Upload
ariel-gross
View
51
Download
2
Tags:
Embed Size (px)
DESCRIPTION
High Power RF Measurements. Ben Woolley, Amos Dexter , Igor Syratchev . Jan Kovermann, Joseph Tagg HG2013, Trieste June 2013. Outline. Phase Stabilisation of CLIC crab cavities RF distribution to the cavities. Accurate phase measurements and stabilisation system. - PowerPoint PPT Presentation
Citation preview
High Power RF Measurements
Ben Woolley,
Amos Dexter, Igor Syratchev.Jan Kovermann, Joseph Tagg
HG2013, Trieste
June 2013
Outline
Phase Stabilisation of CLIC crab cavities• RF distribution to the cavities.• Accurate phase measurements and stabilisation system.
LLRF for future/current X-Band test stands• Production of vector modulated signals for type II SLED pulse
compressor.• Phase and power measurements of RF signals.• Working example using TWT and SLED II pulse compressor.• Easily transferable to other test stands (e.g. TERA C-band test)
CLIC Synchronisation RequirementCavity to Cavity Phase synchronisation requirement (excluding bunch attraction)
degrees1S
1
c
f7204rmsc
x
Target max. luminosity loss fraction S
f (GHz)
sx (nm) qc (rads)
frms (deg) Dt (fs) Pulse Length (ms)
0.98 12.0 45 0.020 0.0188 4.4 0.156
Estimate RF to beam synchronisation ~ 100 fs (0.43 degrees)
Integration
1)Use over-moded waveguide from klystron to the tee
1)35m of waveguide from the Tee to the cavities,
Scale: 20.3m from cavities to IP
2)Two klystrons with low-level/optical signal distribution.
RF Distribution
Option 1: A single klystron with high level RF distribution to the two cavities.
• Klystron phase jitter gets sent to both cavities for identical path length. Δφ=0.
• Will require RF path lengths to be stabilised to within 1 micron over 40m.
Option 2: A klystron for each cavity synchronised using LLRF/optical distribution.
• Femtosecond level stabilized optical distribution systems have been demonstrated (XFELs).
• Requires klystron output with integrated phase jitter <4.4 fs.
Expected Klystron Stability
• From kinematic model of klystron, phase and amplitude stability depend on gun voltage, V:
• For the Scandinova modulator with measured voltage stability of 10-4 phase and amplitude stability should be 0.12° and 0.013%.
• Active feed-forward or feedback would be needed to gain the required stability of 0.02°.
Waveguide Choice
7
Waveguide type35 meters COPPER
Expansion = 17 ppm/K
Mode Transmission Timing error/0.3°C
Width
Timing error/0.3°C
length
No of modes
WR90(22.86x10.16mm) TE10 45.4% 210.5 fs 498.9 fs 1
Large Rectangular (25x14.5mm)
TE10 57.9% 189.3 fs 507.8 fs 2
Cylindrical r =18mm TE01 66.9% 804.9 fs 315.9 fs 7Cylindrical r =25mm TE01 90.4% 279.6 fs 471.4 fs 17
Copper coated extra pure INVAR 35 meters
Expansion = 0.65 ppm/K
Mode Transmission Timing error/0.3°C
Width
Timing error/0.3°C
length
No of modes
WR90(22.86x10.16mm) TE10 45.4% 8.13 fs 19.04 fs 1
Large Rectangular (25x14.5mm)
TE10 57.9% 6.57 fs 19.69 fs 2
Cylindrical r =18mm TE01 66.9% 30.8 fs 12.1 fs 7Cylindrical r =25mm TE01 90.4% 10.7 fs 18.02 fs 17
Rectangular invar is the best choice as it offers much better temperature stability-> Expands 2.3 microns for 35 m of waveguide per 0.1 °C.
