of HOMs in the HTC Adam Bartnik for ERL Team, Daniel Hall, John Dobbins, Mike Billing, Matthias Liepe, Ivan Bazarov.
M.Gasior, CERN-AB-BIBase-Band Tune (BBQ) Measurement System 1 Base-Band Tune (BBQ) Measurement System Marek Gasior Beam Instrumentation Group, CERN.
Lock-in amplifiers Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure.
Ion instability at SuperKEKB H. Fukuma (KEK) and L. F. Wang (SLAC) ECLOUD07, 12th Apr. 2007, Daegu, Korea 1. Introduction 2. Ion trapping 3. Fast ion instability.
Designing a Lock-in Amplifier with Analog to Digital Conversion Muir Morrison Rachel Miller Mike Gallaspy.
PEP II Transverse Feedback System Ron Akre Anatoly Krasnykh Uli Wienands MAC April 15, 2004.
Recent observations of collective effects at KEKB H. Fukuma, J. W. Flanagan, S. Hiramatsu, T. Ieiri, H. Ikeda, T. Kawamoto, T. Mitsuhashi, M. Tobiyama,
Spectrum analyser basics Spectrum analyser basics 1.
E+ Tune Measurements for 4-ns Spaced Bunches Tune Measurements of 4-ns spaced bunches: An update of the strides made using the digital BPM system to measure.
Spectrum Analyzer. Another Oscilloscope??? Like an oscilloscope Oscilloscope in time domain Spectrum analyzer in frequency domain (selectable)
Beam commissioning strategy Global machine checkout Essential 450 GeV commissioning System/beam commissioning Machine protection commissioning.
Searching for CesrTA guide field nonlinearities in beam position spectra Laurel Hales Mike Billing Mark Palmer.
PEP-II B Factory Machine Status and Upgrades John T. Seeman for the PEP-II Staff SLAC DOE Site Review April 9, 2003.
Department of EECS University of California, Berkeley EECS 105 Fall 2003, Lecture 2 Lecture 2: Transfer Functions Prof. Niknejad.
June 2-4, 2004 DOE HEP Program Review 1 M. Sullivan for the PEP-II Team DOE High Energy Physics Program Review June 2-4, 2004 PEP-II Status and Plans.
Longitudinal instabilities: Single bunch longitudinal instabilities Multi bunch longitudinal instabilities Different modes Bunch lengthening Rende Steerenberg.
Vibration of the Support Tube: Luminosity Lost and Found Alan Fisher, Jim Turner, Franz-Josef Decker, Mike Sullivan, Clive Field
January 15, 2005D. Rubin - Cornell1 CESR-c Status -Operations/Luminosity December/January vs September/October -Machine studies and instrumentation -Simulation.
W. KozaneckiMCC AP meetiing, 20 May 04 Serendipitous measurement of beam-beam tune shift in the LER  Principle  measure colliding tunes (tune tracker.
Impedance measurements at SLS E. Koukovini-Platia CERN, EPFL TIARA mid-term meeting, Madrid, 13 th June 2012 Many thanks to M. Dehler, N. Milas, A. Streun.
F Tevatron Software Digital Receiver Beam Line Tuner Vic Scarpine Instrumentation Instrumentation Meeting July 13, 2005.
Lock-in amplifiers
Future Very High Luminosity Options for PEP-II John T. Seeman For the PEP-II Team e+e- Factories Workshop October 13-16, 2003.
Over-Sampling and Multi-Rate DSP Systems
OSCILLATORS.
Ni.com Data Analysis: Time and Frequency Domain. ni.com Typical Data Acquisition System.
W. KozaneckiMCC AP meeting, 29 July 04  Goal: measure the luminosity degradation associated with  parasitic crossings  horizontal crossing angle  Principle.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
Witness Bunch Experimental Studies at CESR-TA Robert Holtzapple Alfred University/Cal Poly San Luis Obispo.
Longitudinal transfer function a.k.a. (M 55 ) measurements at the JLab FEL Pavel Evtushenko, JLab  Jlab IR/UV upgrade longitudinal phase space evolution.
6. betatron coupling sources: skew quadrupoles, solenoid fields concerns: reduction in dynamic (& effective physical) aperture; increase of intrinsic &
Eeng Chapter 4 Bandpass Circuits   Limiters   Mixers, Upconverters and Downconverters   Detectors, Envelope Detector, Product Detector  
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
J. Turner 02/07/05 SLAC PEPII Accelerator Physics LER WIGGLER PLAN J. Turner, M. Donald, M. Sullivan, U. Wienands, J. Yocky Motivation and Concerns Details.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
BBQ system Tatiana and Benoit, thanks to a lot of help from Christian Boccard, Marek Gasior and Ralph Steinhagen (BE/BI-QP)
Magnet Motion Produces Luminosity Loss. NLC Feedback Operation Kicker Gain Bunch Charge Measure deflected bunches with BPM and kick other beam to eliminate.
January 19, 2006PEP TFB R.Akre PEP II Transverse Feedback System Ron Akre William Colocho Anatoly Krasnykh Vojtech Pacak Dmitry Teytelman Uli Wienands.
Equalisation.
IP BPM Shift Report FONT Meeting: 22 December 2014 Talitha Bromwich.
Summary of Booster Dampers Systems Dave McGinnis December 7, 2010.
Fast feedback, studies and possible collaborations Alessandro Drago INFN-LNF ILCDR07 Damping Rings R&D Meeting 5-7 March 2007.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
1 Franz-Josef Decker 1 Multi-Bunch Operation for LCLS Franz-Josef Decker March 17, Definitions and goals multi-bunch within.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
BIC Issues Alan Fisher PEP-II Run-4 Post-Mortem Workshop 2004 August 4–5.
ADT Tune Measurement F. Dubouchet, W. Hofle, D. Valuch Acknowledgement: R. Calaga, F. Roncarolo, E. Bravin, shift crews New developments and tests on August.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
R.SREEDHARAN  SOLEIL main parameters  Booster and storage ring low level RF system  New digital Booster LLRF system under development  Digital LLRF.
Orbits, Optics and Beam Dynamics in PEP-II Yunhai Cai Beam Physics Department SLAC March 6, 2007 ILC damping ring meeting at Frascati, Italy.
Beam Physics Issue in BEPCII Commisionning Xu Gang Accelerator physics group.
Chaos and Emittance growth due to nonlinear interactions in circular accelerators K. Ohmi (KEK) SAD2006 Sep at KEK.
Stanford Linear Accelerator Center Ron Chestnut EPICS Collaboration Mtg June 18-20, SLAC Tune Tracker/Feedback Mike Laznovsky.
NLC - The Next Linear Collider Project Keeping Nanometer Beams Colliding Vibration Stabilization of the Final Doublet Tom Himel SLAC NLC MAC review October.
MD377 Schottky diagnostic M. Wendt, M. Betz, T. Lefevre.
ADT kickers and amplifiers in tunnel point 4 of LHC, RB44 and RB46 1 W. Hofle LHC Transverse Damper LARP CM20 Napa April 8-10, 2013 LHC Transverse Damper.
Beam Diagnostics Seminar, Nov.05, 2009 Das Tune-Meßverfahren für das neue POSI am SIS-18 U. Rauch GSI - Strahldiagnose.
SPM Users Basic Training August 2010 Lecture VIII – AC Imaging Modes: ACAFM and MAC Imaging methods using oscillating cantilevers.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
FUNCTION GENERATOR.
Weiming Guo Accelerator Physics Group / ASD Advanced Photon Source
Dither Luminosity feedback versus Fast IP feedback
Lab 2: Simple Harmonic Oscillators – Resonance & Damped Oscillations
Lock-in amplifiers
M. Mehler1), H. Klingbeil1), B. Zipfel2)
Top-Up Injection for PEP-II and Applications to a Higgs Factory
Wednesday Morning 8: :30 end of fill study - octupole polarity inversion (Elias, Tatiana, Alexey, Georges, …): Goal: study the effect of the.
Telecommunications Engineering Topic 2: Modulation and FDMA
Presentation transcript:

