Title: HOM Studies at the FLASH(TTF2) Linac
1HOM Studies at the FLASH(TTF2) Linac
- Nathan Eddy, Ron Rechenmacher, Luciano Piccoli,
Marc Ross - FNAL
- Josef Frisch, Stephen Molloy
- SLAC
- Nicoleta Baboi, Olaf Hensler
- DESY
2FLASH Facility (formerly TTF2)
- 1.3 GHz superconducting linac
- 5 current accelerating modules, with a further
two planned for installation. - Typical energy of 400 750 MeV.
- Bunch compressors create a 10 fs spike in the
charge profile. - This generates intense VUV light when passed
through the undulator section (SASE). - Used for ILC and XFEL studies, as well as VUV-FEL
generation for users.
3Higher Order Modes in Cavities
- In addition to the fundamental accelerating mode,
cavities can support a spectrum of higher order
modes. - Traditionally they are seen as bad.
- Beam breakup (BBU), HOM heating,
- Here we investigate their usefulness,
- Beam diagnostics
- Cavity alignment
- Cavity diagnostics
4TESLA Cavities
- Nine cell superconducting cavities.
- 1.3 GHz standing wave used for acceleration.
- Gradient of up to 25 MV/m.
- Addition of piezo-tuners and improvement of
manufacturing technique intended to increase this
to 35 MV/m. - HOM couplers with a tunable notch filter to
reject fundamental. - One upstream and one downstream, separated by
115degrees azimuthally. - Couple electrically and magnetically to the
cavity fields.
5Response of HOM modes to beam
6Sample HOM Spectrum
7HOMs as a Beam Diagnostic
- Beam Position Monitoring
- Dipole mode amplitude is a function of the bunch
charge and transverse offset. - Exist in two polarisations corresponding to two
transverse orthogonal directions. - Not necessarily coincident with horizontal and
vertical directions due to perturbations from
cavity imperfections and the couplers. - Problem polarisations not necessarily
degenerate in frequency. - Frequency splitting lt1 MHz (of same size as the
resonance width). - Beam Phase Monitoring
- Power leakage of the 1.3 GHz accelerating mode
through the HOM coupler is approximately the same
amplitude as the HOM signals. - i.e. Accelerating RF and beam induced monopole
modes exist on same cables. - Compare phase of 1.3 GHz and a HOM monopole mode.
8Narrow-band Measurements
- 1.7 GHz tone added for calibration purposes.
- Cal tone, LO, and digitiser clock all locked to
accelerator reference.
- Dipole modes exist in two polarisations
corresponding to orthogonal transverse
directions. - The polarisations may be degenerate in
frequency, or may be split by the perturbing
affect of the couplers, cavity imperfections,
etc. - May be difficult to determine their frequencies.
9Method
- Steer beam using two correctors upstream of the
accelerating module. - Try to choose a large range of values in (x,x)
and (y,y) phase space. - Record the response of the mixed-down dipole mode
at each steerer setting.
10Singular Value Decomposition (SVD) to Find Modes
- Collect HOM data for series of machine pulses
with varying beam orbits - Use SVD to find an orthonormal basis set.
- Select 6 largest amplitude modes
- Calculate mode amplitudes
- Linear regression to find matricies to correlate
beam orbit (X,X,Y,Y), and mode amplitudes - Use SVD modes and amplitudes to measure position
on subsequent pulses
11Singular Value Decomposition
- SVD decomposes a matrix, X, into the product of
three matrices, U, S, and V. - U and V are unitary.
- S is diagonal.
- It finds the normal eigenvectors of the
dataset. - i.e. modes whose amplitude changes
independently of each other. - These may be linear combinations of the expected
modes. - Use a large number of pulses for each cavity.
- Make sure the beam was moved a significant amount
in x, x, y, and y. - Does not need a priori knowledge of resonance
frequency, Q, etc. - Similar to a Model Independent Analysis.
