Many physics channels require excellent heavy flavour ID
Higgs, SUSY, Top....
4 Heavy Flavour Identification Heavy flavour particles with lifetime 1 ps (?, b and c) travel a few mm then decay. Precision silicon detectors can reconstruct decay vertices. 5 Baseline Vertex Detector
800 Mchannels of 20?20 ?m pixels in 5 layers
Optimisation
Inner radius (1.5 cm?)
Readout time (50 ?s?)
Layer thickness (0.1 X0?)
6 Simulation and Physics
Optimise detector design
Need reliable tracking
Been using Fortran/SGV
Develop vertex tools
Work within common framework
Writing C package
Physics analysis
7 ZVTOP
Topological vertex finder
Developed at SLD
Being ported to C (JAVA at SLAC)
Used as basis for flavour tag
8 Vertex Charge
Do more than identify b, c quarks
Find vertices with ZVTOP
Attach candidate tracks
Measure charge
Can tell quark from antiquark!
e.g. LED scenarios 9 Vertex Charge in Physics
Luminosity factor for two jets
Quantify effect of beam pipe radius
Neutral B Leakage Rates
10 LCFI Mechanical Studies
Thin Ladder Mechanics
Materials and designs for ?T 100K
Preference for uniform material in tracking volume
CCDs routinely thinned to epitaxial layer
Global Design
Ensure ladder designs practical
Cooling
Gas cooling has always been assumed
11 Mechanical Options
Target of 0.1 X0 per layer
(100?m silicon equivalent)
Unsupported Silicon
Longitudinal tensioning provides stiffness
No lateral stability
Not believed to be promising
Thin Substrates
Detector thinned to epitaxial layer (20?m)
Silicon glued to low mass substrate for lateral stability
Longitudinal stiffness still from tension
Beryllium has best specific stiffness
Rigid Structures
12 Mechanical Studies of Be-Si
Physical Prototyping
FEA Simulations
160 µm ripples at -60C
Good qualitative agreement
Minimum thickness 0.15 X0
13 Carbon Fibre Substrates
Carbon fibre has better CTE match than beryllium
Prototype 0.09 X0
No rippling down to lt 200K
Lateral stability insufficient
Other thin substrates under consideration
14 Rigid Structures Foam substrate or sandwich core
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