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Imaging Properties of the Medipix2 System exploiting Single and Dual Energy Thresholds L. Tlustos 1,...

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Imaging Properties of the Medipix2 Imaging Properties of the Medipix2 System exploiting Single and Dual System exploiting Single and Dual Energy Thresholds Energy Thresholds L. Tlustos L. Tlustos 1 1 , R. Ballabriga , R. Ballabriga 1 , , M. Campbell M. Campbell 1 , , E. Heijne E. Heijne 1 , k Kincade , k Kincade 2 , X. Llopart , X. Llopart 1 , P. , P. Stejskal Stejskal 3 1 1 Ph Department, CERN, Geneva, Switzerland Ph Department, CERN, Geneva, Switzerland 2 University of Canterbury, Christchurch, University of Canterbury, Christchurch, New Zealand New Zealand 3 Institute of Experimental and Applied Institute of Experimental and Applied Physics, Technical University of Prague, Physics, Technical University of Prague, Czech Republic. Czech Republic.
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Imaging Properties of the Medipix2 System Imaging Properties of the Medipix2 System exploiting Single and Dual Energy exploiting Single and Dual Energy

ThresholdsThresholds

L. TlustosL. Tlustos11, R. Ballabriga, R. Ballabriga11, , M. CampbellM. Campbell11, E. Heijne, E. Heijne11, k , k KincadeKincade22, X. Llopart, X. Llopart11, P. Stejskal, P. Stejskal33

1 1 Ph Department, CERN, Geneva, SwitzerlandPh Department, CERN, Geneva, Switzerland22 University of Canterbury, Christchurch, New Zealand University of Canterbury, Christchurch, New Zealand33 Institute of Experimental and Applied Physics, Institute of Experimental and Applied Physics, Technical University of Prague, Czech Republic. Technical University of Prague, Czech Republic.

27 September 2004 Michael Campbell

The Medipix2 ConsortiumThe Medipix2 Consortium Institut de Fisca d'Altes Energies, Barcelona, Spain Institut de Fisca d'Altes Energies, Barcelona, Spain University of Cagliari and INFN Section thereof, ItalyUniversity of Cagliari and INFN Section thereof, Italy CEA, Paris, FranceCEA, Paris, France CERN, Geneva, Switzerland, CERN, Geneva, Switzerland, Universitat Freiburg, Freiburg, Germany, Universitat Freiburg, Freiburg, Germany, University of Glasgow, ScotlandUniversity of Glasgow, Scotland Universita' di Napoli and INFN Section thereof, ItalyUniversita' di Napoli and INFN Section thereof, Italy NIKHEF, Amsterdam, The NetherlandsNIKHEF, Amsterdam, The Netherlands University of Pisa and INFN Section thereof, ItalyUniversity of Pisa and INFN Section thereof, Italy University of Auvergne, Clermont Ferrand, France, University of Auvergne, Clermont Ferrand, France, Laboratory of Molecular Biology, Cambridge EnglandLaboratory of Molecular Biology, Cambridge England Mitthogskolan, Sundsvall, Sweden, Mitthogskolan, Sundsvall, Sweden, Czech Technical University, Prague, Czech RepublicCzech Technical University, Prague, Czech Republic ESRF, Grenoble, FranceESRF, Grenoble, France Academy of Sciences of the Czech Republic, PragueAcademy of Sciences of the Czech Republic, Prague Universität Erlangen-Nurnberg, Erlangen, GermanyUniversität Erlangen-Nurnberg, Erlangen, Germany University of California, Berkeley, USAUniversity of California, Berkeley, USA

27 September 2004 Michael Campbell

OutlineOutline

Motivation and a brief overview of the Motivation and a brief overview of the Medipix2 systemMedipix2 system

MTF, NPS and DQE for a single photon MTF, NPS and DQE for a single photon counting system as a function of lower counting system as a function of lower threshold threshold

Imaging of an object using the energy Imaging of an object using the energy window window

Concluding remarksConcluding remarks

27 September 2004 Michael Campbell

Introduction and MotivationIntroduction and Motivation

Single photon counting provides clean images Single photon counting provides clean images across a wide range of incoming photon fluxes across a wide range of incoming photon fluxes

Flexible – many applicationsFlexible – many applications

Energy selective x-ray imaging possibleEnergy selective x-ray imaging possible

MTF, NPS and DQE as a function of threshold - MTF, NPS and DQE as a function of threshold - Medipix2 readout chip and a 300 Medipix2 readout chip and a 300 m thick Si sensor m thick Si sensor

First energy selective images of an object using a First energy selective images of an object using a polychromatic sourcepolychromatic source

27 September 2004 Michael Campbell

Hybrid Pixel Detector Hybrid Pixel Detector

Detector and electronics readout are optimized separately

27 September 2004 Michael Campbell

Hybrid Pixel Detector - Cross SectionHybrid Pixel Detector - Cross Section

27 September 2004 Michael Campbell

Charge sensitive preamplifier with individual leakage current compensation2 discriminators with globally adjustable threshold3-bit local fine tuning of the threshold per discriminator1 test and1 mask bitExternal shutter activates the counter13-bit pseudo-random counter1 Overflow bit