Developing Tune Feedback for PEP-II Alan Fisher SLAC e + e – Factories 2003 October 13–16

Tune-Tracker Concept Instead of whole spectrum, just follow the resonance. Don’t use amplitude of peak. –Dithering is required to identify a peak. –Peak height varies with current and luminosity. –Peaks often flat and broad when colliding. Use phase of beam’s response to sinusoidal shake. –Phase drops 180° as frequency scanned across peak. –Adjust frequency to find the middle of this resonance. –No dithering. Slope of phase provides a clear direction. –Little dependence on current or luminosity.

SR830 Lock-In Amplifier Stanford Research Systems digital lock-in amp: –Built-in sine-wave source (or use external reference). –Digital mixer and narrow low-pass filter to isolate signal component at the reference frequency. –Finds amplitude and phase (relative to reference). –Remote control by GPIB. –Similar to our FFT spectrum analyzers, but one frequency at a time. Tune-tracking loop controls lock-in through EPICS. –Computer sets frequency of lock-in, then reads back phase.

Lock-In EPICS Window

Frequency Scans Plots of magnitude and phase taken by stepping the lock-in through a frequency range around the tune peak. For finding the target phase and slope for tracking. Target phase is midpoint of transition. Curve fit performed around target phase. –As wide a range as possible between blue cursors. –Chi-squared cut-off criterion to ignore big wiggles.

LER Amplitude & Phase Scans: No HER Amplitude shows a sharp peak at the tune. Phase drops smoothly by 180°.

