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Transcript of Investigations on BaseBand tune measurements using direct digitized BPM signal - progress report -
![Page 1: Investigations on BaseBand tune measurements using direct digitized BPM signal - progress report -](https://reader030.fdocuments.net/reader030/viewer/2022032414/5681338b550346895d9a9355/html5/thumbnails/1.jpg)
Workshop Chamonix, Dec, 12, 2007
Investigations on BaseBand tune measurements using direct
digitized BPM signal- progress report -
Investigations on BaseBand tune measurements using direct
digitized BPM signal- progress report -
P. Forck, W. Kaufmann, P. Kowina, P. Moritz, U. RauchGSI
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CARE workshop Chamonix, Dec 2007 2Udo Rauch
OutlineOutline
Brief introduction to accelerators at GSI and motivation
Classical measuring method
Short crosslink: direct diode detection
Libera position data as possible data source
Summary and outlook.
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CARE workshop Chamonix, Dec 2007 3Udo Rauch
SIS-18 synchrotron at GSISIS-18 synchrotron at GSI
Important parameters of SIS-18:- Circumference 216 m- Inj. type Multiturn- Energy range 11 MeV → 2 GeV- Acc.RF 0.8 → 5 MHz- Acc. harmonic 4 (no. of bunches)- Bunching factor 0.6 → 0.2- Ramp duration 0.3 → 1.5 s- Typical tune h/v 4.319 3.29- Tune meas. sys. Exciter + BPM
Schottky- Ion range (Z) 1 → 92 (p to U)- Design beams 2 x 10¹¹ U 28+
1 x 10¹³ p
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CARE workshop Chamonix, Dec 2007 4Udo Rauch
SIS-18 synchrotron at GSISIS-18 synchrotron at GSI
Important parameters of SIS-18:- Circumference 216 m- Inj. type Multiturn- Energy range 11 MeV → 2 GeV- Acc.RF 0.8 → 5 MHz- Acc. harmonic 4 (no. of bunches)- Bunching factor 0.6 → 0.2- Ramp duration 0.3 → 1.5 s- Typical tune h/v 4.319 3.29- Tune meas. sys. Exciter + BPM
Schottky- Ion range (Z) 1 → 92 (p to U)- Design beams 2 x 10¹¹ U 28+
1 x 10¹³ p
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CARE workshop Chamonix, Dec 2007 5Udo Rauch
MotivationMotivation
Up to now no tune tracking system yet available at GSI Necessity arises due to upgrade of existing accelerator for higher
beam intensities and/for future accelerator(s) in FAIR project Target
(PLL) tune tracking BaseBand – q Single bunch separation
Two platforms possible for baseband: 3D and direct digitization Earlier recorded data (FFTransformed) show rich amount of not
understood frequency spikes in spectra also in region of baseband (without any beam excitation). Thus: starting with an easy and safe method => noise excitation of sidebands
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CARE workshop Chamonix, Dec 2007 6Udo Rauch
amplifier
amplifier
BPM
hybr
id
BEAM
Exciter
RSA
180 splitter
25 W
50dB
25 W
50dB
digital noise
generator
Digital Random Noise GeneratorDigital Random Noise Generator
RF clock signal
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CARE workshop Chamonix, Dec 2007 7Udo Rauch
amplifier
amplifier
BPM
hybr
id
BEAM
Exciter
RSA
180 splitter
25 W
50dB
25 W
50dB
digital noise
generator
Digital Random Noise GeneratorDigital Random Noise Generator
RF clock signal
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CARE workshop Chamonix, Dec 2007 8Udo Rauch
amplifier
amplifier
BPM
hybr
id
BEAM
Exciter
180 splitter
25 W
50dB
25 W
50dB
digital noise
generator
RSA
Digital Random Noise GeneratorDigital Random Noise Generator
RF clock signal
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CARE workshop Chamonix, Dec 2007 9Udo Rauch
Digital Random Noise GeneratorDigital Random Noise Generator
1 MHz carrier frequencyNumber of harmonics : 1q is set to 0.3 with a dq of 0.01
Frequency sweep (pseudo-RF as input)Number of harmonics : 4q is set to 0.3 with a dq of 0.03
Amplitude and width of excitation can be modified also remote controlled
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CARE workshop Chamonix, Dec 2007 10Udo Rauch
Classical approach: one harmonic onlyClassical approach: one harmonic only
Argon 18+100 ms coolingRamp to 2 GeV in 700 ms
t = 250m
s
11 MeV
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CARE workshop Chamonix, Dec 2007 11Udo Rauch
Classical approach: one harmonic onlyClassical approach: one harmonic only
Argon 18+100 ms coolingRamp to 2 GeV in 700 ms
t = 250m
s
11 MeV
- Only one harmonic- Signal to noise improvable
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CARE workshop Chamonix, Dec 2007 12Udo Rauch
The direct diode detection (principles)The direct diode detection (principles)
Design and realisation by Marek Gasior et al (CERN)
Decay constant: R x C = tau ~ 100 x T
Gain comparedto classical system
G_d = Signal to noise(3d)