12Predict position at one cavity from positions at
adjacent cavities
X resolution 6.1µm
Y resolution 3.3 µm
13Cavity Alignment ACC5
- X 240 micron misalignment, 9 micron
reproducibility - Y 200 micron misalignment, 5 micron
reproducibility
14Multi-Bunch Processing
15Multi-Bunch Processing
16Multi-Bunch Initial Results
17HOM as BPM in DOOCs
VME HOM Front-End
Display X, X Y, Y
DOOCs
DataBase
Matlab Vectors Calibration Constants
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21HOM BPM Details
Raw Data
Mode Vectors
Amplitudes
k 6, j 100 to 4k
Calibration Matrix
4D Position
22DESY System
- Need to read out raw data for modcavcoupler
channels at 4k to 10k data points per for
multibunch then perform dot products to determine
mode amplitudes - This requires a lot of I/O in the front-end
(slow) and then a bunch multiply accumulates
which must be done sequentially on the front-end
processor - The current system is unable to report a position
for every pulse at 5Hz for single bunch even with
only a few cavities per module enabled
23Custom FPGA Based Board
- Extreme flexibility inherent in FPGA
- Algorithms and functionality can be changed and
updated as needed - Code base which can be used for multiple projects
- Intellectual Property (IP) cores provide off the
shelf solutions for many interfaces and DSP
applications - The speed of parallel processing
- Can perform up to 512 multiplies using dedicated
blocks - The Pipeline nature of FPGA logic is able to
satisfy rigorous and well defined timing
requirements
24Dot Product FPGA Implementation
FPGA
ADC
S
xnvn,j
Coupler Data
- Store mode vectors in FPGA RAM
- Perform dot product (multiply accumulate) in FPGA
for digitized data as it arrives from ADC - Simply read out mode amplitudes which are
available as soon as data has arrived - Can perform calculation on all channels in
parallel - Also able to store raw data in internal RAM
25Dedicated HOM BPM Digitizer
- Dedicated HOM Digitizer
- Provide amplitudes in real time
- Reduce front-end processor I/O and load by orders
3-4 orders of magnitude - Maximum rate still limited by front-end I/O
- Provide bunch by bunch data for every pulse
- Design dedicated 8 channel digitizer
- Modify existing design 6 months
- Commissioning time (have prototype already)
- Conservative estimate of 200 per channel
26Broadband System
- Broadband (scope-based) system
- Monitor HOM modes up to 2.5GHz
- Several simultaneous channels (4 or 8)
- Limited dynamic range (8 bit scope)
- Use for Phase measurement
27Monopole Spectrum
- Data taken with fast scope. Both couplers for 1
cavity shown
Note that different lines have different
couplings to the 2 couplers More on this later
Monopole lines due to beam, and phase is related
to beam time of arrival Fundamental 1.3GHz line
also couples out provides RF phase
28Analysis of Monopole Data
- Lines are singlets frequencies are easy to find
- Find real and imaginary amplitudes of the
waveform at the line frequency - Find phase angle for each HOM mode
- Convert phases to times
- Weight the times by the average power in each
line - Correct the scope trigger time using this
weighted average of the times - Calculate the phase of the 1.3GHz fundimental
relative to this new time
29Beam Phase vs. RF Measurement During 5 Degree
Phase Shift
Measure 5 degree phase shift commanded by control
system See about 0.1 degrees of rms
30Summary
- HOMs are useful for diagnostic purposes.
- Beamline hardware already exists.
- Large proportion of linac occupied with
structures. - Beam diagnostics.
- Accelerating RF and beam induced monopole HOM
exist on same cable. - No effect from thermal expansion of cables.
- Can find beam phase with respect to machine RF.
- Dipole modes respond strongly to beam position.
- Can use these to measure transverse beam
position. - Cavity/Structure diagnostics.
- Alignment of cavities within supercooled
structure. - Possibility of exploring inner cavity geometry by
examining HOM output and comparing to simulation.
31Backup Slides
32Intuitive modes?
- This calibration matrix, M, shows how much of
each SVD mode contributes to the modes
corresponding to x, y, (x, y). - Therefore, can sum the SVD modes to find the
intuitive modes. - Lack of calibration tone in the reconstructed
modes, as expected. - Beating indicates presence of two frequencies,
i.e. actual cavity modes are rotated with respect
to x and y. - Could rotate these modes to find orientation of
polarisation vectors in the cavity
33Using SVD
- Using SVD on the (n x j) cavity output matrix, X,
produces three matrices. - U (n x j), S (j x j, diagonal), and V (j x j)
- V contains j modes.
- These are the orthonormal eigenvectors.
- Intuitive modes will be linear combinations of
these. - The diagonal elements of S are the eigenvalues of
the eigenvectors. - i.e. the amount with which the associated
eigenvector contributes to the average coupler
output. - It can be shown that the largest k eigenvalues
found by SVD are the largest possible
eigenvalues. - U gives the amplitude of each eigenvector for
each beam pulse.
34Theoretical Resolution
Energy in mode
Thermal noise
- Corresponds to a limit of 65 nm
- Included 10 dB cable losses, 6.5 dB noise figure,
and 10 dB attenuator in electronics. - Need good charge measurement to perform
normalisation. - 0.1 stability of toroids, to achieve 1 um at 1
mm offset. - Not the case with the FLASH toroids.
- LO has a measured phase noise of 1 degree RMS.
- This will mix angle and position, and will
degrade resolution. - LO and calibration tone have a similar circuit,
and cal. tone has much better phase noise. - Therefore, should be simple to improve.
35HOM Calibration Overview
VME HOM Front-End
TTF2 Correctors BPMs, Etc
Matlab Control Code
Display
Matlab Data Structure
DOOCs
Matlab Analysis Code
Display
Matlab Vectors
36Steering Plots
37Apply calibration to a different dataset
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39Practical system
- Can use 2 LO frequencies to mix both the 1.3GHz,
and the 2.4GHz Homs to a convienent IF (25MHz). - Digitize with same system used for dipole HOM
measurements. - Filters will greatly improve signal to noise
- Dual bandpass for 1.3GHz, and 2.4GHz
- Risk introducing phase shifts from filters
- System low cost couplers already exist,
electronics is inexpensive.
40HOM Downmix Board
IF output amplifier
Mixer
Pre-amplifier
Bandpass filters
Input and sample out
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