vertex detector r&d work plan in 2004
DESCRIPTION
Vertex detector R&D Work Plan in 2004. 2004/3/11 Y. Sugimoto for KEK-Tohoku-TohokuGakuin-Niigata-ToyamaCMT Collaboration. Achievement in 2003. Study of Radiation Damage Jul/Oct: High energy electron irradiation at LNS (Tohoku) Electron energy dependence of CTI - PowerPoint PPT PresentationTRANSCRIPT
Vertex detector R&D Work Plan in 2004
2004/3/11Y. Sugimoto
forKEK-Tohoku-TohokuGakuin-Niigata-T
oyamaCMT Collaboration
Achievement in 2003
Study of Radiation Damage Jul/Oct: High energy electron irradiation at LNS (Tohoku)
Electron energy dependence of CTI Observation of Hot Pixel generation by H.E. electrons
Confirmation of effect of Fat-zero charge injection Study of charge diffusion in CCDs
Measurement of Diffusion Time in CCDs Development of cPCI ADC & DAQ System Thin CCD
Ordered 4 types of small samples
Mid-term Plan Milestone:
Construction of prototype sebsors and ladders which can achieve an impact parameter resolution of b=5 10/(psin3/2) m
To achieve the target above we need study on ; Thinning of CCD wafers to minimize the multiple scattering. The supp
ort structure for the thin wafers is also needed Radiation tolerance to put the detector as close to the IP as possible. Multiport readout of the CCD compatible with the required readout sp
eed of the vertex detector at LC experiments. It also contributes to the improvement of the radiation tolerance.
Readout ASIC for the multiport readout Preparation for the case that TESLA is selected
3-year project 1st year: Basic Study 2nd yeat: Detailed design of prototypes and make an order 3ed year: Prototypes delivery and tests
Mid-term Schedule
Original Plan Now( Hopefully)
Basic Study FY04 FY04 ~ 05 1H
Conceptual Design of Proto-type
FY04 FY05 1H
Detailed Design of Proto-type
FY05 1H FY05 2H
Order Mid FY05 FY05 End
Delivery Mid FY06 FY06 End
Test FY06 2H FY07 1H
R&D Items in 2004 Thin Wafer
Mechanical Strength Electrical Characteristics ( Dark current, Speed ) Impact on Physics : Simulation (Efficiency, Purity, Jet charge, etc) (1)
Radiation Tolerance CTI, DCP, Hot Pix : Clock (F, tw, Amplitude) dependence (2)
New driver board, Timing generator (FPGA), cPCI DAQ system Spatial Resolution vs. Radiation Damage (Using LASER) (3) Study of radiation tolerance of Back-thinned CCD
Beam irradiation test ? or 90Sr irradiation is OK? Background Simulation (Particularly 2-photon b.g. w/o Pt cut) (4)
(Readout ASIC: Conceptual design) (Multi-port CCD: Conceptual design) Preparation for the case of Cold Technology (TESLA)
Study of diffusion in CCD: back-thinned CCD (LASER in H-Reg) (3) Estimation of efficiencies when 50MHz r.o. is impossible(=High Hit density) :
Simulation (5)
Thin Wafer
Sample Chips (S7960-mod) Purpose: Find the maximum cell size to keep flatness CCD format:
24m pixel size 256(H)x1044(H)
4-types with different cell size 4 bare chips and 8 packaged chips (4 types x 2) 2 standard packaged chips
Schedule Mar. 2004: Bare chip delivery Apr.: Flatness measurement Presented at Paris (?)
Radiation Immunity
CCD Study on CCDs(256x256) irradiated in 2003 New irradiation test will be done for S7960 (256x1044) (10
chips will be delivered ) Schedule
By the end of June: Set-up new readout system cPCI based DAQ New Driver Board FPGA Timing Generator
July~: Intensive study Results by ACFA WS in Nov.
In case of Cold Technology No proven technology for VTX (except for thick HAPS) Fully Depleted CPCCD of Digital CMOS Fully Depleted CCD: >50MHz very challenging CMOS proposed by Yale group: Direct encoding of hit address
Very unique and may be promissing We have to make it clear if we can deal with “Cold” before summ
er Diffusion Study Hit density vs. Efficiency Study of CMOS
Japan-US
US Group: SLD members We can learn their know-how and experiences
Different types of thinning and proto-types between Japan and US Wider choice of the best technology Effective R&D
Evaluation and comparison of different types of technology based on the common criteria
US group uses USJ budget for prototype sensors DOE budget for others
Apply again in 2005 (unless US forsake us)
World Wide Effort Future International LC:May not be GLC
Physics & Detector should be flexible Detector Component R&D: more and more inter-regional
TPC – EU, US, Japan CALICE – Europe, US, ( Japan in future? ) SILC – EU, US, Korea, Tokyo U.
Full Simulation requires a Detector Assembly Model Too early to start design of one (or 2) detector in the world Regional study based on Detector Models continue
TESLA Detector US Large Detector US Small/Silicon Detector GLC Detector – too conservative, not usable with “Cold”
Need to re-construct New Detector Model in Asia?
Proposal for New ACFA Advanced Detector Assembly Model
GLC Detector Advanced Detector
Solenoid 3T 4T
Vertex Detector 4 layers (24~60mm)
300m thick
b=720/(psin3/2)
5 layers (15~60mm)
100m thick
b=510/(psin3/2)
Intermediate Tracker
Si Strip Si Strip
t-meas. Layer (SiFi) ?
Central Tracker Jet Chamber
Pt/Pt=1x10-4+0.1%
TPC
Pt/Pt=0.5x10-4+0.1%