7 th ACFA, H.J.Kim Intermediate Tracker H. J. Kim, KNU H. J. Kim, KNU 2004/11/09 7 th ACFA workshop...

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7 th ACFA, H.J.Kim Intermediate Tracker Intermediate Tracker H. J. Kim, KNU H. J. Kim, KNU 2004/11/09 7 2004/11/09 7 th th ACFA workshop ACFA workshop 1. 1. Introduction Introduction 2. 2. Intermediate trackers/FTD for LC Intermediate trackers/FTD for LC 3. 3. Simulation study Simulation study 4. 4. Outside Si-tracker option Outside Si-tracker option 5. 5. Silicon strip R&D for the intermed Silicon strip R&D for the intermed iate tracker iate tracker 6. 6. Summary Summary

Transcript of 7 th ACFA, H.J.Kim Intermediate Tracker H. J. Kim, KNU H. J. Kim, KNU 2004/11/09 7 th ACFA workshop...

Page 1: 7 th ACFA, H.J.Kim Intermediate Tracker H. J. Kim, KNU H. J. Kim, KNU 2004/11/09 7 th ACFA workshop 1.Introduction 2.Intermediate trackers/FTD for LC 3.Simulation.

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Intermediate TrackerIntermediate Tracker

H. J. Kim, KNUH. J. Kim, KNU

2004/11/09 72004/11/09 7thth ACFA workshop ACFA workshop

1.1. IntroductionIntroduction2.2. Intermediate trackers/FTD for LCIntermediate trackers/FTD for LC3.3. Simulation study Simulation study 4.4. Outside Si-tracker optionOutside Si-tracker option5.5. Silicon strip R&D for the intermediate tracker Silicon strip R&D for the intermediate tracker 6.6. SummarySummary

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▣ Why VTX and tracking important?Why VTX and tracking important?

• recoil mass reconstruction - importance of tracking resolution

q qbar ( b bbar -> Vertex! )

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General view ofGeneral view of Three detector option Three detector option

GLD(Huge)

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*To improve1) the linking efficiency of a main track to the corresponding VTX hits,2) the reconstruction efficiency of low-momentum tracks and of particles which decay between the VTX and the Main tracking system3) the momentum resolution of tracks.

* * If the beam background is very severe, you If the beam background is very severe, you can turn off the HV of inner layers of TPC can turn off the HV of inner layers of TPC without serious performance losswithout serious performance loss

*Trigger and/or Time stamping capability

*Standalone tracking

Purpose of Intermediate Tracker

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Silicon Tracking for SiD (Jaros’s talk)Silicon Tracking for SiD (Jaros’s talk)

Why silicon microstrips? SiD starting point Why silicon microstrips? SiD starting point Robust against beam haloRobust against beam halo showers showers

Thin, even for forward tracks.Thin, even for forward tracks. Won’t degrade ECAL Won’t degrade ECAL

Stable alignment and calibration.Stable alignment and calibration. No wandering T to D. No wandering T to D.

Excellent momentum resolution (Excellent momentum resolution (p/pp/p22~2 x 10~2 x 10-5-5))

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TESLA TESLA tracking systemtracking system

from TESLA TDR

cos()=.995

Magnetic field: 4 Tesla

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From Behnke’s talkFrom Behnke’s talk

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From Behnke’s talkFrom Behnke’s talk

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Typical “Typical “Large/Large/Huge” models under considerationHuge” models under consideration

SiVTX pixel(cold version)

HCAL(Pb(Fe)/scinti or digital)

W/Scinti ECAL

TPC(Jet chamber as option)

Si intermedi.-Trk

SC-coil

SiVTX pixel

Pb/scinti HCAL

Pb/Scinti ECAL

Jet chamber

Si intermedi.-Trk

SC-coil

“GLC” design (ACFA) “Large/Huge”

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• stand-alone tracking capability

▣ Intermediate Tracker Configuration

• 5 layers at r = 9 to 37 cm• angular coverage |cosΘ|<0.9• spatial resolution σ = 10 μm• thickness of a layer: 0.6% Xo

Huge detector concept:TPC: Rmin = 40 cm

Do not expect much changes in IT

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Intermediate Tracker DesignIntermediate Tracker Designfor GLCfor GLC - Double-sided silicon microstrip detectors- Double-sided silicon microstrip detectors i. excellent spatial resolution i. excellent spatial resolution ii. well-established technology ii. well-established technology

Layout of the IT surrounding the VTX.Layout of the IT surrounding the VTX.