Signal to noise (class)
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CARE workshop Chamonix, Dec 2007 13Udo Rauch
The direct diode detection (principles)The direct diode detection (principles)
Design and realisation by Marek Gasior et al (CERN)
Decay constant: R x C = tau ~ 100 x T
Gain comparedto classical system
G_d = Signal to noise(3d)
Signal to noise (class)
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CARE workshop Chamonix, Dec 2007 14Udo Rauch
The direct diode detectionThe direct diode detection
Signal difference 2V (offset α)Betatron oscillation relative amplitude β = 0,05Simulated tune value q = 0,319Filter time constant tau = 50T ( = 200Tb)
CircuitryPrinciplesBy MarekGasior(CERN)
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CARE workshop Chamonix, Dec 2007 15Udo Rauch
The direct diode detection (results)The direct diode detection (results)
SIS - 18
1000 kHz
250 kHz
SIS - 100
278 kHz
185 kHz
Tau=100T
G_d = Signal to noise(3d)
Signal to noise (class)
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CARE workshop Chamonix, Dec 2007 16Udo Rauch
The direct diode detectionThe direct diode detection
Calculation of R and C (and gain factor G)
Dependent on accelerator features:- Pickup capacity- Accelerator cycle (frequency range)- Bunch length and bunching factor
And circuitry features:- Noises induced by analog parts- No notch filter applicable
Accelerator R_fo [MΩ] C_fo [pF] G_d [dB] G_d [factor]
SIS-18 1.72 130.99 8.24 ~2.5
SIS-100 5.57 79.97 27.09 ~24
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CARE workshop Chamonix, Dec 2007 17Udo Rauch
Open questionsOpen questions
Due to our frequency range (0.8-5.5MHz) and the varying bunching factor (0.6...0.2) usability of 3d-method not yet sure
Beam intensities on pickup of SIS-18 vary even within 3s from one cycle to the next by order of up to 5 magnitudes (100dB)
Pre-amplifier between pickup and diode required? one peak detector might not be sufficient (discussion ongoing)
Gain factor significantly lower compared to CERN accelerators because of much longer bunches and the higher revolution frequency
BPM data has large baseline shift which may introduce additional uncertainties
3D-circuitry for SIS-18 not yet finished Test and comparison to ‘direct digital processing’
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CARE workshop Chamonix, Dec 2007 18Udo Rauch
What is LiberaWhat is Libera
Instrumentation Technology (I-Tech) – Libera is an integrated setup using a high resolution ADC for onboard data processing on a FPGA
Input actually is one BPM per Libera: 2 channels horizontally and 2 channels vertically
It is targeted to process data online delivering beam position data with delay of about 3 turns, repetition rate of tune spectra of about 100 Hz (presently only offline)
amplifierADC
and
position evaluation
Computer in control room
amplifier
pick up
4 channel ADC125 MSa / s per channel14 bit resolution256 Mb onboard memory
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CARE workshop Chamonix, Dec 2007 19Udo Rauch
Motivation for digital measuring methodMotivation for digital measuring method
One point per integrated bunch (frequency variation eliminated) -> shift to tune baseband when applying FFT
For digital method bunching factor, baseline shift and frequency range is no problem
Noise averaging thanks to integration of bunch data Bunch by bunch tune separation by software
To do: Gain factor not yet evaluated (about same range as 3D) Total time for real time signal processing not yet estimated
Presently only offline analysis Feedback?
Usage of differential signal instead of single plates Used for “optimization process”
What is needed for position calculation: Windowing data stream for bunch integration Baseline restoring (due to AC coupling)
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CARE workshop Chamonix, Dec 2007 20Udo Rauch
What is data looking likeWhat is data looking like
= 0.8 µs
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CARE workshop Chamonix, Dec 2007 21Udo Rauch
Whole rampWhole ramp
= 0.8 µs
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CARE workshop Chamonix, Dec 2007 22Udo Rauch
Whole rampWhole ramp
= 0.8 µs
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CARE workshop Chamonix, Dec 2007 23Udo Rauch
Whole rampWhole ramp
= 0.8 µs
Data averaging over 1000 bunches
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CARE workshop Chamonix, Dec 2007 24Udo Rauch
Whole rampWhole ramp
= 0.8 µs
Data averaging over 1000 bunches
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CARE workshop Chamonix, Dec 2007 25Udo Rauch
SpectrumSpectrumf /
f_re
v
‘q’
Remark error:
No noise sidebandof DRN generator!(Only carrier freq.)
