Progress with GaAs Pixel Detectors K.M.Smith University of Glasgow Acknowledgements: RD8 & RD19 (CERN Detector R.&D. collaboration) XIMAGE (Aixtron, I.M.C.,

Slides:



Advertisements
Similar presentations
Image quality and spectroscopic characteristics of different silicon pixel imaging systems M. G. Bisogni, D.Bulajic, M. Boscardin, G. F. Dalla Betta, P.
Advertisements

First DQE measurment of 500 µm thick Si hybrid pixel sensor with Photon counting readout for X-ray medical imaging M.Caria, J.Chaput, L.Sarry, B.Surre.
STATUS OF MEDIPIX-3, PLANS FOR TIMEPIX-2 X. Llopart.
CHARGE COUPLING TRUE CDS PIXEL PROCESSING True CDS CMOS pixel noise data 2.8 e- CMOS photon transfer.
A silicon microstrip sensor for use in dental digital radiography P.F. van der Stelt Academic Centre for Dentistry Amsterdam, Amsterdam, the Netherlands.
Imaging Properties of the Medipix2 System exploiting Single and Dual Energy Thresholds L. Tlustos 1, R. Ballabriga 1, M. Campbell 1, E. Heijne 1, k Kincade.
B. Mikulec* M. Campbell, E. Heijne, X. Llopart, L. Tlustos CERN, Medipix Collaboration * now with the University of Geneva, Switzerland X-ray Imaging Using.
PHENIX Vertex Tracker Atsushi Taketani for PHENIX collaboration RIKEN Nishina Center RIKEN Brookhaven Research Center 1.Over view of Vertex detector 2.Physics.
Snowmass 2005 SOI detector R&D Massimo Caccia, Antonio Bulgheroni Univ. dell’Insubria / INFN Milano (Italy) M. Jastrzab, M. Koziel, W. Kucewicz, H. Niemiec.
Mid-IR photon counting array using HgCdTe APDs and the Medipix2 ROIC
Photon Counting Sensors for Future Missions
SPIE Instrumentation for Astronomy AO - June22, 2004 John Vallerga, Jason McPhate, Anton Tremsin and Oswald Siegmund Space Sciences Laboratory, University.
Hiroyasu Tajima Stanford Linear Accelerator Center Nov 3–8, 2002 VERTEX2002, Kailua-Kona, Hawaii Gamma-ray Polarimetry ~ Astrophysics Application ~
Photon detection Visible or near-visible wavelengths
ITAM CAS, IEAP CTU IWORID 2004Glasgow, th July IWORID 2004 OPTIMIZATION OF X ‑ RAY DYNAMIC DEFECTOSCOPY USING MEDIPIX-2 FOR HIGH FRAME RATE READ-OUT.
The 6th International Workshop on Radiation Imaging Detectors, July 2004, Glasgow Digital X-ray portable scanner based on monolithic semi-insulating.
K.-F. Pfeiffer, PI4 Universität Erlangen-Nürnberg 1 IWORID 4, September 2002 Large scale x-ray images taken with the Medipix1 chip Karl-Friedrich Pfeiffer.
Applications of a Pixellated Detection System to Digital Mammography
Measurement Results Detector concept works! Flood fields show MCP fixed pattern noise that divides out Spatial resolution consistent with theory (Nyqvist.
Silicon Sensor with Readout ASICs for EXAFS Spectroscopy Gianluigi De Geronimo, Paul O’Connor Microelectronics Group, Instrumentation Division, Brookhaven.
07 October 2004 Hayet KEBBATI -1- Data Flow Reduction and Signal Sparsification in MAPS Hayet KEBBATI (GSI/IReS)
Erik HEIJNE CERN PH DepartmentRADWORKSHOP 29 November 2005 MEDIPIX2 for VERY LOW DOSE INITIAL LHC BENCHMARKING MEDIPIX2 for VERY LOW DOSE INITIAL LHC BENCHMARKING.
Fully depleted MAPS: Pegasus and MIMOSA 33 Maciej Kachel, Wojciech Duliński PICSEL group, IPHC Strasbourg 1 For low energy X-ray applications.
Performance limits of a 55  m pixel CdTe detector G.Pellegrini, M. Lozano, R. Martinez, M. Ullan Centro Nacional de Microelectronica, Barcelona, 08193,
Development of a high-speed single photon pixellated detector for visible wavelengths Introduction A photon incident on the photocathode produces a photoelectron.
Advanced semiconductor detectors of neutrons
Recent developments on Monolithic Active Pixel Sensors (MAPS) for charged particle tracking. Outline The MAPS sensor (reminder) MIMOSA-22, a fast MAPS-sensor.
Energy calibration of the threshold of Medipix for ATLAS Céline Lebel Université de Montréal presenting for the Institut of Experimental.
DynAMITe: a Wafer Scale Sensor for Biomedical Applications M. Esposito 1, T. Anaxagoras 2, A. Fant 2, K. Wells 1, A. Kostantinidis 3, J. Osmond 4, P. Evans.
Strasbourg, France, 17 December, 2004, seminairGrzegorz DEPTUCH  MAPS technology decoupled charge sensing and signal transfer (improved radiation.
