Title: Undulator Prototype Status and Plans
1Undulator Prototype Status and Plans
2Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Improvements
- Canted Pole Undulator Measurements
- Plans
- Summary
3Undulator Design Parameters
Parameter Specified Value
Undulator Type Planar Hybrid
Magnet Material NdFeB
Pole Material Vanadium Permendur
Pole Gap (Min. Allowance) 6 mm
Period Length 30 mm
Effective Magnetic Field 1.296 Tesla
Effective K Value 3.63
Undulator Segment Length 3.40 m
Nr. of Undulator Segments 33
4LCLS Familiar Design Challenges
Between APS insertion devices and the LEUTL FEL,
the APS team has a lot of undulator experience
with
- High-quality undulator magnetic fields
- Magnetic tuning for phase errors and trajectory
straightness - Variable and fixed gaps
- Phasing undulator ends
- Magnetic design
- NdFeB magnets
- Vanadium permendur poles
- 30-mm period
- K3.63 so Beff1.296 T
5Magnetic Design
- Standard undulator design considerations
- Maximize the field
- Dont demagnetize the magnets
- Dont oversaturate the poles
6Magnetic Design (2)
Prevent Radiation Damage
- Chose a new grade of magnet with higher
coercivity (N39SH) for the prototype - Attention to minimizing the demagnetizing field
- Design goal to be as restrictive as usual on the
demagnetizing field, maybe even at the cost of
higher pole saturation, then use the high Hc
magnets
7New Challenges Uniformity and Stability
- Achieving a field-strength uniformity of 1.5 x
10-4 along the undulator line is a challenge - Gap change of 1.4 microns
- Vertical shift 50 microns
- Temperature coefficient of the magnet is 0.1/C
- Thermal expansion
- And there may be a desire to taper in the future
8Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Design Improvements
- Canted Pole Measurements
- Plans
- Summary
9Complete Undulator Module
Magnet Assembly
BPM
Quadrupole
Rails CAM Movers
Cradle
10Mechanical Design
11Mechanical Design Features
- Housing is made from a forged Ti bar
- Ti was preferred over other materials because
- Nonmagnetic
- Low thermal expansion
- Long-term stability
- Rigidity to density ratio for minimal deflection
- Al baseplate provides partial thermal
compensation - Open on one side for magnetic measurement access
and shimming
12Titanium Strongback
13Mechanical design features, cont.
Shims and push-pull screws adjust the
gap. Magnets are clamped from only one side.
Magnetic side shims. Steel bars approach side of
pole. Correction up to 3 in field.
14Pole clamping
Poles have titanium wings, and are clamped on
both sides
15Pole simplification now under consideration
Eliminate the wings and screw the pole in from
the bottom. Still being refined will be used in
a segment of the prototype and reviewed.
16End-phase adjusters in the prototype
- Piezo translators on end sections allowed gap
field strength adjustment - Over the last seven periods only
- Adjusted phasing between undulators
- Can relax the requirement for constant Beff
between undulators to 7x10-4 - Travel range 100 micron each jaw (200 microns in
total gap). 100 microns corresponds to 29.
17Eccentric cam movers
Each cam is driven by a separate motor Adjustable
in both transverse directions in roll, pitch,
yaw
18Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Design Improvements
- Canted Pole Measurements
- Plans
- Summary
19Assembly - Magnet Sorting
Single Magnets Matched Pairs
Magnets were sorted by strength (Total Moment),
then the strongest and the weakest were matched
together. Very important saved lots of time
since we found we could use this vendors
measurements as is for sorting not all vendors
routinely make these measurements.
20Assembly - pole sorting
After magnet sorting, the main contributor to
field errors was pole height variation. Tall and
short poles were paired, and RMS deviation in gap
was reduced from 6.3 to 2.4 microns
After sorting
But this pairing neglected the contribution of
the Al base plate thickness, and variation due to
the attachment to the Ti. Final gap variation
was 50 microns.
Note Put tighter tolerances on the Al baseplate
for production
21Magnetic Tuning
Nonetheless, the device met the trajectory
straightness requirement (2 micron) without
tuning. After tuning, the wiggle-averaged
trajectory was within a range of about 0.5
microns.
22Phase Error Tuning
The calculated spontaneous emission amplitude
needed tuning to raise it from 93 to over 99 of
ideal. (The rms phase error decreased from
11.2 to 6.5.)
23Temperature Dependence
Care must be taken in the measurements to allow
the undulator sufficient thermal equilibration
time Also need to correct for temperature
dependence of the Hall probe (DBeff/Beff)/DT
-5.5 x 10-4 /C
24Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Post-Prototype Design Improvements
- Canted Pole Measurements
- Plans
- Summary
25Post-prototype Considerations
- End phase adjustments
- Piezos long-term stability for this application
is untested - Adjustment to final gap has not yet been done,
but can do this with the cant anyway. - Assume temperature dependence is handled by the
conventional facilities specifications.
26Radiation Damage Post-prototype
- Had considered using SmCo magnets
- Better radiation resistance
- Smaller decrease in strength with temperature
rise - But overall weaker strength and more brittle
- Ruled out based on schedule no time for RD.