FFT slidesor Turns / 2048
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CARE workshop Chamonix, Dec 2007 26Udo Rauch
Single bunch behaviourSingle bunch behaviour
Timespan of every figure: 2.6 µsNote bunch spacing
0.14 ms22 Turns
1.62 ms340 Turns
2.22 ms470 Turns
13.72 ms2950 Turns
Time and turns after start of bunch forming
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CARE workshop Chamonix, Dec 2007 27Udo Rauch
Timespan of every figure: 2.6 µsNote window widths!
Time and turns after start of bunch forming
93.94ms25000 Turns
194.39ms75000 Turns
473.27ms300000 Turns
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CARE workshop Chamonix, Dec 2007 28Udo Rauch
Summary and outlookSummary and outlook
- First approach to establish tune measurement system at GSI- Parameters characteristically for 3d – method calculated- First measurements with real electronics for 3d foreseen in spring
2008
- Beam position out of direct digitized data working properly- FFT to tune baseband through bunch – synchronous position data
possible- First measurements promising- Further measurements and theoretical evaluations foreseen
- Many thanks to M. Gasior and R. Steinhagen
AND
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CARE workshop Chamonix, Dec 2007 29Udo Rauch
Thank you for your
attention!
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CARE workshop Chamonix, Dec 2007 30Udo Rauch
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CARE workshop Chamonix, Dec 2007 31Udo Rauch
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CARE workshop Chamonix, Dec 2007 32Udo Rauch
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CARE workshop Chamonix, Dec 2007 33Udo Rauch
The direct diode detectionThe direct diode detection
SPS Parameter / gain factor
Tau als Ebene = RC = 100
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CARE workshop Chamonix, Dec 2007 34Udo Rauch
Data averaging over 1000 bunches
Single bunch position
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CARE workshop Chamonix, Dec 2007 35Udo Rauch
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CARE workshop Chamonix, Dec 2007 36Udo Rauch
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CARE workshop Chamonix, Dec 2007 37Udo Rauch
Data acquisitionData acquisition
pick up amplifier position
evaluation Shift to frequency domain tune?
K = Sondenkonstante
KO = Offset
X
x X OX
X
s K K
( t T / 2) (t T / 2)t
(x x )y x
2
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CARE workshop Chamonix, Dec 2007 38Udo Rauch
The direct diode detection (3D) (principles)The direct diode detection (3D) (principles)
Comparison to Classical Approach:
„one betatron harmonic filtering“
- Considered 4-Sigma bunch length to be about 100 ns- One obtains a cut-off of about 13.3 MHz- Thus low noise amps required because of small signals- Saturation during ramp has to be avoided
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CARE workshop Chamonix, Dec 2007 39Udo Rauch
Some resultsSome results
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CARE workshop Chamonix, Dec 2007 40Udo Rauch
Some resultsSome results
Time span for every actual done Fourier Transformation is 0.5 ms (25000 data points/channel)
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CARE workshop Chamonix, Dec 2007 41Udo Rauch
Some resultsSome results
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CARE workshop Chamonix, Dec 2007 42Udo Rauch
Some resultsSome results
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CARE workshop Chamonix, Dec 2007 43Udo Rauch
Some resultsSome results
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CARE workshop Chamonix, Dec 2007 44Udo Rauch
Results of one ramp cycleResults of one ramp cycle
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CARE workshop Chamonix, Dec 2007 45Udo Rauch
Results of one ramp cycleResults of one ramp cycle
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CARE workshop Chamonix, Dec 2007 46Udo Rauch
Results of one ramp cycleResults of one ramp cycle
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CARE workshop Chamonix, Dec 2007 47Udo Rauch
Results of one ramp cycleResults of one ramp cycle
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CARE workshop Chamonix, Dec 2007 48Udo Rauch
Curiosities (PosSon6)Curiosities (PosSon6)
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CARE workshop Chamonix, Dec 2007 49Udo Rauch
What‘s missingWhat‘s missing
Programming, programming, programming. (matlab, mathematica,…) Calculations Identifying obtained frequencies (tune? Half tune? Amplifier? Power
Plant?) Statistics on when tune is identifiable. More data needed for statistics,
because most of recent collected data is corrupted mostly due to the parasitic frequency on BPM 6
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CARE workshop Chamonix, Dec 2007 50Udo Rauch
The direct diode detection (principles)The direct diode detection (principles)
Scheme, mathematics and plots by Marek Gasior, CERN
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CARE workshop Chamonix, Dec 2007 51Udo Rauch
The direct diode detection (principles)The direct diode detection (principles)
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CARE workshop Chamonix, Dec 2007 52Udo Rauch
The direct diode detection (analytics / results)The direct diode detection (analytics / results)
Calculation of R and C (and gain factor G)
Dependent on:- Pickup capacity- Accelerator cycle- Bunch length- Temperature- Diode leakage current- Spectral noise density and current of Detector Amplifier- Expected tune value
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CARE workshop Chamonix, Dec 2007 53Udo Rauch
Some resultsSome results
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CARE workshop Chamonix, Dec 2007 54Udo Rauch