Medipix2 Cell SchematicMedipix2 Cell Schematic

Preamp

Disc1

Disc2

Double Disc logic

Vth Low

Vth High

13 bits

Shift Register

Input

Ctest

Testbit

Test Input

Maskbit

Maskbit

3 bits threshold

3 bits threshold

Shutter

Mux

Mux

ClockOut

Previous Pixel

Next Pixel

Conf

8 bits configuration

Polarity

Analog Digital

Preamp

Disc1

Disc2

Double Disc logic

Vth Low

Vth High

13 bits

Shift Register

Input

Ctest

Testbit

Test Input

Maskbit

Maskbit

3 bits threshold

3 bits threshold

Shutter

Mux

Mux

ClockOut

Previous Pixel

Next Pixel

Conf

8 bits configuration

Polarity

Analog Digital

27 September 2004 Michael Campbell

Medipix2 Cell LayoutMedipix2 Cell Layout

55 m

55 m

55 m

55 m

27 September 2004 Michael Campbell

Medipix2 Chip ArchitectureMedipix2 Chip Architecture

IO

Logic

LVDS

Input

LVDS

Output32-bi t C MOS Output

256-bi t Fast Shift Register

3328

-bit

Pix

el C

olum

n-0

13 8-bi t DACs

14111 m

3328

-bit

Pix

el C

olum

n-1

3328

-bit

Pix

el C

olum

n-1

1612

0

m

IO

Logic

LVDS

Input

LVDS

Output32-bi t C MOS Output

256-bi t Fast Shift Register

3328

-bit

Pix

el C

olum

n-0

13 8-bi t DACs

14111 m

3328

-bit

Pix

el C

olum

n-1

3328

-bit

Pix

el C

olum

n-1

1612

0

m256 x 256 pixels10ms readout time

27 September 2004 Michael Campbell

Medipix2 bump bonded to a 300Medipix2 bump bonded to a 300  m Si m Si sensorsensor

27 September 2004 Michael Campbell

Bumps of readout sideBumps of readout side

27 September 2004 Michael Campbell

Bumps of readout side – close upBumps of readout side – close up

27 September 2004 Michael Campbell

9090Sr source scanned in real timeSr source scanned in real time

20 frames per second – limited by DAQ not chip

27 September 2004 Michael Campbell

Calculated incoming spectrum and Calculated incoming spectrum and position of thresholds usedposition of thresholds used

Siefert FK-61-04x12 X-ray tube, W-target, 2.5 mm Al, Vpeak = 25 kV.

Thresholds9.1 keV11.3 keV12.8 keV18.8 keV

27 September 2004 Michael Campbell

Measures MTF @ various thresholdsMeasures MTF @ various thresholds

27 September 2004 Michael Campbell

NPS @ different thresholdsNPS @ different thresholds

NB. Dose changed from threshold to threshold to obtain good statistics

27 September 2004 Michael Campbell

DQE @ different thresholdsDQE @ different thresholds

27 September 2004 Michael Campbell

Summary of measurementsSummary of measurements

27 September 2004 Michael Campbell

Spectrum of X-ray source using energy Spectrum of X-ray source using energy windowwindow

Threshold windows1.4 keV2.8 keV4.2 keV

Sn in bump bond 63%Ag in die attach glue

Siefert FK-61-04x12 X-ray tube, W-target, 2.5 mm Al, Vpeak = 50 kV.

Raw sum of counts in all 64 000 pixels versus global threshold

Spectroscopic information – insight into environment

27 September 2004 Michael Campbell

Image of a Swatch (16.1-19.6 keV)Image of a Swatch (16.1-19.6 keV)

27 September 2004 Michael Campbell

Image of a Swatch (21.6-25.1 keV)Image of a Swatch (21.6-25.1 keV)

27 September 2004 Michael Campbell

Image of a Swatch (27.1-31.4 keV)Image of a Swatch (27.1-31.4 keV)

27 September 2004 Michael Campbell

Image of a Swatch (40.0-43.5 keV)Image of a Swatch (40.0-43.5 keV)

27 September 2004 Michael Campbell

Comparison Comparison

(16.1 – 19.6 keV)(16.1 – 19.6 keV) (21.6 – 25.1 keV)21.6 – 25.1 keV)

27 September 2004 Michael Campbell

Comparison Comparison

(27.1 - 31.4 keV)(27.1 - 31.4 keV) (21.6 – 25.1 keV)21.6 – 25.1 keV)

27 September 2004 Michael Campbell

Comparison Comparison

(27.1 - 31.4 keV)(27.1 - 31.4 keV) (40.0 - 43.5 keV)40.0 - 43.5 keV)

27 September 2004 Michael Campbell

Concluding remarksConcluding remarks The Medipix2 system offers clean particle The Medipix2 system offers clean particle

imagingimaging MTF is typically 70% at pixel pitch. This can MTF is typically 70% at pixel pitch. This can

be enhanced by increasing threshold but at be enhanced by increasing threshold but at the expense of DQEthe expense of DQE

Energy window measurements provide Energy window measurements provide insight into environmentinsight into environment

Quantitative evaluation of the imaging Quantitative evaluation of the imaging properties using the energy window in properties using the energy window in preparationpreparation

Maybe the window should be used to Maybe the window should be used to exclude given energies!exclude given energies!

And finally, a message for those who doubt And finally, a message for those who doubt the future of photon counting energy the future of photon counting energy sensitive imaging systems….. sensitive imaging systems…..

27 September 2004 Michael Campbell

……the clock is ticking!the clock is ticking!

< 1 frame/sec. Limited by DAQ software

27 September 2004 Michael Campbell

AcknowledgementsAcknowledgements

Fellow members of the Medipix ConsortiumFellow members of the Medipix Consortium www.cern.ch/medipix

Colleagues from Nikhef for Muros2 readout system Colleagues from Nikhef for Muros2 readout system J. Visschers H. Verkooijen

Colleagues the Naples group for Medisoft4.0Colleagues the Naples group for Medisoft4.0 P. Russo G. Mettivier M.C. Montesi


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