- The distance between the last layer of VTX and the first layer of Trackeris - The distance between the last layer of VTX and the first layer of Trackeris about 39cm in Large detector design.about 39cm in Large detector design.

i. 5 layers of coaxial cylinders at 9, 16, 23, 30 and 37cmi. 5 layers of coaxial cylinders at 9, 16, 23, 30 and 37cmii. covers | |<0.90 coinciding with the region covered by VTXii. covers | |<0.90 coinciding with the region covered by VTXcos

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r = 10, 20, 30, 40 w/ std. design parameters

Momentum Resolution /Pt Pt .vs Pt( )

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Linking Efficiency

Linking efficiency is able to be measured by “Residual” which is defined as a precision from the difference of distance between the position of extrapolate track of main tracking & the hit position on IT or VTX layers

( )ext hitdrphi r

ext hitdz z z CDC

IT5

Figure. The definition of Residuals.

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Residuals for a single pion

Residuals vs. generation energy for a single pion

For a single pion, a linking efficiency with IT+VTX is improved by ~20 % compared to that with VTX only.

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Why Si Tracker ?Why Si Tracker ? (Sugimoto’s tal (Sugimoto’s talk)k)

• 5x105x10-5-5 does not satisfy the design does not satisfy the design criteria if the beam energy spread is criteria if the beam energy spread is 0.1%0.1%

• The performance goal should be 2x10The performance goal should be 2x10-5-5

• How? How?

Outside Outside Si Tracker for a Si Tracker for a HugeHuge Detector ???Detector ???

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The Detector ModelThe Detector Model

• Si Vertex DetectorSi Vertex Detector– 5 layers, t=705 layers, t=70m, m, =3=3mm– coscos< 1 (non-realistic)< 1 (non-realistic)

• Si Inner TrackerSi Inner Tracker– 3 layers (12, 24, 36 cm), t=3003 layers (12, 24, 36 cm), t=300m, m, =7=7mm– coscos <1 (non-realistic) <1 (non-realistic)

• TPCTPC– 40cm < R < 200cm, Z<235cm40cm < R < 200cm, Z<235cm– Ar gas, 220 samples, Ar gas, 220 samples, =150=150mm

• Si Outer TrackerSi Outer Tracker– R=205cm(barrel)/Z=250cm(EC), R=205cm(barrel)/Z=250cm(EC), =7=7mm

• Momentum resolution is calculated following Momentum resolution is calculated following Gluckstern’s methodGluckstern’s method– No sophisticated method such as Kalman filter is usedNo sophisticated method such as Kalman filter is used

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PerformancePerformance

Pt (GeV/c)

Pt/Pt2

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PerformancePerformance

cos

P/P2 (M.S. not included)

FTD?

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▣ Silicon sensor R&D Silicon sensor R&D <- Details by B.G.Cheon<- Details by B.G.Cheon

Metal 1 and metal 2 contact (VIA) Metal 1 and metal 2 contact (VIA)

n+ ohmic n+ ohmic sideside

p+ p+ junction junction

sideside

11stst metal metal

22ndnd metal readout line metal readout line

• double sided silicon strip• tree metal process- implant strips in ohmic side are orthogonal to those in junction side-readout strips in junction side have the same direction as that of ohmic side

Front Side: - brown: implanted n+ - blue: p-stop - sky blue: SiO2 - gray: Al for readout

Back Side: - blue: implanted p+ - first gray: 1st metal - sky blue: SiO2 - vertical gray: VIA - second gray: 2nd metal

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512ch 100um pitch sensor Without hour glass

512ch 100um pitch sensorWith hour glass

1cm PIN Diode

For SDD R&D

PIN Diode array

16ch 100um pitch sensor

16ch 100um pitch SSD

32ch 100um pitch sensor

64ch 100um pitch sensor

▣ MASK Design : P SideMASK Design : P Side

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▣ Silicon Sensor

n+ implantedp-stop in atoll

via in hourglassreadout pad in staggering

guard ring

p+ implanted readout strip

N side P side

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▣ Measurements

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0 20 40 60 80 100 120

1E-8

1E-7

1E-6

Leak

age

curr

ent (

A)

Reverse bias voltage(V)

LOT4_1_T1 LOT4_4_T1 LOT4_4_T3

These aredisappearedafter insulatingwafer edges

▣ Measurements of the sensor

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▣ Sensor Readout

FADC

Control Signal

DSSD

RC chip

VA-TA

FPGA

USB2DAQ

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USB2 with 25Mhz 12bit FADC for Readout USB2 with 25Mhz 12bit FADC for Readout R&DR&D