RF path length measurement
48MW 200ns pulsed 11.994 GHz Klystron repetition 50Hz
Vector modulation
Control
Phase Shifter
12 GHz Oscillator
Main beam outward pick up
Main beam outward pick up
From oscillator
Phase shifter trombone
(High power joint has been tested at SLAC)
Magic Tee
Waveguide path length phase and amplitude measurement and control
4kW 5ms pulsed 11.8 GHz Klystron/TWT
repetition 5kHz
LLRF
Phase shifter trombone
LLRF
Cavity coupler 0dB or -40dB
Cavity coupler 0dB or -40dB
Expansion joint
Single moded copper plated Invar waveguide losses over 35m ~ 3dB -30 dB
coupler -30 dB coupler
Forward power
main pulse
12 MW
Reflected power main pulse ~ 600 W
Reflected power main pulse ~ 500 W
Waveguide from high power Klystron to magic tee can be
over moded
Expansion joint
RF path length is continuously measured and adjusted
LLRF Hardware Layout (Low BW)• Fast phase measurements during the pulse (20-30 ns).
• Full scale linear phase measurements to centre mixers and for calibration.
• High accuracy differential phase measurements of RF path length difference (5 μs, 5 kHz).
• DSP control of phase shifters. Linear Phase Detector (1MHz BW)
DSP
ADCADC
MagicTee
To Cavity
To Cavity
Wilkinson splitters
-30 dB coupler
DBM
DBM DBM
10.7GHz Oscillator
-30 dB coupler
Piezoelectric Phase Shifter Piezoelectric phase shifter
DAC1
Amp + LPF
LPFAmp
Power Meter
To DSP DAC2
From DAC2
To Phase Shifter
Calibration Stage
Board Development and CW testsFront end electronics to enable phase to be measure during the short pulses to an accuracy of 2 milli-degrees has been prototyped and dedicated boards are being developed.
PLL controller
MCU
10.7 GHz VCO
Digital phase detector
DBMs
Power Meters
Wilkinson splitter
Inputs
400 ns span:RMS: 1.8 mdeg
Pk-Pk: 8.5 mdeg
90 s span:Drift rate : 8.7 mdeg/10s
Total drift: 80 mdeg
Crab cavity stabilisation: Next steps
LLRF board revision:• Some problems with the PLL and tolerances on the
Wilkinson splitters. (Non equal power splitting).• Investigation into pulsed power operation, effect of
amplitude instabilities and higher order mixing products (not visible in CW tests).
RA joining Lancaster in September to increase/broaden the effort on this project.
Future LLRF Generation and Acquisition for X-band test stands
IF2.4 GHz Oscillator
9.6GHz BPF
Amp
Vector Modulator
RFout
LOin LOout
12GHz vector modulated
signal to DUT
2.9 GHz Oscillator
X4 freq.
RF
LO
LOIF RF
12 GHz BPF
12 GHz BPF
12GHz CW reference
signal
2.4GHz vector modulated
signal
2.4GHz CW reference signal
11.6 GHz BPF
X4 freq.
LO
IF
RF Input 1
400 MHzLPFs
LO
IF
RF Input 2
LO
IF
RF Input 3
LO
IF
RF_Referance12GHz CW reference
signal
3dB hybrid
AmpIF Amps
Oscillators should be phase locked
1.6 GSPS
12-bit ADCs
Digital IQ demodulation
LOADTWT
System Testing: SLED II PC
Phase modulated pulse input
-40 dB coupler
-40 dB coupler
SLED II pulse compressor
RF Input 1RF Input 2 RF Input 3
20 dB attenuator
20 dB attenuator
System Testing: SLED II PCNational Instruments PXI crate containing:
• 2 CW generators for the LOs.
• Vector modulator (up to 6.6GHz) with 200 MSPS I/Q generator
• 5Chs 1.6GSPS 12-bit and 4Chs 250MSPS 14-bit ADC each connected to FPGAs.
• 200 MHz digital I/O board for interlock and triggering signals.
Up/down-mixing components and cabling
TWT: 3kW
10-12GHz
SLED II Pulse compressor
Igor Syratchev
RF Load
Power Meter
LLRF System Test: SLED II PCPhasePower400MHz raw signals
Trans.
Refl.
Inc.
LLRF System Test: Dynamic RangePhasePower400MHz raw signals
40 dB below TWT saturation!
Pulse compressor DetuningPhasePower400MHz raw signals
LLRF system Accuracy IPower accuracy: 0.4%rms Phase accuracy: 0.9°rms
Possible sources of error• Problem with locking between the two CW generators
and the 10MHz system reference caused the signal to beat. This affects acquisition AND vector generation. Proposed solution: Clock ADC’s with 400MHz reference.
