Title: Undulator Physics Diagnostics Commissioning Strategy HeinzDieter Nuhn, SLAC SSRL August 11, 2004
1Undulator PhysicsDiagnostics / Commissioning
StrategyHeinz-Dieter Nuhn, SLAC / SSRLAugust
11, 2004
- Undulator Overview
- FEL Parameters
- Diagnostics and Commissioning Strategy
2Linac Coherent Light Source
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4Undulator Segment Prototype
5Workshops and Meetings
- Undulator Parameter Workshop
- October 24, 2003, Argonne
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2003-10-24_parameter_workshop/ - Undulator Review
- November 14, 2003, Argonne
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2003-11-14_review/ - Undulator Diagnostics and Commissioning Workshop
- January 19-20, 2004, UCLA
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2004-01-19_diagnostics_comissioning/ - Report http//www-ssrl.slac.stanford.edu/lcls/wor
kshops/2004-09-22_diag_comm/lcls-tn-04-2.pdf - Undulator Systems Review
- March 3-4, 2004, Argonne
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2004-03-03_review/ - Undulator Physics and Engineering Meeting
- June 28-29, 2004, Argonne
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2004-06-28_phy_eng/ - Undulator Meeting
- July 23, 2004, Argonne
- URL http//www-ssrl.slac.stanford.edu/lcls/undula
tor/meetings/2004-07-23_und_mtg/
6Undulator Design Changes Since May 2003
- Canting of Undulator Poles
- Remote Undulator Roll-Away and K Adjustment
Function - Increase in Undulator Gap
- Reduction in Maximum Beam Energy
- Reduction in Quadrupole Gradient
- Increase in Beta Function
- Increase in Break Section Length
7Amplitudes of Undulator Parameter Changes
- May 2003 August 2004
- Undulator Type planar hybrid
- Magnet Material NdFeB
- Wiggle Plane horizontal
- Gap 6.0 6.8 mm
- Gap Canting Angle 0.0 4.5 mrad
- Period Length 30.0 0.1 mm
- Effective On-Axis Field 1.325 1.249 T
- Effective Undulator Parameter K 3.630 0.015
3.500 0.015 - Module Length 3.40 m
- Number of Modules 33
- Undulator Magnet Length 112.2 m
- Standard Break Lengths 18.7 - 18.7 - 42.1 48.2 -
48.2 - 94.9 cm - Total Device Length 121.0 131.9 m
- Lattice Type FODO
8Performance Impact of Changes (1.5 Å)
- May 2003 August 2004 Change
- Electron Beam Energy 14.35 13.64 GeV -5.0
- Emittance 0.043 0.045 nm rad 5.2
- Avg. Electron Beam Radius 27 35 µm 27.5
- Avg. Electron Beam Divergence 1.6 1.3 µrad -17.5
- Peak Beam Power 49 46 TW -5.0
- FEL Parameter (3D) 0.00033 0.00032 -3.5
- Power Gain Length (3D) 4.2 4.3 m 3.6
- Saturation Length (w/o Breaks) 82 86 m 4.9
- Saturation Length (w/ Breaks) 89 101 m 13.5
- Peak Saturation Power 7.4 7.6 GW 2.5
- Coherent Photons per Pulse 1.41012 1.51012 2.5
- Peak Brightness 1.51033 1.51033 2.5
- Average Brightness 4.61022 4.71022 2.5
- Peak Spont. Power per Pulse 91 73 GW -19.7
- Increase due to 3D effects (reduction in
diffraction due to beam radius increase) - Ph./s/mm2/mr2/.1
9Undulator Specification Documents
- Controlled Specification Documents support
Inter-Laboratory Communications - Global Requirements Document (GRD)
- GRD 1.1-001 (http//www-ssrl.slac.stanford.edu/lcl
s/prd/1.1-001-r1.pdf) - Physics Requirements Documents (PRDs)
- PRD 1.4-001 General Undulator System Requirements
(http//www-ssrl.slac.stanford.edu/lcls/prd/1.4-00
1-r0.pdf) - PRD 1.4-002 Magnetic Measurement Facility
Requirements (http//www-ssrl.slac.stanford.edu/lc
ls/prd/1.4-002-r0.pdf) - PRD 1.4-003 Beam Based Alignments System
Requirements (http//www-ssrl.slac.stanford.edu/lc
ls/prd/1.4-003-r0.pdf) - PRD 1.1-314 LCLS Beam Position Measurement System
Requirements (http//www-ssrl.slac.stanford.edu/lc
ls/prd/1.1-314-r0.pdf) - Engineering Specification Documents (ESDs)
- ESD 1.4-100 Undulator Segment Specifications
- ESD 1.4-101 Undulator Segment Support
Specifications - ESD 1.4-102 Quadrupole Magnet Specifications
- ESD 1.4-103 Diagnostics System Specifications
- ESD 1.4-104 Wire Position Monitor System
Specifications - ESD 1.4-105 Hydrostatic Leveling System
Specification - ESD 1.4-106 Vacuum System Specifications
- ESD 1.4-106 Controls Specifications
- Interface Control Documents (ICDs)
- ICD 1.4-500 Undulator Mechanical Interfaces
10FEL Commissioning Workshop 1/19-20/04
- Scope
- Commissioning of the FEL Undulator with Beam
- Goals
- End-Of-Construction Goal
- Defined by DOE to close-off construction project
(CD-4) - One of the first Commissioning Milestones
- Commissioning Goal
- Get LCLS ready for operation
- Prerequisites
- Undulator, Diagnostics, Shielding, Beam Dump etc.
