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MDI Vacuum Status. Ray VENESS CERN TE-VSC. Introduction. Pressure requirements for QD0 and the experimental sector Pressure profile for QD0 Vacuum layout in the MDI Post-collision line Conclusions and open questions. Pressure Requirements for QD0 and Experiment. - PowerPoint PPT Presentation
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MDI Vacuum Status
Ray VENESSCERN TE-VSC
Introduction
o Pressure requirements for QD0 and the experimental sector
o Pressure profile for QD0o Vacuum layout in the MDIo Post-collision lineo Conclusions and open questions
FP420 13 X 08 Warm beampipe - R.Veness
Pressure Requirements for QD0 and Experiment
o Requirements from beam dynamicso Recent calculations from Rumolo [1] show that coherent
instabilities are not an issue if pressures with pressures in the last 20m of the BDS upto 105 nTorr (~1.3x10-4 mbar)
o He notes however that incoherent effects and emittance growth should be studied
o Requirements from the experimentso ILC simulations [2] suggest that beam-gas background is not an
issue at 103 nTorr (~1.3x10-6 mbar)o This needs to be confirmed for the CLIC experiments
o These pressure requirements suggest that a non-baked solution could be adopted for the QD0, and possibly also the experimental sector
CLIC-MDIWG 6 XI 09 MDI beam vacuum - R.Veness[1] G.Rumolo, CLIC-MDI meeting March 2010[2] T.Maruyama, LCWA 2009 Albuquerque
Unbaked QD0 Vacuum
o Geometryo Inner diameter of 7.6 mmo Separation between pumps ~4
m
o Assumptionso The system can be pumped for
100h before beamo … or it is not exposed to air during
the push-pull operation
o Unbaked, but UHV clean system, dominated by outgassing of H20
o Outgassing rates for unbaked systems are variable – uncertainty on result
o Assume 1x10-10 mbar.l.s.cm-2
FP420 13 X 08 Warm beampipe - R.Veness
Outgassing rates of water on stainless steel [F.Dylla CAS 2006]
Unbaked Pressure Profile in QD0
o Static pressureso Average 4.8x10-7 mbar [~3.6x102
nTorr]o Peak 8.1x10-7 mbar [~6x102
nTorr]o Achievable pressure is dominated
by the small conductance of the tube and the outgassing rate
o Dynamic pressure componentso Additional gas load due to surface
bombardment by ions, electrons and photons will increase these static pressures
o Some data starting to arrive from A.Sailer, but calculations are time-consuming
o Beryllium in the experimental chamber has a high secondary electron yield and may need special coating
FP420 13 X 08 Warm beampipe - R.Veness
Static partial pressure of H20 [mbar] along the QD0 beam tube [m]
QD0
Baseline Sectorisation Scheme
o Sectorso Separate machine, QD0, Detector and post-collision for independence and safety
during shutdownso Add additional sector valve to maintain cleanliness in both QD0 and detector
o Keep QD0 and experiment either under vacuum or dry gas during push-pullo Essential to reduce pump-down time after detector push-pull in a non-baked system
o Possibly add fast shutter to protect detectors from incidents in post-collision
CLIC-MDIWG 6 XI 09 MDI beam vacuum - R.Veness
Detector
QD0
Post-Collision Vacuum line
Machine Vacuum line
Post-Collision Vacuum line
Machine Vacuum line
= Sector valve= Fast shutter valve
QD0-Experiment Layout
FP420 13 X 08 Warm beampipe - R.Veness
H.Gerwig, 8th MDI meeting
We are missing a pump here
..and a pumping port here
Is this transition acceptable?
Post Collision Line
o Absorberso Latest information from Edda
is that the baseline design is for absorber blocks outside the vacuum system
o This will mean a ‘reasonable’ gas load on the pumping system, but will require several vacuum windows
o Important to maintain contact between post-collision and vacuum system designers
FP420 13 X 08 Warm beampipe - R.Veness
Conclusions and Open Issues
o Unbaked QD0 design presentedo Average static pressure 4.8x10-7 mbar [~3.6x102 nTorr]o This will need 2 sector valves between QD0 and experiment for rapid
recovery after push-pull and pumps on both ends of QD0o Pumping on both ends of QD0 is essential, as well as a port for pumping the
space between the 2 valves
o Open issues for pressure profileso Ion, electron and photon induced desorption rates need to be calculated
o Other beam dynamics requirements?o Incoherent effects and emittance growtho Wall impedance requirement for vacuum chambers
o low resistivity coatings?
o Beampipe geometry transitions?o Trapped RF modes giving coherent/incoherent losses and heating effects
o Next stepso Confirm the acceptability of unbaked design in QD0o Calculate static pressure profile in an unbaked experimental sector
FP420 13 X 08 Warm beampipe - R.Veness