• Bit-noise on the ADCs limit accuracy to 0.1% (9.5ENOB).• All harmonics generated by the multipliers and/or mixers
will be mixed down to 400MHz and be indistinguishable from the signal of interest.
400MHz Reference
LLRF system Accuracy II
Comparison with calibrated power meter• Transients at the start of the main pulse
and phase flip are observed (input).• Transients reduced when passed through
the detuned system. Hybrid is narrow band extra filtering of harmonics gives cleaner signal when mixing down.
Input
Output
Calibrated Power Meter
Output:Gain 2.9
Input
TERA C-band Cavity Testing
5.7GHz 4MWMagnetron
Circulator
Directional coupler
Cavity under test
PMT and faraday cup
PXI crate
RF detector diodes, PMT and faraday cup inputs.
Timing board/ trigger generation
Pictures: Alberto Degiovanni
Screenshots from ‘CBOX1’
X-band LLRF: Future Developments
• Characterisation of errors/transients in the system. Both on the generation and acquisition side.
• Miniaturisation of LLRF system components into crate.
• Software: logging, interlock control, timing and triggers etc.
• Integration into XBOX-2 test stand.• Scaling up and integration towards XBOX-3.
22
Thank you for your attention!
Extra Slides
Observed Klystron Stability
• Observed ~5% amplitude jitter on the output of the klystron. This was due to a mismatch in the pulse forming diode in the LLRF network and a triggering error in the ADC firmware.
• Amplitude jitter reduced to ~1-2%.
• Phase measurements will be performed in the coming weeks.
Klystron phase noise• Can use a standard method to measure the phase stability of the klystron.
• Reference source is split such that its phase noise is correlated out by the mixer for both channels.
• Phase shifter adjusted as to bring RF and LO inputs into quadrature.
• Digital scope or ADC and FPGA/DSP preforms FFT analysis, to obtain phase noise curve.
• Experiment can also be repeated for different lengths of waveguide to ascertain the effects of waveguide dispersion.
To Cavity
Wilkinson splitter DBM
12 GHz Oscillator
-57 dB coupler
phase shifter
KlystronTWT
Φ
PIN diodeswitch
Oscilloscope/ADC for FFT analysis
RFLO
IF
Waveguide
Measurement requires good amplitude stability as any AM will be present in the IF.
Waveguide Stability ModelUse ANSYS to find “dangerous” modes of vibration for a 1 m length of waveguide fixed at both ends.Fundamental mode 65.4 Hz
Planned CLIC crab high power tests
Test 1: Middle Cell Testing – Low field coupler, symmetrical cells. Develop UK manufacturing.
Test 2: Coupler and cavity test – Final coupler design, polarised cells, no dampers.Made with CERN to use proven techniques.
Test 3: Damped Cell Testing – Full system prototype
Travelling wave 11.9942 GHz
phase advance 2p/3
TM110h mode
Input power ~ 14 MW
Future
• Continued investigations into the phase stability of the 50 MW X-band klystron.
• Development of feed-forward and/or feedback system to stabilise the klystron’s output.
• Continued characterisation of electronics to obtain stand alone phase measurement/correction system.
• Design/procurement of the waveguide components needed.• Demonstration RF distribution system, with phase stability
measurements. • Perform phase stability measurements during the CTF dog-leg
experiments.
• Measure phase across the prototype cavity during a high power test.
29
LLRF Hardware Layout (High BW)• Fast phase measurements during the pulse (50MHz).
• 400MHz direct sampling to centre mixers and for calibration.
• High accuracy differential phase measurements of RF path length difference (5 μs, 5 kHz).
• DSP control of phase shifters.
1.6 GSPS 12-bit ADC’s
DSP
ADC
MagicTee
To Cavity
To Cavity
Wilkinson splitters
-30 dB coupler
DBM
DBM DBM
11.6 GHz Oscillator
-30 dB coupler
Piezoelectric Phase Shifter Piezoelectric phase shifter
DAC1
Amp + LPF
400MHzLPF
Amp
Power Meter
To DSP DAC2
From DAC2
To Phase Shifter
Calibration Stage