HOM Studies at the FLASH(TTF2) Linac - PowerPoint PPT Presentation

About This Presentation
Title:

HOM Studies at the FLASH(TTF2) Linac

Description:

HOM Studies at the FLASH(TTF2) Linac Nathan Eddy, Ron Rechenmacher, Luciano Piccoli, Marc Ross FNAL Josef Frisch, Stephen Molloy SLAC Nicoleta Baboi, Olaf Hensler – PowerPoint PPT presentation

Number of Views:113
Avg rating:3.0/5.0
Slides: 44
Provided by: pcsu151
Category:

less

Transcript and Presenter's Notes

Title: HOM Studies at the FLASH(TTF2) Linac


1
HOM 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

2
FLASH 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.

3
Higher 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

4
TESLA 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.

5
Response of HOM modes to beam
6
Sample HOM Spectrum
7
HOMs 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.

8
Narrow-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.

9
Method
  • 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.

10
Singular 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

11
Singular 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.

12
Predict position at one cavity from positions at
adjacent cavities
X resolution 6.1µm
Y resolution 3.3 µm
13
Cavity Alignment ACC5
  • X 240 micron misalignment, 9 micron
    reproducibility
  • Y 200 micron misalignment, 5 micron
    reproducibility

14
Multi-Bunch Processing
15
Multi-Bunch Processing
16
Multi-Bunch Initial Results
17
HOM as BPM in DOOCs
VME HOM Front-End
Display X, X Y, Y
DOOCs
DataBase
Matlab Vectors Calibration Constants
18
(No Transcript)
19
(No Transcript)
20
(No Transcript)
21
HOM BPM Details
Raw Data
Mode Vectors
Amplitudes
k 6, j 100 to 4k
Calibration Matrix
4D Position
22
DESY 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

23
Custom 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

24
Dot 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

25
Dedicated 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

26
Broadband 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

27
Monopole 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
28
Analysis 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

29
Beam 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
30
Summary
  • 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.

31
Backup Slides
32
Intuitive 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

33
Using 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.

34
Theoretical 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.

35
HOM Calibration Overview
VME HOM Front-End
TTF2 Correctors BPMs, Etc
Matlab Control Code
Display
Matlab Data Structure
DOOCs
Matlab Analysis Code
Display
Matlab Vectors
36
Steering Plots
37
Apply calibration to a different dataset
38
(No Transcript)
39
Practical 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.

40
HOM Downmix Board
IF output amplifier
Mixer
Pre-amplifier
Bandpass filters
Input and sample out
41
(No Transcript)
42
(No Transcript)
43
(No Transcript)
Write a Comment
User Comments (0)
About PowerShow.com