xfel undulator efforts at desy and thoughts on lcls-ii h.-d. nuhn june 30, 2010

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XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

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Page 1: XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

XFEL Undulator Efforts at DESY and Thoughts on LCLS-II

H.-D. NuhnJune 30, 2010

Page 2: XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

• XFEL Undulator– Undulator Magnet Development– Magnet Measurement Facility– Conceptual Design Review of Undulator Segments for Pre-Series Prototype

for SASE1-3– Production of circularly polarized radiation at SASE3

• 2 Talks– Experience with Commissioning of the LCLS Undulator System– Plans for LCLS-II

• FLASH control room• PETRA III / HERA III

2-week visit at XFEL June 7 – 18, 2010

XFEL Undulator EffortsPage 2

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• XFEL Undulators (J. Pflueger)

• XFEL Undulator Alignment Concept

• XFEL Phase Shifters

• XFEL Earth Field Compensation

• XFEL Undulator Controls (S. Karabekyan)

• Production of Circular Polarization (M.Yurkov)

Overview

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Page 6: XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

Joachim Pflueger

XFEL Energy Change 17.2 GeV to 14 GeV Requires Change in Undulator Design

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Page 20: XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

LCLS-I fixed gap undulators• MMF

– Install tuning benches in same orientation to Earth field as in the UH. Use mu-metal wrapper to suppress field differences.

• Undulator Hall– Undulators with mu-metal wrappers

and oriented tuning have sufficient Earth field compensation. No further protection needed.

The method can not easily be applied to variable gap undulators

Earth Field Compensation

XFEL Undulator EffortsPage 20

XFEL variable gap undulators• Tuning Lab

– Eliminate Earth field with 3 orthogonal Helmholtz coils mounted to the room edges.

• XFEL Tunnel– Eliminate Earth field with 3

orthogonal Helmholtz coils per segment mounted to the tunnel walls and floor.

Page 21: XFEL Undulator Efforts at DESY and Thoughts on LCLS-II H.-D. Nuhn June 30, 2010

• Vacuum chamber and RF cavity BPMs fixed to floor• Quadrupoles with (x, y) remote adjustability• Undulator segments with (y, jaw) remote adjustability

1.Align 175-m long vacuum chamber roughly to a straight line with conventional alignment methods

2.Align RF cavity BPMS to same straight line as vacuum chamber with conventional alignment methods

3.Straighten electron beam orbit using BBA by remotely adjusting quadrupole positions

4.Center undulators with beam based K measurements (find smallest K value for mid-plane position.

5.Adjust gap heights of all undulators with beam based K measurements.6.(Optional) Vertically center vacuum chamber inside undulator gap using

local adjustments.

XFEL Alignment Concept

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XFEL Phase Shifters

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NIM A 605 (2009) 399-408

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XFEL Phase Shifters

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NIM A 605 (2009) 399-408

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Presentation TitlePage 32

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Presentation TitlePage 33

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Presentation TitlePage 34

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Presentation TitlePage 35

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Presentation TitlePage 37

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Presentation TitlePage 38

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Presentation TitlePage 39

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• XFEL is planning to use one type of planar, variable gap undulator for the SASE 1, 2, and 3 lines.

• Ideas of adding helical or Apple-type undulators are being discussed but no designs or detailed plans exist, yet.

• Tuning by adjusting pole positions appears to be advantages for variable gap devices and should be considered for LCLS-II.

• Undulator Line Alignment Concept for XFEL is less flexible than for LCLS-I and depends quite heavily on K-Mono (or K-Spectrometer) measurements.

• Permanent magnet XFEL Phase Shifters are complex and do not appear to provide benefits over 4-EM dipole chicanes.

• XFEL Earth Field Compensation using 3 orthogonal Helmholtz coils might be need for LCLS-II variable gap undulators.

• XFEL Undulator Controls appear to be based on localized control system.• XFEL is working on ideas for polarization control, similar to what we are considering

for LCLS-II• Problem of removing unpolarized component is being addressed. 2nd harmonic

solution is presently preferred. Beam deflection while preserving micro-bunching is being studies.

Summary

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End of Presentation