Technology Overview or Challenges of Future High Energy Particle Detection Tomasz Hemperek
L.Royer– Calice LLR – Feb Laurent Royer, J. Bonnard, S. Manen, P. Gay LPC Clermont-Ferrand R&D pole MicRhAu dedicated to High.
The development of the readout ASIC for the pair-monitor with SOI technology ~irradiation test~ Yutaro Sato Tohoku Univ. 29 th Mar  Introduction.
Radiation hardness of Monolithic Active Pixel Sensors (MAPS)
A Fast Monolithic Active Pixel Sensor with in Pixel level Reset Noise Suppression and Binary Outputs for Charged Particle Detection Y.Degerli 1 (Member,
HEXITEC ASIC – A Pixellated Readout Chip for CZT Detectors Lawrence Jones ASIC Design Group Science and Technology Facilities Council Rutherford Appleton.
COMETH*: a CMOS pixel sensor for a highly miniaturized high-flux radiation monitor Yang ZHOU, Jérôme Baudot, Christine Hu-Guo, Yann Hu, Kimmo Jaaskelainen,
Prospects to Use Silicon Photomultipliers for the Astroparticle Physics Experiments EUSO and MAGIC A. Nepomuk Otte Max-Planck-Institut für Physik München.
Pixel detector development: sensor
W. Kucewicz a, A. A.Bulgheroni b, M. Caccia b, P. Grabiec c, J. Marczewski c, H.Niemiec a a AGH-Univ. of Science and Technology, Al. Mickiewicza 30,
CMOS Sensors WP1-3 PPRP meeting 29 Oct 2008, Armagh.
X-ray Dynamic Defectoscopy (XRDD) Direct observation of damage development in time dependent gradually stressed materials by means of X-ray transmission.
WG3 – STRIP R&D ITS - COMSATS P. Riedler, G. Contin, A. Rivetti – WG3 conveners.
-1-CERN (11/24/2010)P. Valerio Noise performances of MAPS and Hybrid Detector technology Pierpaolo Valerio.
Monolithic and Vertically Integrated Pixel Detectors, CERN, 25 th November 2008 CMOS Monolithic Active Pixel Sensors R. Turchetta CMOS Sensor Design Group.
Stéphanie Hustache-Ottini S LEIL SYNCHROTRON iWoRID 2011 – 140 – July 5 th Towards ps and fs diffraction with the XPAD detector S. Hustache-Ottini 1, J.-C.
Edgeless semiconductor sensors for large-area pixel detectors Marten Bosma Annual meeting Nikhef December 12, 2011, Amsterdam.
Equalization of Medipix2 imaging detector energy thresholds using measurement of polychromatic X-ray beam attenuation Josef Uher a,b, Jan Jakubek c a CSIRO.
Medipix3 chip, downscaled feature sizes, noise and timing resolution of the front-end Rafael Ballabriga 17 June 2010.
Highlights from the VTX session Marc Winter & Massimo Caccia R&D reports: – DEPFET (M. Trimpl) – CCD (S. Hillert) – UK-CMOS (J.Velthuis) – Continental-CMOS.
NEWS FROM MEDIPIX3 MEASUREMENTS AND IMPACT ON TIMEPIX2 X. Llopart CERN.
Study of Geiger Avalanche Photo Diode applications to pixel tracking detectors Barcelona Main Goal The use of std CMOS tech. APD's in Geiger mode (that.
Semiconductor Detectors and Applications on X-ray imaging Natalie Diekmann Particle Physics 1 NIKHEF.
6:th IWORID, Glasgow, Scotland, July 2004 Energy Dependence in Dental Imaging with Medipix 2 Börje Norlin & Christer Fröjdh Mid Sweden University.
DEVELOPMENT OF PIXELLATED SEMICONDUCTOR DETECTORS FOR NEUTRON DETECTION Prof. Christer Fröjdh Mid Sweden University.
A new family of pixel detectors for high frame rate X- ray applications Roberto Dinapoli †, Anna Bergamaschi, Beat Henrich, Roland Horisberger, Ian Johnson,
Progress with GaAs Pixel Detectors
for the SPiDeR collaboration (slides from M. Stanitski, Pixel2010)
Charge sensitive amplifier
LHC1 & COOP September 1995 Report
HV-MAPS Designs and Results I
Performance of the Medipix and Timepix devices for the recognition of electron-gamma radiation fields C. Teyssier1,3, J. Bouchami1, F. Dallaire1, J. Idarraga1,
Exploring the limits of hybrid pixel detectors with MÖNCH
Characterisation and Application of Photon Counting X-ray Detector Systems Disputation seminar
TCAD Simulation and test setup For CMOS Pixel Sensor based on a 0
Beam Test Results for the CMS Forward Pixel Detector
A new family of pixel detectors for high frame rate X-ray applications Roberto Dinapoli†, Anna Bergamaschi, Beat Henrich, Roland Horisberger, Ian Johnson,
Front-end Digitization for fast Imagers.
Phase Frequency Detector &
Presentation transcript:

