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FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

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Page 1: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

FPCCD Vertex detector

22 Dec. 2006

Y. Sugimoto

KEK

Page 2: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Vertex detector for ILC

Performance goal :  Impact parameter resolution;

   IP = 5 10/(psin3/2) m   ( << c of D, )

This m.s. term is very challenging• Very thin wafer, beam pipe, support • Innermost layer as close to IP as possible High b.g. rate High pixel occupancy

Track density (/cm2/BX)

Page 3: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Vertex detector options If signals of one train (2820 bunches) are accumulated, too many

hits by beam b.g. for 25 m pixels, the pixel occupancy >10% for B=3T and R=20mm  

Solutions; Fast readout : Example; Column Parallel CCD @50MHz, 20 frames/train

No time to wait for diffusion in epi-layer after particle incident Fully depleted CCD No diffusion Poor resolution Still smaller pixel size is necessary to recover the resolution Possible effect by RF noise by beam

Analog registers in each pixel (~20/pixel), and readout between trains CMOS: Flexible Active Pixel Sensor (FAPS) CCD: In-situ Storage Image Sensor (ISIS) Fine and complicated structure Large area OK?

Make pixel density x20Fine Pixel CCD (FPCCD)

Page 4: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Vertex detector options

Si Pixel

Readout between

trains

Readout duringtrain

Fine pixel(x20 more

pixels)

Standard pixel(x20 time slice

in 1 train)

Standard pixel(x20 time slice

in 1 train)

FPCCD

ISIS

FAPS

MAPS

CPCCD

DEPFET

SOI

Page 5: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

GLD Vertex detector FPCCD vertex detector as the baseline design of GLD

Accumulate hit signals for one train (2840 BX) and read out between trains (200ms) Completely free from EMI

Fine pixel of ~5m (x20 more pixels than “standard” pixels) to keep low pixel occupancy Spatial resolution of ~1.5m even with digital readout

Fully depleted epitaxial layer to minimize the number of hit pixels due to charge spread by diffusion

Two layers in proximity make a doublet (super layer) to minimize the wrong-tracking probability due to multiple scattering

Three doublets (6 CCD layers) make the detector Tracking capability with single layer using hit cluster shape can hel

p background rejection Multi-port readout with moderate (~20MHz) speed (Very fast read

out (>50MHz) not necessary) Simpler structure than FAPS or ISIS Large area No heat source in the image area

Page 6: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK
Page 7: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Standard CCD Fine Pixel CCD

High Pt

Signal

Low Pt

b.g.

Z

B.G. rejection by hit cluster shape (tracking capability with single layer!)

Page 8: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Challenge of FPCCD Fully depleted Lorentz angle

tan=rHB, rH: Hall coefficient~1, : mobility (m2/Vs), B: Magnetic field (T)

Stronger E-field in dep. layer (>104V/cm = 1V/m) gives saturation of carrier velocity and smaller

Epi layer of ~15m would be OK Radiation tolerance Small pixel ( ~5 m) Fast readout speed ( ~20Mpix/

s ) Multi-port readout

H-Register in image area Low noise:

<50 e (total) < 30 e (CCD)

Low power consumption Metal layer Low drive pulse voltage Output circuit

Large area:10x65mm2( in) /20x100mm2( out)

Thinning( <50 m) Full well capacity

>104 e is OK Readout ASIC

Necessary for proto-type ladder

Page 9: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Lorentz angle

tan=rHB~B (:m2/Vs, B:T), =v/E

~0.1 m2/Vs

~0.07 m2/Vs

~0.14 m2/Vs

Page 10: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

R&D for FPCCD Study of fully depleted CCD

Charge spread Lorentz angle Radiation damage

Development of FPCCD 3 rounds expected Prototype ladder in 5 years Collaboration with Hamamatsu

Minimization of material budget Wafer thinning FEA study of support structure

Development of readout ASIC

Supported by Gakujyutu Sousei

Page 11: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

R&D Roadmap

2006 2007 2008 2009 2010

DCRDOD LOIConstruction

Study of fullyDepleted CCD

Design of small Prototype of FPCCD

FPCCD fabrication

Sample test Sample test Sample test

2nd round 3rd round (prototype ladder)

Development of readout ASIC for prototype CCD

Wafer thinning and the support structure

Other 2nd priority R&Ds

ILC Project (Detector)

DOD: Detector Outline DocumentDCR: Detector Concept ReportLOI: Letter of Intent (?)

FPCCD VTX

Page 12: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Short term plan Study of fully depleted CCD

New CCDs will be delivered mid December Epi-layer: 30m / 15m Pixel size: 24m

Study of charge spread and Lorentz angle Using green YAG LASER B-field up to 1T

Radiation tolerance Electron / neutron damage Dark current / charge transfer inefficiency

Study of support structure FEA study of Si-RVC-Si sandwich structure (RVC: Reticula

ted Vitreous Carbon)

Page 13: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Study of charge spread

Apparatus

CCD for reference(Front-illumination)

CCD for test(Back-illumination)

Page 14: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK
Page 15: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK
Page 16: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK
Page 17: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Charge spread

Front illumination Standard

Back illumination Deep2

Page 18: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Field simulation

NA=1.0, 1.5, 2.0, 2.5, 3.0, 3.5, 4.0 x1013/cm3

Page 19: FPCCD Vertex detector 22 Dec. 2006 Y. Sugimoto KEK

Summary

We have started R&D of FPCCD for GLD vertex detector

Study of fully depleted CCD is on going in FY2006, and will be continued to FY2007

The 1st test sample of FPCCD is expected to be made by Hamamatsu in FY2007

We wish to construct and test prototype ladders of FPCCD by the end of Gakujyutu-Sousei project, but the budget (for r.o. ASIC and support structure) is not enough to complete that goal