Feedback System Design Alessandro Drago SuperB Meeting 26-30 January 2000 SLAC.

Slides:



Advertisements
Similar presentations
Measurements of adiabatic dual rf capture in the SIS 18 O. Chorniy.
Advertisements

1 Design of a Mixed-Signal Feedback Damper System Michael J. Schulte * Some slides are provided by Craig Deibele (Oak Ridge National Laboratory) and Anil.
Managed by UT-Battelle for the Department of Energy Status and Implementation of Wideband Feedback System for e-p Instabilities in SNS Craig Deibele, Z.
Damping ring K. Ohmi LC Layout Single tunnel Circumference 6.7 km Energy 5 GeV 2 km 35 km.
ALPHA Storage Ring Indiana University Xiaoying Pang.
F Tevatron Software Digital Receiver Beam Line Tuner Vic Scarpine Instrumentation Instrumentation Meeting July 13, 2005.
3/7/05A. Semenov Batch-by-Batch Intensity Monitor 1 Two-Channel Batch by Batch Intensity Monitor for Main Injector BBI.
STRIPLINE KICKER STATUS. PRESENTATION OUTLINE 1.Design of a stripline kicker for beam injection in DAFNE storage rings. 2.HV tests and RF measurements.
Electronics for PS and LHC transformers Grzegorz Kasprowicz Supervisor: David Belohrad AB-BDI-PI Technical student report.
KICKER LNF David Alesini LNF fast kickers study group* * D. Alesini, F. Marcellini P. Raimondi, S. Guiducci.
DLS Digital Controller Tony Dobbing Head of Power Supplies Group.
Feedback on Nanosecond Timescales (FONT) - Review of Feedback Prototype Tests at ATF(KEK) Glenn Christian John Adams Institute, Oxford for FONT collaboration.
Font 4 Review Digital Feedback System BPM Analogue Processor Digital Processor Feather Kicker Power Amplifier Pick up StriplinesKicker StriplinesBeam.
BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.
Digital Signal Processing and Generation for a DC Current Transformer for Particle Accelerators Silvia Zorzetti.
INTRODUCTION  RECYCLER BPM – Original system not adequate to measure beam position precisely. It is being upgraded to meet the required physics precision.
History and motivation for a high harmonic RF system in LHC E. Shaposhnikova With input from T. Argyropoulos, J.E. Muller and all participants.
S. De Santis “Measurement of the Beam Longitudinal Profile in a Storage Ring by Non-Linear Laser Mixing” - BIW 2004 May, 5th Measurement of the Beam Longitudinal.
FAST KICKER STATUS Fabio Marcellini On behalf of LNF fast kickers study group* * D. Alesini, F. Marcellini P. Raimondi, S. Guiducci.
LLRF-05 Oct.10,20051 Digital LLRF feedback control system for the J-PARC linac Shin MICHIZONO KEK, High Energy Accelerator Research Organization (JAPAN)
Initial Performance Results of the APS P0 (Transverse Bunch-to-Bunch) Feedback System N. DiMonte#, C.-Y. Yao, Argonne National Laboratory, Argonne, IL.
January 19, 2006PEP TFB R.Akre PEP II Transverse Feedback System Ron Akre William Colocho Anatoly Krasnykh Vojtech Pacak Dmitry Teytelman Uli Wienands.
F Beam Line Tuners Vic Scarpine Instrumentation DoE Review Oct 28-31, 2002.
Fast feedback, studies and possible collaborations Alessandro Drago INFN-LNF ILCDR07 Damping Rings R&D Meeting 5-7 March 2007.
The Quadrupole Pick-up in the CPS -intro and progress report PPC 3 Dec 1999 A. Jansson.
F Fermilab July 6, 2005Recycler Damper Stability1 Recycler Damper High Frequency Stability Jim Crisp
High Bandwidth damper Input from W.Hölfe Acknowledgement to all collaborators at SLAC, INFN, LBNL and CERNL Presentation of recent MD results (J.Cesaratto):
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
