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Project Update: A Possible New RF FOIL for the VELO UPGRADE
Ray Mountain, Sheldon Stone
Syracuse University
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 2-
RF FOIL (1) -- R&D PLANPhase I Objective: Produce a quarter-length RF Foil prototype, incorporating all difficult design features needed.
– Collaboration with CMA, Inc. (compositemirrors.com)
– Develop a new high performance material, likely a multi-function nanocomposite material. A candidate formulation has been identified (X0 ≈ ½ AlMg3)
– Develop processing procedures for the materials and structure shape
– Optimize material and process parameters by series of coupon samples
– Fabricate the ¼-length prototype, incorporating the foil surface, sides, and flange in one integrated piece (no sealing)
– Test and evaluate performance characteristics, including metrology, thickness uniformity, vacuum permeability, etc.
– Build “accelerator simulator” as RF shielding test chamber (at SU)
Evaluation Phase: Evaluate viability of prototype material and structure. Perform radiation damage testing, involve CERN LHC experts for determination of its operation in primary vacuum, etc.
Phase II Objective: Design and fabricate real RF Foil for LHCb upgrade.
Plan to begin Phase I in December, but awaiting funding decision (expected soon)...
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 3-
(extras)
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 4-
RF FOIL & RF BOXcross section
~1mm
INSIDE VIEW OF RF-BOX MOUNTED IN VACUUM VESSEL
• Separates modules from beam vacuum • Foil is 300 um AlMg3, coated with
insulator and getter• Foil shape set by overlapping sensors
and beam clearance and beam effects• Large area: 200 x 1000 mm2
• Maximum allowed pressure differential: 5 mbar (=> 10 kg = 22 lb)
• Shields against beam-induced EMI• Wakefield suppressors to adapt beam
pipe geometry• Was a huge engineering effort
(NIKHEF)
CURRENTDESIGN
FOIL
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 5-
RF FOIL REQUIREMENTSPhysics:
– Must not allow excessive multiple scattering• should have the smallest radiation length possible (e.g.,
low Z) in acceptance• should minimize total material before first measured
point [MFL,PC]
– Must allow detectors to overlap, for reasons of tracking (i.e., no acceptance gaps) and alignment
• will have complicated corrugated shape– Must get as close as possible transversely to IP
• must allow approach to be < ~7.mm (original design goal was 5.mm, accelerator limit in 2001)
– Must stand high radiation environment without degradation in mechanical or electrical properties
• must withstand ~500 Mrad dose [MA,PC]
Mechanical:– Separate primary vacuum <1e-9 mbar (accelerator) from
secondary vacuum ~1e-4 mbar (detector), and maintain this ultra-high vacuum level
• must have no pinholes or virtual leaks• outgassing must be minimal
– Must mechanically hold differential vacuum of ~5.mbar (transient) to ~1e-4 mbar (steady) without rupturing or even deflecting so as to touch sensors (1 mm clearance)
• must be strong (to this level of load)• must be stiff • must have low fatigue, for repeated pumpings• must hold mechanical stability and accuracy (tolerances)
Electrical:– Must shield against RF EMI pick-up effects from accelerator
(noise in detectors)• must provide enough RF skin depth thickness (T<10-3)• must be made at least partly of good conductor• must reduce any surface/skin effects (?) [MFL]
– Must not electrically short sensors if contact is made• must have inner insulating surface or coating
Thermal:– Must handle heating effects (electronics, beam wakefield) and
cooling effects (modules, bb radiation) and not thermally deform so as to damage sensors
• must have sufficiently low CTE from about +40ºC down to -30ºC (? plus beam heating)
• wakefield power dissipation can be large (~kW)– Perhaps like it to help with cooling the electronics [pref not req’d]
• low emissivity surface (or coating), or actual cooling of foil (active/passive) [SB]
• would need then to bleed off heat away from sensors
Beam (Electrodynamic):– Must suppress wakefield impact on beams
• need smooth geometry to reduce effects [MFL]
• need continuous electrical contact from one end to the other [MFL]
• should have a small beam aperture [PC]
– Must be “dynamic”-vacuum-compatible (i.e., effects due to presence of beam, which means ion-induced desorption, synchrotron radiation, electron multipacting) [MFL]
• so need NEG coating on UHV side, which as low (ion-, photon-, electron-) desorption coefficient
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 6-
Composite Mirror Applications Inc.Initial conversations very promising
– They are interested in this projectCMA has experience producing:
– Many space-based mirrors and structures for NASA
– Spherical mirrors for LHCb RICH-1 – Prototype mirrors for BTEV RICH
Manufacture technique– Compression molding replication
• Make forms (positive + negative)• Lay up sheets of CF “cloth” and “uni” with
resin• Apply elevated pressure and temperature to
forms, resin flows, squeezes layup to required thickness
– Can replicate features down to 3 mm (or maybe smaller), as long as they are on the forming mandrel
– Can make many types of structures, can make exact duplicates of structures as well
– Have good control of thickness variations– Have solved adhesion problem in vacuum
(delamination, so-called)• 18 years experience in high strength
Aluminum adhesion to polymers• Used in many space (vacuum) applications
Good corporate partner for R&D
R. Mountain, Syracuse University VELO Update, 5 Nov\2009 - 7-
FIRST ORDER DESIGN (1)Keep same design as current foil
– same geometric form of foil and box
– as a basis for discussions, for now
Replace AlMg3 by CFRP composite– plus Al deposition and NEG on
accelerator side
– plus insulator deposition on VELO side (n.b. CF is conductive)
Produce foil + box + flange as a single integrated unit
– Avoids welding foil to box, and other sealing problems
– No seams, better for vacuum tightness
Investigate the critical issues using this first-order design …
FOIL
BOX
FLANGE
“straw man”