T. Yamazaki (RIKEN) Y. Akaishi (KEK), A. Dote (KEK), M. Iwasaki (RIKEN), T. Suzuki (Uni Tokyo),
Status report on the Asian Solid State Tracking R&D March 31, 2003 M. Iwasaki University of Tokyo.
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Transcript of Status report on the Asian Solid State Tracking R&D March 31, 2003 M. Iwasaki University of Tokyo.
![Page 1: Status report on the Asian Solid State Tracking R&D March 31, 2003 M. Iwasaki University of Tokyo.](https://reader036.fdocuments.net/reader036/viewer/2022062517/56649f285503460f94c412da/html5/thumbnails/1.jpg)
Status report on the Asian Solid State Tracking R&D
March 31, 2003
M. Iwasaki University of Tokyo
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1. Si -strip central tracker: Univ. of Tokyo2. Si -strip intermediate Tracker: Kyungpook National Univ., Ewha Univ., Yonsei Univ., Korea Univ. Today, I introduce these two groups activities
There are two groups working on SI tracker in Asian LC Group
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1)Si -strip central tracker R&D by Tokyo Group
Univ. of Tokyo Group: M. Iwasaki, H. Aihara
GEANT4 Full simulation study on the SI tracker 1. Basic detector parameter studies 2. Photon BG estimation
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U. Tokyo Group works on the Full detector simulation of the SI central tracker
In Linear Collider environment, Central Tracker must be robust SI tracker is one of the good candidate for LC
In our simulation, we use GEANT4 Full detector simulation + tracker hit position smearing Assuming NLC-SD detector parameters (SDMar01): 5 double-sided Si -strip layers R = 20cm - 125 cm B = 5.0 Tesla Track finding … cheater (gathering hits from the same particle) Track fitting … Using Kalman Filter (implemented by T.Abe)
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Silicon Central Tracker
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Tracker Hit Occupancy
10-3 10-2 at inner most
e+e- tt 6 Jets, s=500 GeV, noISR, no beamstrahlung
(strip pitch size * length)
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- - - #hit1 in central & #VXD hit=5- - - #hit2 in central & #VXD hit=5
- - - #hit3 in central
- - - #hit=5 in central
|cos|<0.8
Vertex Detector linking is important to reconstruct low-P tracks
Track Reconstruction Efficiency (Central tracker + VXD)
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Momentum resolutionGenerate single particle at |cos| = 0
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Photon BG from IR region (from beamstrahlung)
We use theBG data made by T. Maruyama
We input this data go through GEANT4 detector simulation
SDMar01 Tracker region:
180 photons / bunch
180*190 = ~34000 /event
Ave. Energy = 1.0 MeV
(Peak at 0.511MeV positron annihilation)
Energy distribution for BG photon from IR
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*On average,
~2000 /event make hits
in a SI tracker
*Ave. Energy of the photons
which make hits in a tracker
= 0.7 MeV
*Assuming 50m*20cm strip :
one makes 1.04 hits in average
BG photon detector simulation using GEANT4 (input ~34000 /event)
(Note: Hits which are seen between layers are from End-cap )
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Tracker Hit OccupancySignal: e+e- tt 6 Jets, s=500 GeV, noISR, no beamstrahlung
Due to the BG, occupancy increases by an order of magnitude .. But still 1% level at inner most (for 50m*20cm)
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GEANT4 Beam Delivery System simulation study at Tokyo K. Tanabe (JLC Road Map report design)
Currently we have outputs (ROOT) Using this BDS simulation, we’re going to do more detail detector BG studies
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2) Si -strip intermediate tracker R&D
H. Park (KNU), I.H. Park (Ewha U.), H.J. Kim (Yonsei U.), J.S.Kang, HC Ha (Korea U.)
1. Simulation 2. Design and Fabrication 3. Measurements 4. Applications in LC
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• Require good σrΦ and σz
• Reasonable (moderate) cost
Type σrΦ σz
MSGC 40μm 40μm Fast Signal
SSD 20 μm 40 μm
Straw Chamber 50 μm 1mm
Fiber Tracker 50 μm 1mm Fast Signal
Inner DC 80 μm 1mm
Intermediate Tracker
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• 5 layers at r=9 to 37 cm• angular coverage: |cosΘ|<0.9• spatial resolution: σ = 40μm• thickness of a layer: 0.6% radiation length
Application in LC: Intermediate Tracker
CDC, 50 wires
IT, 5 layers
VTX, 4 layers
Beam pipe
e+ e-
Support Tube
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Momentum Resolution
• Full detector simulation• 1 GeV single muon: • reconstruction including energy loss and multiple scattering
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Momentum Resolution
Effect of Spatial resolution is dominant
Multiple scattering, dominant
- as function of spatial resolution for different energies of the incident particle
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Design/Simulation/Fabrication of Si PIN diode
Clean wafer
Oxidation
Cover with photoresist
Expose through mask
Develop
Etch, Stip
N+Diffusion
P+ Implantation
Anneal
Metallization
P+ 0.6um
N+1.0um
Current
High Energy Particle
(1,1,1) 5 k N-type
N-sub
Metal
P+
Metal
P+
Oxide
100m
VfFloating
N-sub
Metal
P+
Metal
P+
Oxide
50m
VfFloating
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Design and Fabrication
• wafer (500/625/380 m)
- n-type high resistivity
- (111) orientation
- single side polished
- A pad size : 1.5 x 1.4 cm2
30um10um
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Leakage current : 70nA/1cm2 at 250V
Leakage Current Measurement
68nA
176nA
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Assembly: Ladder
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S/N Ratio Measurement
Dark box
Pb Pb
Photodiode sensor
Beta (90Sr) source
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Heavy Ion Beam with A/Z=2, E=30GeV
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Silicon Sensor vs dE/dx Correlation
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Design of Si Strip
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700um 700um
200 200 200100
20000um
200
250
SiO2 0.4um
For metal contact (n+) 0.4um
Aluminum 0.3um
50um
100um
n-type wafer 300um
Al
Design of Si Strip
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Summary
1) Si -strip central tracker Using GEANT4, full simulation studies have been done
* Several basic parameters are studied … Vertex Detector Linking is important to reconstruct low-momentum tracks under the high magnetic field
* Estimated the photon BG from IR-region … We are also working for the IR/beam-delivery system simulation using GEANT4 at Tokyo useful for the detail BG study in Si tracker
* Track-fitting.. Use Kalman filter * Track-finding.. Not yet Need to be implemented
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2) Si -strip intermediate tracker
* Korean group is accumulating knowHow of SI detector
* Korean group fabricated SI detector and test results showed that it is as good as others
* Submitted R&D proposal for SSD in LC
* Apply/extend to silicon detector (Intermediate tracker, Calorimetry) in LC
* Need study momentum resolution vs # of layers, thickness, ……