1 brookhaven science associates detectors r&d d. peter siddons a p. o’connor b a national...

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1 BROOKHAVEN SCIENCE ASSOCIATES Detectors R&D D. Peter Siddons a P. O’Connor b a National Synchrotron Light Source Dept. b Instrumentation Division

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1 BROOKHAVEN SCIENCE ASSOCIATES

Detectors R&D

D. Peter Siddonsa

P. O’Connorb

a National Synchrotron Light Source Dept.b Instrumentation Division

2 BROOKHAVEN SCIENCE ASSOCIATES

Outline

• Requirements for NSLS-II Detectors

• NSLS Detector Experience

• Emerging Technologies for Sensor/Electronics Integration

• Proposed R&D Plan

3 BROOKHAVEN SCIENCE ASSOCIATES

Goals for NSLS-II Detector Development

• A pixel detector with multiple-tau time autocorrelation electronics on each pixel• Dynamics of systems on the atomic scale.• NSLS-II’s quasi-DC brightness will make it an optimal source for this

experiment.• Megapixel detector with on-pixel correlators can provide sufficient

sampling density to access the sub-microsecond domain.• 3D technology will provide the necessary integration density.

• A pixelated detector with on-pixel MCA• Simultaneous spectroscopy/diffraction detector.• Energy and spatial resolution.• X-ray microprobes with microdiffraction and fluorescence analysis on the

same sample position with the same detector.

4 BROOKHAVEN SCIENCE ASSOCIATES

NSLS Detectors

• A series of detectors for selected SR applications has been developed over the past ~5 years

• Key technologies:• Silicon pad and strip detectors (Instrumentation)

• CMOS Application Specific ICs (Instrumentation)

• Advanced Data Acquisition hardware and software (NSLS)

• The highly parallel architectures enabled by these technologies lead to significant performance advantages

5 BROOKHAVEN SCIENCE ASSOCIATES

Rapid XRF Elemental Mapping(BNL/CSIRO collaboration)

Pipelined, parallel processor and digitizer

Si padsensor(96 elements)

Low-noise preamp(32 x 3 chan.)

10

mm

Peak detector- multiplexer

size : 3.6 x 3.2 mm²technology: 0.35µm CMOS DP4M

Comparators

Cross-point switchand arbitration logic

PD/TAC array

MUX

Serial Programmable Interface

Bias

• Hardware: 32-element detector + 2 ASICs + digitizer/processor board.

• Dynamic Analysis real-time deconvolution demonstrated at 108 events/second.

• X-ray elemental images of Fiji pyrite collected at NSLS X27A beamline.

• 800 x 500 pixels of 10um x 10um, collected in 5 hr.

• 20X faster than conventional detector.

• Increase to 400 elements + NSLS-II brightness would give additional ×104 gain.

6 BROOKHAVEN SCIENCE ASSOCIATES

Detector for Diffraction Applications

sensor640 strips125um pitch

20 ASICslow-noise preamp+ discr. + counter

Real-time growth / surface modification• Beamline X21 in-situ growth endstation

Reflectivity / truncation rods / GISAXS• Tests at Cornell• System under construction for X9 undulator/CFN

Inelastic scattering• System under construction for Argonne• Interest from SSRL

80 mm

7 BROOKHAVEN SCIENCE ASSOCIATES

Limitations of Wirebonded Interconnection

pitch

throw

excess area(can’t tile)

NSLS-II detectors will require:

• larger area (100’s cm2)

• finer pixels (< 200m)

• more processing power/pixel (MCA, correlators)

• mosaic construction

8 BROOKHAVEN SCIENCE ASSOCIATES

Monolithic Approaches for Sensor/ASIC Integration

• Common Technology• sensor in CMOS process (MAPS)• transistor in sensor process (DEPFET, XAMPS)

• Charge-Shifting• capture charge in a potential well and physically move

it to output port (CCD, CDD)

• Physical Connection• bump bonding (PbSn, In)• direct wafer-wafer bonding

9 BROOKHAVEN SCIENCE ASSOCIATES

human hair for s

cale

8m

human hair for s

cale

8m

Bump-bonding: Examples

PX detectorSwiss Light Source1M, 200m2 pixels

large modules possible but:expensive, esp. for fine-pitchmany post-fab process stepsPb fluorescencedelamination

infrared imager(Raytheon)

ATLAS Vertex tracker85M pixels2 m2 silicon

10 BROOKHAVEN SCIENCE ASSOCIATES

direct wafer-wafer bonding

• Ultimate goal is monolithic integration of

any technology

• Immediate push in industry is for reducing

wireload distribution in digital ICs

• Science applications being pursued in

optical/IR imaging, HEP tracking

• FNAL and KEK have active HEP designs

• Processes available at Lincoln Labs, JPL,

OKI Semiconductor, IBM

11 BROOKHAVEN SCIENCE ASSOCIATES

3D CMOS/Photodiode Integration

1024 x 1024 imageroxide bonded 275°C SOI processthinned to 50m8m pixel pitch106 3D vias; yield 99.999%3.8x106 0.35m CMOS FETs2nA/cm2 dark current10 frames/secV. Sunthuralingam, Lincoln Labs (ISSCC2005)

bonded 2 wafer imager stack

Pixel readout chip for ILC15m pixel pitch106 3D vias; yield 99.999%104 0.18m CMOS FETs per pixel3 transistor levels11 metal layersIn fab (10/1/2006) at Lincoln LabsR. Yarama, Fermilab (FEE 2006)

12 BROOKHAVEN SCIENCE ASSOCIATES

R&D Plan

FY 07-08• research the available 3D foundry services and the CAD tools

required to access them• acquire design capability• 1 foundry run (test vehicle)

FY 09-13• further technology experiments as needed• design of correlator and MCA chips• other detector hardware (vacuum, cooling, motion control)• design and production of DAQ hardware• control, acquisition, and user interface software

13 BROOKHAVEN SCIENCE ASSOCIATES

Milestones: FY 07-08

Milestones

FY07Identify R&D partner with 3D capability.Acquire design tools compatible with R&D partner.Research correlator designs.Research ADC designs.

FY08Design a suitable test device to verify 3D capabilityFabricate test device with R&D partner.