Frequency-Scan Control

Schematic of PEP-II Tune Tracker

Colliding away from x  0.5 LER x HER y LER y HER x Frequency (kHz) Amplitude (µV) Phase (degrees)

LER Scans in Collision with x  0.51 Amplitude: Tune spread creates long plateau and multiple peaks. Phase: No longer monotonic for x, which is near 0.5

HER Scans in Collision with x  0.52

Pilot Bunches Broadening of spectrum in collision through beam-beam tune shift. –Hard to restore a previous high-luminosity setup, since the midpoint moves higher as the luminosity is improved. Non-colliding bunches—“pilot” bunches—make a better reference. We add 4 pilots to the end of each ring’s fill pattern. At our working point, with x just above 0.5, they are closest to the resonance. –If these are safe, then the colliding bunches are safe too. –But we sometimes lose them on the half integer or the synchrotron sideband above the half integer.

Gating the Pilot-Bunch Signals Measure the tune response from the pilots only. –A fast RF switch between the hybrids that form  x (or  y) and the mixer directs the bunch signals into two streams. Switches toggle once per turn. –Start and stop times selected by ring timing channels. –Separate mixers to process colliding- and pilot-bunch signals. –Colliding-bunch spectra displayed on spectrum analyzers. –Pilot-bunch outputs go to four tune trackers (one per tune plane) and to another spectrum analyzer. –Tune trackers re-assigned to measure pilots rather than whole train.

Downconverter Schematic

New Pilot-Bunch Downconverter

Switching between Excitation & Feedback Bunch-by-bunch transverse feedback strongly damps bunch motion. To get a good signal from a few pilot bunches: –Apply sinusoidal shaking from tune tracker. –Do not damp the shaking with transverse feedback. A fast RF switch (one per tune plane) toggles on every turn between shaking and damping. –Transverse feedback correction or sine excitation selected.

Pilot-Bunch Tests Last spring, tune gating was set up and timed for the HER and LER x planes only. 4 pilot bunches with by-2 spacing were added to the end of the HER and LER bunch trains (  1000 bunches). –A strong response, with a very sharp tune transition typical of non-colliding bunches. But pilot bunches were often lost on the 0.5 resonance. –Short lifetime for pilots. –Easily driven out by small tune tweaks. Nothing left to measure. –Will this improve when we have better control of beta beat? We re-introduced pilots in the last few days. –Several hours without trouble, but then... –We recovered more of last spring’s luminosity by raising the LER current and lowering the x tune a bit. LER pilots became hard to fill and had a short lifetime. Removed pilots from fill pattern.

From Tune Tracking to Feedback Adjust tune quads in response to tracker measurement. –Feedback loop to hold tune constant. –Optionally, a more complex algorithm: Vary tunes with currents. Loop controlled in EPICS, but moves tune quadrupoles through “multiknobs” in older VMS (SCP) software. –EPICS more flexible; gives access to currents, loss of beam. Operators must use modified tune knobs. –Move feedback setpoints as well as quads. –Otherwise feedback would undo a knob tweak. When beam is lost, tune is knobbed to a no-beam setpoint for filling. Tested for several days in June. –Used whole train rather than vanishing pilots. –HER y feedback ran for days without trouble.

Feedback Flowchart

6/2002: First Tune Feedback, No Pilots No tune feedback LER y feedback also on, G=20% LER abort 2% 20% G=5% 10% 20% HER y drive up 5dB LER tunes knobbed LER skews tweaked HER x and y feedback on, various gains

6/2003: Tune Feedback with LER x Pilots 2003 June 9 10-hour plots of: –Measured tune from tracker –Quadrupole multiknob setting –LER current Feedback on for 3.5 hours. –Intentional perturbations applied, corrected automatically by feedback. –Tune changes held within over 4 top-offs. Test perturbations LER x tune tracker LER x tune knob LER current Feedback on

6/2003: Feedback with Trickle Charge No Pilots

Software for Vanishing Pilots New code written over the summer checks the bunch- current monitor to see if pilots are empty. Also looks for a minimum magnitude for the tracker’s response. Feedback is stopped if the pilots are too small. Then the code seamlessly reverts to an older feedforward algorithm. –Tunes are moved automatically in response to changes in HER and LER currents, based on operator experience. After the pilots are refilled, the feedback takes over again. Code is ready for testing.

Tracker Main Window

Tracker Control Window

Feedback Control Window

Future Plans Near Term –Retime triggers for fast gates, due to new cabling. –Tune up the new mixer chassis for the pilots. –Test new code to see it shift from feedback based on pilot bunches to feedforward based on total currents. –Find a way to avoid losing pilots. Let them collide a bit, with a small tune shift? Long Term –New hardware proposed for transverse feedback. New receiver, new digital delay with more bits. Should then incorporate the RF switches for damping/shaking.