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Undulator Physics Diagnostics / Commissioning Strategy Heinz-Dieter Nuhn, SLAC / SSRL August 11, 2004 Undulator Overview FEL Parameters Diagnostics and.

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Presentation on theme: "Undulator Physics Diagnostics / Commissioning Strategy Heinz-Dieter Nuhn, SLAC / SSRL August 11, 2004 Undulator Overview FEL Parameters Diagnostics and."— Presentation transcript:

1 Undulator Physics Diagnostics / Commissioning Strategy Heinz-Dieter Nuhn, SLAC / SSRL August 11, 2004 Undulator Overview FEL Parameters Diagnostics and Commissioning Strategy

2 Linac Coherent Light Source
Undulator Near Hall Far Hall

3

4 Undulator Segment Prototype

5 Workshops and Meetings
Undulator Parameter Workshop October 24, 2003, Argonne URL: Undulator Review November 14, 2003, Argonne URL: Undulator Diagnostics and Commissioning Workshop January 19-20, 2004, UCLA URL: Report: Undulator Systems Review March 3-4, 2004, Argonne URL: Undulator Physics and Engineering Meeting June 28-29, 2004, Argonne URL: Undulator Meeting July 23, 2004, Argonne URL: LCLS Diagnostics and Commissioning Workshop September 22-23, 2004, SLAC URL:

6 Undulator 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

7 Amplitudes of Undulator Parameter Changes
May 2003 August 2004 Undulator Type planar hybrid Magnet Material NdFeB Wiggle Plane horizontal Gap mm Gap Canting Angle mrad Period Length ± 0.1 mm Effective On-Axis Field T Effective Undulator Parameter K ± 0.015% ± 0.015% Module Length m Number of Modules 33 Undulator Magnet Length m Standard Break Lengths cm Total Device Length m Lattice Type FODO Integrated QF Gradient T/m Integrated QD Gradient T/m Average b Function at 1.5 Å m Average b Function at 15. Å m

8 Performance Impact of Changes (1.5 Å)
May 2003 August Change Electron Beam Energy GeV -5.0 % Emittance nm rad +5.2 % Avg. Electron Beam Radius µm % Avg. Electron Beam Divergence µrad % Peak Beam Power TW -5.0 % FEL Parameter (3D) % Power Gain Length (3D) m +3.6 % Saturation Length (w/o Breaks) m +4.9 % Saturation Length (w/ Breaks) m % Peak Saturation Power GW +2.5 %* Coherent Photons per Pulse 1.4× × %* Peak Brightness 1.5× ×1033 ** +2.5 %* Average Brightness 4.6× ×1022 ** +2.5 %* Peak Spont. Power per Pulse GW % *Increase due to 3D effects (reduction in diffraction due to beam radius increase) ** [Ph./s/mm2/mr2/.1%]

9 Undulator Specification Documents
Controlled Specification Documents support Inter-Laboratory Communications Global Requirements Document (GRD) GRD ( Physics Requirements Documents (PRDs) PRD General Undulator System Requirements ( PRD Magnetic Measurement Facility Requirements ( PRD Beam Based Alignments System Requirements ( PRD LCLS Beam Position Measurement System Requirements ( Engineering Specification Documents (ESDs) ESD Undulator Segment Specifications ESD Undulator Segment Support Specifications ESD Quadrupole Magnet Specifications ESD Diagnostics System Specifications ESD Wire Position Monitor System Specifications ESD Hydrostatic Leveling System Specification ESD Vacuum System Specifications ESD Controls Specifications Interface Control Documents (ICDs) ICD Undulator Mechanical Interfaces Process of generating these documents is on-going.

10 FEL 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 Charge Single Shot Low Charge, 10 Hz 10 Hz

11 Workshop 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

12 Undulator Radiation Protection
Two-Phase, Two-Plane Collimation, 1½ Times p/2 ~p/2 3 mm edge scattering 2.5 mm 2 mm halo e- beam undulator beam pipe x1 x2 x3 phase-1 again phase-1 phase-2 (also collimation in y and energy – see next slides)

13 E1 E2 x1 y1 x2 y2 x3 y3 LCLS Collimation Proposal (2 energy, 3 x, and 3 y adjustable collimators) muon shielding undulator x3 & y optional?

14 well shadowed in x, y, and E
2nd-order tracking with all collimators closed and big halo 2.5 mm 2-phase, 2-plane, and energy collimation in 2nd-order well shadowed in x, y, and E ? - CY3 CX3 2.0 CY2 CX2 CY1 CX1 5.0 CE2 CE1 Dy mm Dx Coll. gex,y = 4000 mm, sE/E = 10% (uniform)

15 First beam shot through undulator?
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?

16 FEL 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 Bunch Micro-Bunching

17 Dose / Power Considerations
Fluence to Melt Energy Density Reduction of a Reflector Be will melt at normal incidence at E < 3 KeV near undulator exit. Using Be as a grazing incidence reflector may gain x 10 in tolerance.

18 End-of-Undulator Commissioning Diagnostics
Measurements Total energy Pulse length Photon energy spectra Spatial coherence Spatial shape and centroid Divergence

19 4' 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

20 Measurement 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

21 Measurement of SASE Gain with end-of-undulator diagnostics
GENESIS Simulations by Z. Huang

22 Spontaneous vs. FEL Radiation -1-

23 Spontaneous vs. FEL Radiation -2-

24 Workshop 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 R&D Study of Spectral and Spatial Distribution of Spontaneous Radiation Diagnostics Prototyping Microbunching Measurement

25 Requirements for LCLS undulator are well established
Conclusions 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 LCLS Start-Up Test Plan (

26 End of Presentation


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