A Possibility of Constant Energy Extraction at ATF2 A.Kalinin Accelerator Science and Technology Centre Daresbury Laboratory Warrington UK FONT Meeting.
E-cloud studies at LNF T. Demma INFN-LNF. Plan of talk Introduction New feedback system to suppress horizontal coupled-bunch instability. Preliminary.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
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.
Experience and Perspectives of Transverse Feedback Systems for Scrubbing Thanks to: SPS OP crew and colleagues from BE-ABP and BE-RF, for their support.
U. Raich CERN Accelerator School on Digital Signal Processing Sigtuna Digital Signal processing in Beam Diagnostics Lecture 1 Ulrich Raich CERN.
12/16/03Tev BPM requirements1 Tevatron BPM requirements Mike Martens.
1 Experiments with pulse supplies and strip-lines at ATF, Plans for fast extraction kicker for ATF2 1. Fast Kicker R&D at ATF 2. Instrumentation at ATF.
IoP HEPP/APP annual meeting 2010 Feedback on Nanosecond Timescales: maintaining luminosity at future linear colliders Ben Constance John Adams Institute,
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.
Characterization of the Fast Ion Instability at CesrTA David Rubin Cornell University.
Beam Diagnostics Seminar, Nov.05, 2009 Das Tune-Meßverfahren für das neue POSI am SIS-18 U. Rauch GSI - Strahldiagnose.
Beam dynamics in crab collision K. Ohmi (KEK) IR2005, 3-4, Oct FNAL Thanks to K. Akai, K. Hosoyama, K. Oide, T. Sen, F. Zimmermann.
LFB, LLRF, TFB Alessandro Drago Annecy, March 2010.
Summary of ions measurements in 2015 and priorities for 2016 studies E. Shaposhnikova 3/02/2016 Based on input from H. Bartosik, T. Bohl, B. Goddard, V.
Beam Instrumentation of CEPC Yue Junhui (岳军会) for the BI Group Accelerator Center, IHEP HF2014.
Electron cloud feedback collaboration meeting Participants: ANL: Kathy Harkay SNS: S. Cousineau, S. Henderson, Jeff Holmes, Y. Sato SLAC: A. Chao LANL:
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
LFB, LLRF, TFB update Alessandro Drago XIII SuperB General Meeting Isola d’Elba, 5/30-6/
Multi-bunch Feedback System Review and Challenges for 1-2GHz Japan Synchrotron Radiation Research Institute (JASRI) SPring-8 T. Nakamura CFA Beam Dynamics.
Feedback Systems Update Alessandro Drago SuperB General Meeting Perugia June 2009.
RF manipulations in SIS 18 and SIS 100 O. Chorniy.
RF acceleration and transverse damper systems
Dither Luminosity feedback versus Fast IP feedback
Glen White, SLAC Jan th ATF2 Project Meeting, KEK
Bunch-by-bunch feedbacks and Low Level RF
Working groups status report on Feedbacks
Feedback systems and Low Level RF
Feedbacks for low emittance accelerators
Horizontal e+ instability Study & Solution
P. Forck, P. Kowina, M. Schwickert, R. Singh
M. Mehler1), H. Klingbeil1), B. Zipfel2)
Fill-pattern Control System for KEKB
Limits on damping times
Chapter 6 Discrete-Time System
The performance requirements for DSP applications continue to grow and the traditional solutions do not adequately address this new challenge Paradigm.
Accelerator R&D Results from the B-factory
Feedback Systems in Circular Colliders
Lecture 6 ACCELERATOR PHYSICS HT E. J. N. Wilson
PSB magnetic cycle 900 ms MeV to 2 GeV
Presentation transcript:

Feedback System Design Alessandro Drago SuperB Meeting January 2000 SLAC

Main Topics SuperB parameters for feedback design Design general consideration R & D main list Scalability Innovation Conclusion