- Instead, take advantage of APS radiation exposure
and damage experience at the APS. - Provide dose limit guidance and information to
SLAC to be used as input into the undulator
protection system. - Do not operate LCLS under conditions likely to
result in damage to the undulators.
27Post-prototype, cont.
- A comb shunt for adjusting the field strength was
proposed - Initial tests look promising, but added design
complexity (remote capability - considerable
added design complexity) - Also a possibility for end phase correction only
28Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Post-Prototype Design Improvements
- Canted Pole Measurements
- Plans
- Summary
29Canting The Gap
- A scheme ( thanks to J. Pflueger) of canting the
poles so that field strength varies with lateral
(horizontal) position was very promising. - A test section was canted and measured with
excellent results. Canting was adopted into the
baseline.
30Canted Cross-section (exaggerated)
LCLS Undulator Cross- Section with Wedged
Shims
31 Effective Magnetic Field
- Measured slope of 6.6 Gauss/mm agrees with
calculations ( 5.7 Gauss/mm for 3 mrad cant). - Alignment accuracy needed for DB/B 1.5x10-4 2
Gauss -gt 0.3 mm
32RMS Phase Error
- No significant dependency on X
- An RMS phase error of 6.5 degree is an upper
limit for near-perfect (100) performance.
33Horizontal Trajectory (averaged over period
length) at 14.1 GeV
- Trajectory vs. X well behaved and well within the
tolerance requirement of 2 mm maximum walk-off
from a straight line. - Operational range is 1.2 mm for 1.0C
temperature compensation.
34 Fringe Fields at X65 and 100 mm
- Fringe fields with new shims are close to earth
field for X100 mm. (Earth field contribution to
trajectory shift has to be corrected.)
35Fine adjustment of effective magnetic
field(Isaacs field-tuning procedure )
- Select spacers with thickness step 15 µm to set
the effective field in the range of 30 Gauss (1
µm in gap corresponds to 2 Gauss in field). - Set spacer horizontal position to adjust the
effective field to 6 Gauss (spacers are wedged
with 3 mm/mm cant) - Set horizontal position of the undulator as a
whole so the effective field is in the range 2
Gauss (DB/B 1.5x10-4) (This step saves time
and provides better accuracy) - The undulator horizontal position could be
remotely controlled during operation to
compensate for in-tunnel temperature variations
(motion of 1.2 mm for 1C needed). Such option
is available, if quadrupoles are separated from
undulator sections.
36Magnetic needles for alignment
- Only one needle is required for alignment in the
X direction - One more needle has to be added at Y0 for
alignment in the Y direction
37Outline Prototype Undulator Status
- Design Challenges
- Mechanical Design Features
- Performance
- Post-Prototype Design Improvements
- Canted Pole Measurements
- Plans
- Summary
38Scope and Plans Undulator Systems
- 33 Precision magnetic arrays with canted poles
- 33 Support/alignment systems including
- Cradle that supports the undulator, BPM, and
quadrupole magnet. - Precision CAM movers and motors enabling
positioning, alignment, and adjustment of the
cradle. - Rail system to move the undulator, facilitating
manual retraction of an undulator out of the
beamline and precision reproducible re-insertion. - 7 Spare Undulator Modules
- 1 Undulator Transport Device for Installation
39Plan Undulators (1)
- To meet schedule and funding profiles, and to
ensure that the Undulator Systems are complete by
July 2007, we plan to procure the following
long-lead items as early as possible in FY05 - Precision-machined titanium strongbacks
- NdFeB Magnet blocks
- Vanadium Permendur Magnet poles
- The same APS undulator experts, who were relied
upon for design, construction, and assessment of
the prototype, will finalize procurement packages
for the LL items, in accordance with our Advance
Procurement Plans APP.
40Scope Quadrupole Magnet Systems
- 33 Quadrupole Magnet Systems - installed
- Permanent Magnet Quadrupole
- Support with Precision Translator settable to 5
um readout to 1um - 5 Spare Magnet Systems
- Separate steering is not included
41Summary
- A full-scale prototype undulator was constructed
and tested at APS, and met LCLS performance
goals. - A subsequent design improvement, that of
introducing a 3-mrad cant in the pole gap, was
implemented using wedged spacers between the
aluminum base plates and the titanium core. It
was successfully tested and the concept was
adopted in the baseline. - A disadvantage of the canted-pole design is the
necessity to provide a separate support for
vacuum chamber - Magnetic measurements show good agreement with
calculated change of the effective magnetic field
versus X (horizontal motion). - No significant change of the RMS phase error
versus X was measured.
42Current Status
- Significant effort has been devoted to planning,
resulting in a detailed undulator construction
schedule that is integrated with the BPM,
quadrupole and vacuum chamber construction and
testing. The undulator schedule and the magnet
measurement schedule are mostly integrated, and
are consistent with completion of undulator
systems in July 2007. - A skeleton installation schedule exists details
are being added and integration with the rest of
the schedule is ongoing. - Schedule refinement is ongoing.
- Costs were estimated by in-house experts with
relevant experience and were based on vendor
quotes and previous experience. Cost scrubbing
will continue. - The greatest schedule risks come from
- Design changes
- Delayed funding