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First Test Measurements of a 64k pixel First Test Measurements of a 64k pixel readout chip working in single photon readout chip working in single photon

counting modecounting mode

X. Llopart

CERN, 1211 Geneva 23, Switzerland

On behalf of the Medipix2 Collaboration*

* See: http://medipix.web.cern.ch/MEDIPIX/

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OutlineOutline

u Introductionu Motivation for the chip designu The Medipix2 pixel cellu The Medipix2 chip architectureu Electrical measurementsu Conclusionsu Future work

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Medipix1 image of a sardineMedipix1 image of a sardine

X-ray tubeMo target 30 µm Mo filter25 kV5 mAs50 cm from sourceRaw data

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MotivationsMotivations

u Medipix I proved potential for photon counting pixel detectors.

u Deep sub-micron CMOS (0.25µm) is available and well characterized.

u 170 µm to 55 µm pixel side and 64x64 to 256x256 pixels per chip. Pixel dimensions competitive with film-screen systems.

u More functionality can be added to a smaller pixel.

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Characteristics of Medipix2 ChipCharacteristics of Medipix2 Chip

u Square pixel size of 55 µm u Sensitive to positive or negative input charge (different

detector materials can be used)u Pixel by pixel detector leakage current compensation u Window in energy as precise as possibleu 13-bit counter per pixel u Count rates of 1 MHz/pixel (0.33 GHz/mm2)u 256 x 256 pixels u 3-side buttableu serial or parallel I/O

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Medipix2 Pixel CellMedipix2 Pixel Cell

Preamp

DiscL

Double Disc logic

Vth Low

Vth High

13-bits

Shift Register

Input

Ctest

Testbit

Test Input

Maskbit

3 bits Threshold Adjust

3 bits Threshold Adjust

Shutter

Mux

Mux

ClockOut

Previous Pixel

Next Pixel

Conf

8 bits configuration

Polarity

Analog Digital

DiscH

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Medipix2 Pixel Cell LayoutMedipix2 Pixel Cell Layout

55 µm

55 µm

55 µm

55 µm

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Medipix2 Chip Architecture (I)Medipix2 Chip Architecture (I)14111 µm

IO

Logic

LVDS

Input

LVDS

Output32-bit CMOS Output

256-bit Fast Shift Register

3328

-bit

Pix

el C

olum

n-0

13 8-bit DACs

14111 µm

3328

-bit

Pix

el C

olum

n-1

3328

-bit

Pix

el C

olum

n-1

1612

0 µ

m

IO

Logic

LVDS

Input

LVDS

Output32-bit CMOS Output

256-bit Fast Shift Register

3328

-bit

Pix

el C

olum

n-0

13 8-bit DACs

14111 µm

3328

-bit

Pix

el C

olum

n-1

3328

-bit

Pix

el C

olum

n-1

1612

0 µ

m

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Medipix2 Chip Architecture (II)Medipix2 Chip Architecture (II)14111 µm

14111 µm

1612

0 µ

m

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Measurement SetupMeasurement Setup

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Preamplifier and discriminator measurementPreamplifier and discriminator measurement

u Measurements have been done using the Test output Pads and applying a voltage test pulse to the on-pixel injection capacitance.

Preamp Out (e-)Qin=9.28 Ke-

Y=20mVX=500ns

Preamp Out (h+)Qin=9.28 Ke-

Y=20mVX=500ns

Disc OutTHL=7Ke-

Y=2VX=500ns

Disc OutTHL=7Ke-

Y=2VX=500ns

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Measurements and CalibrationMeasurements and Calibrationu All the reported measurements are done using the electronic

calibration (Injection capacitor + external voltage pulse). u The 8fF injection capacitor nominal value has a tolerance of 10%.u The dedicated Muros2 readout system had been used

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THH

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Threshold LinearityThreshold Linearity

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easu

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THLLinear (THL)

Using internal THL 8-bit DAC

Using external 12-bit DAC

Maximum injection charge is 57.5 Ke-

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Threshold Equalization (I)Threshold Equalization (I)

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Unadjusted Thresholds ~ 500 e- rms

Adjusted Thresholds~ 110 e- rms

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Threshold Equalization (II)Threshold Equalization (II)

1 row of Unadjusted pixels 1 row of Adjusted pixels

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x30

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Threshold Equalization (III)Threshold Equalization (III)•THL=120•THL=100•Matrix unmasked•30x30 pixels active

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Threshold Equalization (IV)Threshold Equalization (IV)•THL=120•THL=110•Matrix unmasked•30x30 pixels active

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Threshold Equalization (V)Threshold Equalization (V)•THL=140 (2.8 Ke-)•Injection of 1000 pulses of 3.6 Ke-

•Matrix unmasked•30x30 pixels active

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Summary of the Electrical MeasurementsSummary of the Electrical Measurements

σnTHL~ 110 e- σnTHH~ 110 e-Adjusted Threshold dispersion

~8 µW/channel for a 2.2 V supplyAnalog power dissipation

σnTHL~ 500 e- σnTHH~ 500 e-Threshold dispersion

σnL~ 105 e- σnH~ 105 e-Electronic Noise

<1µs for Qin <50 ke-Return to baseline

<200 nsPeaking time

<3% to 80 ke-<3% to 100 ke-Non linearity

13.25 mV/ke-12.5 mV/ke-Gain

Holes Collection

Electron Collection

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Periphery MeasurementsPeriphery Measurements

u The 13 DACs perform as simulationsu Fast shift register works at > 100 Mhz*u Peripheral logic works to > 100 Mhz*u Serial/parallel I/O worku LVDS drivers and receivers work to > 100 MHz*

* IC-Tester maximum clock frequency

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Radiation Tolerance MeasurementsRadiation Tolerance Measurements

u 10 keV X-ray source

u Chip under bias conditions

u Applied dose rates:u 3.9 krad/min up to 150 krad

u 8.04 krad/min from 150 krad to 500 krad

u Analog power supply current increase from 200mA to 260 mA

u Digital power supply current increase sharply @ 200 krad reaching 1100 mA @ 500 krad

u After 1 week of annealing at 100°C the power supplies current recovered to pre-irradiation values

u Chip showed normal behavior untill 200 krad and still functioning after annealing at 500 krad

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ConclusionsConclusions

u A prototype chip consisting of 256x256 pixels has been produced with a square pixel size of 55 µm. Each pixel has around 500 transistors.

u Using the dedicated Medipix2 readout system (Muros2 and Medisoft4) complete electronic measurements and threshold calibration have been done.

u Adjusted threshold variation ~110 e- rms for both levels of discrimination.

u Electronic Noise ~105 e- rms.

u Difficulties to lower the threshold under 2.5 Ke- with the present setup.

u The chip is radiation tolerant until at least 200 Krad.

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OnOn--going workgoing worku A new chipboard card is ready to be tested with

improved decoupling and power distribution.

u Probe tested wafers have been sent for bump bonding to silicon detectors.

u This should allow an absolute calibration with radioactive sources.

u Other materials will be tried later ( CdTe, GaAs, etc…)

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Future ProspectsFuture Prospects

u With pixel shrinking charge sharing starts to dominate the detector behavior.

u Hexagonal pixels (on the detector side) become attractive.

u New front-end electronics architectures are needed.

u Some ideas are presented in a recently accepted paper for publication in the NSS/MIC IEEE journal.

u A whole spectrum of new possibilities opens with e.g. time-resolved measurements, very high dynamic range applications, colour X-ray imaging…