in Place - Commissioning Without Beam for all Components
Complete - Main Commissioning Tasks
- Characterization of Electron Beam Up-Stream of
Undulator - Establishment of a Good Beam Trajectory Through
Undulator to Beam-Dump - Characterization of Spontaneous Radiation
- Establishment of SASE Gain
- Characterization of FEL Radiation
Low ChargeSingle Shot
Low Charge, 10 Hz
10 Hz
11Workshop Issues
- Undulator Radiation Protection
- Measurements of FEL Radiation vs. Z
- Radiation Power Damage to Inter Undulator X-Ray
Diagnostics - End-of-Undulator Diagnostics
- Beam Based Detection of Gain Reducing Errors
- Using Spontaneous Radiation
- Using FEL Gain Curve
- Numerical Simulation Support for Detector
Development and Commissioning
12Undulator Radiation Protection
Two-Phase, Two-Plane Collimation, 1½ Times
p/2
p/2
?3 mm
?2.5 mm
edge scattering
?2 mm
halo
e- beam
undulator beam pipe
x1
x2
x3
phase-1 again
phase-2
phase-1
(also collimation in y and energy see next
slides)
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15- Track 100 times with
- DL2 BPM rms res. 10 mm
- DL2 BPM rms misa. 200 mm
- DL2 Quad rms misa. 200 mm
- Undulator Quad rms misa. 100 mm
- Correct und-launch, then open stopper-2 for one
beam shot - Just 11 of 100 trajectories exceed ?2.5 mm within
undulator - None exceed ?3.5 mm
G 110 T/m
First beam shot through undulator?
16FEL Gain Measurement
- Desirable measurements as function of position
along undulator - Intensity (LG, Saturation)
- Spectral Distribution
- Bunching
Saturation
Exponential Gain Regime
Undulator Regime
1 of X-Ray Pulse
Electron BunchMicro-Bunching
17Dose / Power Considerations
Fluence to Melt
Energy Density Reduction of a Reflector
Be will melt at normal incidence at E lt 3 KeV
near undulator exit. Using Be as a grazing
incidence reflector may gain x 10 in tolerance.
18End-of-Undulator Commissioning Diagnostics
- Measurements
- Total energy
- Pulse length
- Photon energy spectra
- Spatial coherence
- Spatial shape and centroid
- Divergence
194' Muon shield
PPS
Access Shaft
PPS
Spectrometer, Total Energy
Solid Attenuator
Access Shaft
Direct Imager Indirect Imager
Slit A
Slit B
Windowless Ion Chamber
PPS
Gas Attenuator
13' Muon shield
Fast close valve
20Measurement of SASE Gain along the undulator
- Direct Detectors in the Breaks between Undulator
Segments. - No good solution for x-ray detector in existence,
yet. - Alternative End-Of-Undulator Diagnostics
- Turn-Off Gain at Selectable Point Along Undulator
by - Introduction of orbit distortion
- Removal of undulator segments (New roll-away
option) - Characterize x-ray beam at single station down
stream of undulator
21Measurement of SASE Gain withend-of-undulator
diagnostics
- GENESIS Simulations by Z. Huang
22Spontaneous vs. FEL Radiation -1-
23Spontaneous vs. FEL Radiation -2-
24Workshop Recommendations
- No Intra-Undulator-Segment X-Ray Diagnostics in
Baseline Design - Instead End-of-Undulator X-Ray Diagnostics to
Characterize FEL Radiation vs. z - Trajectory Distortion Method
- Roll-Away Undulator Segments Function
- Investigation of Spontaneous Radiation as
Diagnostics Tools - Code Development to Support Commissioning
- Areas for Follow-Up RD
- Study of Spectral and Spatial Distribution of
Spontaneous Radiation - Diagnostics Prototyping
- Microbunching Measurement
25Conclusions
- Requirements for LCLS undulator are well
established - LCLS undulator performance requirements are well
understood - Risks have been assessed and undulator
specifications address the risk - Detailed commissioning strategy is being
developed. Startup Test Plan exists. - PRD 1.1-002 LCLS Start-Up Test Plan
(http//www-ssrl.slac.stanford.edu/lcls/prd/1.4100
2-r1.pdf)
26End of Presentation