SuperB Parameters From M.Biagini Elba’08

SuperB feedback parameters FB Sampling frequency476MHz Harmonic number2850 Revolution period~ 6us Stored bunches~1250 (2500)Ph-1 ( Ph-2) Bucket length~2ns Ph-1 (ph-2) bunch spacing1.26 (.63)m n s HER/LER0.0141/ Synchrotron frequency~2.35/2.2kHz Longitudinal damping time~20ms n x,y HER/LER0.52/.54 (???) Betatron frequency86.8/90.2kHz Transverse damping time40ms Transv. feedback expected damping time>120 (> 20 turns) us Power amplifier (long.)4x250W Power amplifier (trasv.)2x500W Trasverse kickers (1xV, 1xH)2-portsStripline type Longitudinal kicker4-portsCavity type

Considerations on H H, harmonic number=2850 Still if the stored bunches will be ~1250 (PH1) & ~2500 (PH2) to let ion clearing gaps, from a feedback point of view all buckets (2850=H) have to be processed H=2850 = 2*1425 =2*5*285=2*5*5*57 that is not exactly a wonderful number for FB’s 1056 dsp: 1056=2*2*2*2*2*3*11 DAFNE_H=120=2*2*2*3*5 PEPII_H=3492 [with revolution period 7.336us ] 3492 = 1746*2 = 2*2*3*3*97 In conclusion, for H, highly composed numbers are better than prime numbers

Key points for starting to write a TDR for b-b-b feedback system Innovation Costs Manpower for design Design duration (on years timescale) Design robustness /self & beam diagnostics Compatibility for new upgrade Flexibility Scalability Maintenance & manpower necessary for maintenance

Key points for starting TDR / 2 Consequences: –Design based on last version components –Design based on stable (popular) components –Recycle what doesn’t need changes –Unified technology choices as much as possible –Scale savings –Easy interface for not expert operators

Key points for starting TDR / 3 Consequences of second orders: –Every design based on old FPGA (as iGp with V-II) should migrate to last version FPGA (as Xilinx V5) –Unified technology choices lead to possibly use same tools, parts or designs for similar systems: Transverse feedback Longitudinal feedback Fast IP feedback Timing/injection system (pulse generator) Low level RF 1-D Bunch-by-bunch and turn-by-turn diagnostics, as for example transverse and longitudinal dimension/position detectors 2D Bunch-by-bunch and turn-by-turn diagnostics, as for example profile monitor, etc.

Design robustness Self diagnostics: internal efficient tools to identify quickly correct operation of every subsystem Easy timing procedures Beam diagnostics, in particular instability grow rate measurements Easy access for non expert operators

e+ instability grow rates versus Δνx in PS1-PS2 and RCR OPTICS: Collision mode m = -1 (blue) Δνx = (PS1÷PS2) νx = νy mode m = 0 (red) Δνx = (0.5 in PS1÷PS2 0.5 in RCR) νx = νy mode m = -1 (cyan) This is to study the e+ instability as a function of the relative phase advance between the WGLs

Hor. e+ grow rates, August 4, 2005Hor. e+ grow rates, 2004 In the past years, troubles were much smaller!!!

e+ instability grow rates versus orbit in the main ring dipoles The orbit variation is performed changing the RF frequency and then compensating the beam energy

e+ instability grow rates versus orbit in the main ring dipoles The orbit variation shows important differences from the point of view of understanding the instability source but not to solve completely the e+ current threshold

Scalability Double feedback in the same oscillation plane to use at the best the power output A proved example of the scalability advantages Possibility to have and manage easily more than one feedback in a single oscillation plane Capability to damp coherent high order modes even if faster than foreseen

New e+ Transverse Horizontal Feedback The damping times of the two feedbacks add up linearly Damping time measured: ~100 ms-1 (1 FBKs)  fb damps in 30 revolution periods (~10 us) ~200 ms-1 (2 FBKs)  fb damps in 15 revolution periods (~ 5 us) The power of the H FBK has been doubled

