Sven Lederer (MVS) Lutz Lilje (MVS) Torsten Wohlenberg (MVS)
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Transcript of Sven Lederer (MVS) Lutz Lilje (MVS) Torsten Wohlenberg (MVS)
Update of the vacuum system of the European X-ray free electron
laser XFEL
Sven Lederer (MVS) Lutz Lilje (MVS) Torsten Wohlenberg (MVS) DESY,
HAMBURG OLAV III July 11-14, 2011 Oak Ridge, Tennessee How to edit
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Introduction
Vacuum- & RF-requirements for the warm vacuum system Warm
vacuum section & components Gun Injector Bunch compressors
(BC1, BC2) Collimator Beam distribution Undulator chamber &
Intersection Exit-window for the main dumps Summary and Outlook
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Master View OLAV III July 11-14, 2011 Oak Ridge, Tennessee Update
of the vacuum system of the European X-ray free electron laser
Torsten WohlenbergMVS DESY, Hamburg Introduction European X-ray
free electron laser (XFEL) is a light sourceof the 4th
generation.Comparable with LCLS in California and SACLA in Japan
Spring-8 OLAV III July 11-14, 2011 Oak Ridge, Tennessee Update of
the vacuum system of the European X-ray free electron laser Torsten
WohlenbergMVS DESY, Hamburg Introduction Location of the European
XFEL:
The 3.4-km-long X-ray laser will begin on the DESY site in
Hamburg-Bahrenfeld and run mostly underground to the research site,
south of the town of Schenefeld (Schleswig-Holstein). DOP, FHH,
Landesbetrieb Geoinf. und Vermessung, LGV //DOP, (c) LVermA S-H
2007, S OLAV III July 11-14, 2011 Oak Ridge, Tennessee Update of
the vacuum system of the European X-ray free electron laser Torsten
WohlenbergMVS DESY, Hamburg Introduction Research examples:
Deciphering the structure of biomolecules: Exploring the nanoworld
in 3D: Filming chemical reactions: Observing small objects in
strong fields: Investigating extreme states of matter: OLAV III
July 11-14, 2011 Oak Ridge, Tennessee Update of the vacuum system
of the European X-ray free electron laser Torsten WohlenbergMVS
DESY, Hamburg XFEL- vacuum sections:
Introduction XFEL- vacuum sections: 5 m Undulator Warm vacuum
system at room temperature Cold vacuum system superconducting
linear accelerator inTESLA-technologie OLAV III July 11-14, 2011
Oak Ridge, Tennessee Update of the vacuum system of the European
X-ray free electron laser Torsten WohlenbergMVS DESY, Hamburg
Vacuum and RF requirements for the warm vacuum system
Goal: Avoid effects that causes of significant beam losses or beam
quality deterioration Pressure requirements beam loss from
scattering on residual gas PCO=10-7m bar (Ptot=510-7 mbar),
calculation 10 e- from each bunch negligible! Bremsstrahlung is
small, mirrors! Emittance growth negligible as well Fast ion
instability: ionized molecules interact with bunches alongtrain,
initial small offset is exponentially amplified along
bunchtrain;for XFEL bunch distance of 200 ns only ion masses beyond
M100 can be captured no thread independent of pressure OLAV III
July 11-14, 2011 Oak Ridge, Tennessee Update of the vacuum system
of the European X-ray free electron laser Torsten WohlenbergMVS
DESY, Hamburg Vacuum and RF requirements for the warm vacuum
system
Caused by the short elctron bunch length, wake fields are a
critical issue to the performance of the machine.To minimize the
deterioration of the beam quality for each vacuum section
requirements on rms surface roughfness Oxide layer Relative
permeability Maximal step at flange connections Maximal gap in
longitudinal direction RF-shielding of bellows, valves and pump
ports are specified in the High level specifications for aligment
and surface properties of vacuum components OLAV III July 11-14,
2011 Oak Ridge, Tennessee Update of the vacuum system of the
European X-ray free electron laser Torsten WohlenbergMVS DESY,
Hamburg Vacuum and RF requirements for the warm vacuum system
High Level Specifications for Alignment and Surface Properties of
Vacuum Components, Available at EDMS D OLAV III July 11-14, 2011
Oak Ridge, Tennessee Update of the vacuum system of the European
X-ray free electron laser Torsten WohlenbergMVS DESY, Hamburg Warm
vacuum section & components
Gun & Injector : RF-gun copy of the prototype RF- gun4 1.5 cell
L-band normal conducting Cu cavity. Tuning to the resonance
frequency is done by controlling the cooling water temperature of
14 separated cooling channels Average pressure in the gun section
p