FX2 FADCCPLD

Flash RAMSRAM

31 FPGA I/O for R&D

trigger

input

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Radiation hardness beamtest with protonRadiation hardness beamtest with proton

•Radiation damage problem -> Signal reduction -> Noise increase -> Depletion voltage increase -> Sensor damage

• Radiation damage Measurement -> 30-50MeV Cyclotron proton, neutron beam irradiation (Korean cancer center hospital, Seoul, Korea) -> Leakage current measurement -> Capacitance measurement -> Signal measurement

• Processing improvement -> Radiation damage characteristics study -> Radiation hardness improvement

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IIntermediatentermediate TTracker R&D Activities in racker R&D Activities in KoreaKorea

√ linking and reconstruction efficiency (Fast Simulation) √ track momentum resolution (Full Simulation) √ DSSD simulation/design/fabrication Electronics(RC chip, VA1TA, FADC), DAQ √ S/N ratio measurement and beam test

- Kyungpook National University - Korea University - Seoul National University - Chunnam National University - Sungkyunkwan University

Sensor designProcess chart

KNU / SNU

Simulation(process and device)

KNU/SKKU

DAQ/Electronics/Test

KNU/KU/CNU

Sensor

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SummarySummary

• Intermediate Tracker is necessary to improve momentum rIntermediate Tracker is necessary to improve momentum resolution and track linking efficiencyesolution and track linking efficiency

• TPC+Si Tracker System in GLD including SOT TPC+Si Tracker System in GLD including SOT will satisfy the original design criteria even will satisfy the original design criteria even for for Eb=0.1% in wide angular range (|cosEb=0.1% in wide angular range (|cos||<0.9). <0.9).

• Double (single) side silicon strip sensor R&D is ongoing in Double (single) side silicon strip sensor R&D is ongoing in KoreaKorea

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Study issueStudy issue

• Intermediate tracker geometry optimization Intermediate tracker geometry optimization

• FTD geometry optimizationFTD geometry optimization • Double side vs Single side strip senorDouble side vs Single side strip senor

• Intermediate tracker trigger?Intermediate tracker trigger?

• Time stamping (Separation of bunches)Time stamping (Separation of bunches)

• Radiation hardness Radiation hardness

• Mechanical structureMechanical structure

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Backup slide

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▣ Cleaning Room

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512ch 50um pitch sensor

1cm PIN Diode

For SDD R&D

64ch 50um pitch sensor

32ch 50um pitch sensor

16ch 50um pitch sensor

Backside of SSD

PIN Diode array

▣ MASK Design : N MASK Design : N SideSide

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Radiation damage by n, p and Radiation damage by n, p and ee

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• Require good σrΦ and σz

• Reasonable (moderate) cost

TypeType σσrrΦΦ σσzz

MSGCMSGC

+GEM+GEM

3030μμ 3030μμmm Fast SignalFast Signal

SSDSSD 10 10 μμmm 20 20 μμmm

Straw ChamberStraw Chamber 50 50 μμmm 1mm1mm

Fiber TrackerFiber Tracker 50 50 μμmm 1mm1mm Fast SignalFast Signal

Inner DCInner DC 80 80 μμmm 1mm1mm

▣ Intermediate Tracker Option

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Pt/PtPt/Pt2 2 : Measurement Term: Measurement Term

SiDSiD GLDGLD((SiSi=7=7m)m)

GLDGLD((SiSi=10=10m)m)

TESLATESLA((SiSi=10=10m)m)

TESLATESLA((SiSi=7=7m)m)

TPCTPC 1.2x101.2x10-4-4 1.2x101.2x10-4-4 1.5x101.5x10-4-4 1.5x101.5x10-4-4

VTX+TPCVTX+TPC 4.6x104.6x10-5-5 4.6x104.6x10-5-5 5.2x105.2x10-5-5 5.2x105.2x10-5-5

VTX+SIT+TPCVTX+SIT+TPC 2.9x102.9x10-5-5 3.4x103.4x10-5-5 4.1x104.1x10-5-5 3.5x103.5x10-5-5

VTX+SIT+TPC+SVTX+SIT+TPC+SOTOT

1.9x101.9x10-5-5 2.3x102.3x10-5-5 2.6x102.6x10-5-5 2.2x102.2x10-5-5

VTX+SIT+SOTVTX+SIT+SOT 2.1x102.1x10-5-5 2.4x102.4x10-5-5 3.2x103.2x10-5-5 3.7x103.7x10-5-5 2.8x102.8x10-5-5

VTX=3m in all cases