Vertex Detector Mechanics Bill Cooper Fermilab VXD.

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Presentation transcript:

Vertex Detector Mechanics Bill Cooper Fermilab VXD

Bill Cooper25 December 2008 R&D Meeting2 Introduction Vertex detector mechanical efforts have been in process for several years in the UK, continental Europe, Asia, and the United States. Prior to funding reductions at the end of 2007, Joel Goldstein and I led meetings to develop designs for a low-mass, highly-stable vertex detector support system. –The meetings included contributions from each of the three major ILC regions (Europe, Asia, the United States). –Since then, efforts have been directed towards generic designs. –Though progress has continued, it has been slower. R&D results have been presented at a variety of conferences, workshops, and reviews. The goals are a material budget not to exceed 0.1% of a radiation length per layer at normal incidence and a sensor location stability in each coordinate ~ 1 µm. Sensor operating temperature depends upon the sensor technology that will be used in the end. –Initial studies assumed -10 o C. –More recent studies have sought stability to -80 o C. –A reasonable compromise may be -40 o C.

Bill Cooper25 December 2008 R&D Meeting3 Designs with Longer LaddersDesign Varieties with Long Ladders LCFI Both approaches include interesting ladder features and assume foam is used as a structural element. Length of longest ladders ~ 240 to 250 mm KEK SiC Ladders Main bulkhead (SiC) Strain relief bulkhead Simple glue or wedge Retention of ladders Silicon – foam – silicon ladders

Bill Cooper25 December 2008 R&D Meeting4 Design with short Ladders plus Disks (SiD) Barrel length ~ 125 mm Innermost silicon at a radius of 14 mm

Bill Cooper25 December 2008 R&D Meeting5 CTE Mismatch Two general approaches offer promise of stability to low temperatures. Support from silicon-based foam structures with CTE close to that of silicon. –Good progress within LCFI –Initial studies at LBNL have been slowed by reduced funding.

Bill Cooper25 December 2008 R&D Meeting6 CTE Mismatch “All-silicon” barrel of length 125 mm –Acceptable results from FEA by LCFI and by U. Washington for 10 o C temperature change (smaller change than desired) –End rings were assumed to be CF laminate. We propose a renewed effort to measure and predict the properties of CF laminate.

Bill Cooper25 December 2008 R&D Meeting7 CTE Issues Silicon-based foams of sufficiently low density have been difficult to obtain. –They have also been difficult to machine without fracture. CF laminates have shown more thermal distortion than we would like. Even with perfectly matched CTE’s within a barrel, support is likely to be necessary from a more robust external structure with a different CTE. –Properly oriented leaf springs or equivalent should help. VTX Barrel Outer Support Structure

Bill Cooper25 December 2008 R&D Meeting8 Cabling, Power Distribution, Vibration All of these are serious issues. Cabling contributes significantly to the material budget. –Part of that arises from the power requirements of sensors and the need to limit IR losses in cables. –Either DC-DC conversion or serial powering are likely to be necessary to obtain an acceptable conductor thickness. Hence the interest in power distribution. Pulsed power in ILC designs, coupled with forces and moments from the solenoidal field, may lead to vibration. –To address that, power cables with three conductor layers (return – supply – return or equivalent) have been suggested. SiD

Bill Cooper25 December 2008 R&D Meeting9 In Conclusion We understand a variety of mechanical R&D topics that should be pursued. Areas of interest include: –CTE matching and accommodation –Cabling and power distribution –Minimization of material –Prototyping and tooling to demonstrate precise fabrication –Heat removal –Hermeticity and acceptance –Integration with outer tracker and forward detectors –Beam pipe design and support Thank you!