Progress with GaAs Pixel Detectors K.M.Smith University of Glasgow Acknowledgements: RD8 & RD19 (CERN Detector R.&D. collaboration) XIMAGE (Aixtron, I.M.C., Metorex, Freiburg, Glasgow, K.T.H.) MEDIPIX (CERN, Freiburg, Glasgow, Pisa) IMPACT (B.N.F.L., E.E.V., Oxford Instr., R.A.L., Glasgow, Imperial College, Leicester, UMIST) NSS Toronto 11/11/’98K.M.Smith

NSS Toronto 11/11/'98K.M.Smith Imaging 3 Requirements 0 Good 2-dimensional resolution(< 100 µm) 0 Linear dynamic range for low contrast (< 3%) 0 Lower dose to Patient/Sample in medical applications 0 Image processing capability (digital image) Readout Electronics Detector - Large dynamic range - 2-dimensional geometry (Pixel) - Single photon counting - High conversion efficiency for  - Low noise energies in the range keV - Digital output - Good charge collection

NSS Toronto 11/11/'98K.M.Smith Why Single Photon Counting?  Linear and extendable dynamic range  Energy threshold 1) Compton suppression 2) Large signal-to-noise ratio 3) Insensitive to leakage current  Local threshold tuning ( for each pixel): - can also be used for gain equalisation  Asynchronous counting Minimum dead time

NSS Toronto 11/11/'98K.M.Smith Photon Counting Devices Monolithic Pixel Detectors  Material budget (H.E.P.) – fabrication – cost – material choices – efficiency – application specific