Hybrid Kicker e- ring old pulser horizontal fdbk horizontal fdbk e+ ring

Single horizontal feedback: I=560mA, mode -1 [=119], grow=34.5 (ms-1), damp=-127(ms-1)

Double horizontal feedback: I=712mA, mode -1 [=119], grow=43.7 (ms-1), damp=-233 (ms-1 ) Damping time in 4.3 microsecond i.e. in ~13 revolution turns

Grow rates at higher e+ current, instability controlled by 2 feedback: the unstable mode changes becoming slower! m=-1 m=-2 m=-3 The beam current does not seem limited by the horizontal instability

Innovation

R&D feedback for low emittance accelerator (proposed in July 08 MiniMac) R&D list includes: 1)very low noise analog front n*RF [n=3?] 2)maintain low cross-talk between adjacent bunches under 40 dB (better 60 dB) in front end 3)dual separated timing to pilot the backend power stage 4)digital processing unit with high dynamic range (12/16 bits) > 60dB 5)“dual gain” approach to minimize residual beam motion and feedback noise on the beam [in digital processing unit] 6)integrated beam-feedback model with easy code and parameter download to digital processing unit

Considering a feedback upgrade for low emittance accelerators -Feedback are active system and can have strong negative impact on very low emittance beams -The basic ideas of the upgrades consist in making the noise in the feedback loop as low as possible, and this means: -a) Filtering at the best the external noise, i.e. coming or generated outside the feedback -b) Reducing the internal noise, i.e. the noise coming from parts in the feedback system -c) Reduce the crosstalk between bunch signals

R & D areas Analog R&D: Front End / Back End / transverse /longitudinal Digital processing unit R&D Beam/feedback Model R&D for coefficient generation/maintenance other important design areas: –Power amplifiers R&D: not strictly necessary but the high cost of commercial power devices could justify a R&D –Longitudinal & transverse kickers –Beam signal pickups

The dynamic range in DAFNE feedback analog blocks is in the range 78 dB – 88 dB

ADC dynamic range versus # of bits 7.5_bit ADC_= dB } very poor dyn.range ! 8_bit ADC _ = dB 10_bit ADC _= dB 12_bit ADC _= dB 14_bit ADC _= dB [best value considering the analog blocks!] 15_bit ADC _= dB 16_bit ADC = dB 24_bit ADC = dB Note: in general at least 0.5 bit (= 3dB) is not effective in the conversion

A factor liming the effectiveness of the ADC is the sampling clock jitter. I can suppose that a realistic value of the RMS jitter for the timing signal will be ~0.5 ps This value must be included in SuperB Timing specifications In this case (yellow trace), the ADC dynamic range should be better than 60 dB (12bits)

FIR The core of a feedback digital processing unit is the FIR filter (=Finite Impulse Response filter) An FIR filter can have any kind of coefficients and transfer functions but the output y is always built as y = sum i (c i *x i ) i = number of taps (of the filter) c i = “static” but downloadable coefficients x i = previuos i input values for each bunches

2001 VIRTEX-II [used in iGP]

Virtex-5 has 1056 DSP48 and 550MHz clock speed

Ready for R&D: a Xilinx board with 288 digital signal processors inside

The last version of feedback system (the “iGp”) is built around a Virtex-II FPGA by Xilinx Virtex-II, aging ~10 years, has 168 multiplier blocks, as shown in the Xilinx table below The internal clock speed is 420MHz

Conclusions Feedback systems needs internal and beam diagnostics tools The instability grow rates measured by FB show a good agreement with e-cloud model and simulations It is possible manage more power in the feedbacks installing as many systems as necessary Two separate feedback systems for the same oscillation plane work in perfect collaboration doubling the damping time DAFNE feedback damping time is 4.3 microsecond i.e. ~13 revolution turns, this value can be used to design the SuperB feedback system