NSS Toronto 11/11/'98K.M.Smith Photon counting devices Hybrid Pixel Sensors : separation of detector - r/o : material choice : efficiency : dynamic range  smart pixels – cost – spatial resolution – bump bonding

NSS Toronto 11/11/'98K.M.Smith Hybrid Pixel Detectors

NSS Toronto 11/11/'98K.M.Smith Detection Modes Integration : spatial resolution : cheap : experience – dynamic range – detection efficiency – r/o speed – cost (if custom made) – charge integration Photon Counting : individual particle counting : choice of active media : detection-r/o separated : efficiency : dynamic range : “smart” pixels – spatial resolution – bump bonding – cost

NSS Toronto 11/11/'98K.M.Smith Pixel detectors Ω3 ROIC (CERN)  Matrix of 128 rows and 16 columns –Row pitch (depth) = 50  m –Column pitch (width) = 500  m –total area = 8 x 6.35 mm 2  ENC ~ 100 e - rms  Individual pixel addressing (mask + test)  Globally adjustable threshold

NSS Toronto 11/11/'98K.M.Smith Ω3 50  m 500  m 28  m

NSS Toronto 11/11/'98K.M.Smith Image - Washer (Al) full matrix single column 500  m stepsingle column 50  m step GaAs -  3

NSS Toronto 11/11/'98K.M.Smith Image Quality (II) Flood image

NSS Toronto 11/11/'98K.M.Smith MTF comparison

NSS Toronto 11/11/'98K.M.Smith X-Ray Diffraction   d d sin  Bragg’s law 2d sin  = n Powder Method X-ray beam Powder sample 22 detector

NSS Toronto 11/11/'98K.M.Smith Silicon Powder (XRD)

NSS Toronto 11/11/'98K.M.Smith Si-XRD (Resolution)

NSS Toronto 11/11/'98K.M.Smith Potassium Niobate (XRD)

NSS Toronto 11/11/'98K.M.Smith Potassium Niobate (XRD)

NSS Toronto 11/11/'98K.M.Smith Potassium Niobate

NSS Toronto 11/11/'98K.M.Smith MEDIPIX  A true single photon counting readout chip  64 x 64 pixel matrix  pixel dim. 170 x 170  m 2  Sensitive area 1 cm 2  Individually adjust threshold  15-bit counter  Frame r/o 384  s at 10MHz

NSS Toronto 11/11/'98K.M.Smith Image - Objects (Pb) Thickness 600  m GaAs detector

NSS Toronto 11/11/'98K.M.Smith Read-out Electronics Photon Counting Chip (PCC): based on ideas developed by the RD19 collaboration (CERN)  SACMOS 1  m FASELEC Technology * Matrix of 64 x 64 Pixels  Pixel size 170  m x 170  m * 1.2 cm 2 sensitive area * 1.7 cm 2 total area * 1.6 M transistors

NSS Toronto 11/11/'98K.M.Smith Pixel Design 0 Charge sensitive amplifier with leakage current compensation 0 Discriminator with globally settable threshold 0 3-bit local threshold adjustment 0 Individual pixel test and mask modes 0 Counting controlled by shutter signal 0 15-bit pseudo-random counter 0 16-bit I/O Bus 0 Readout frequency: max. 10 MHz  Readout time: 384  s

NSS Toronto 11/11/'98K.M.Smith Performance of readout

NSS Toronto 11/11/'98K.M.Smith Detector performance Interesting energy range for medicine keV [NIST Physical Reference Data]

NSS Toronto 11/11/'98K.M.Smith Detector design  Material: GaAs, S.I., 200  m thick * 64 x 64 pixel matrix  square pixels of 170 x 170  m 2 * 1.2 cm 2 sensitive area

NSS Toronto 11/11/'98K.M.Smith Electrical performance of system System = detector flip-chip bonded to readout chip Bonded detector settings:  min. mean threshold: ~2000 e -  trimmed threshold rms: ~125 e -  noise: ~200 e - (Note: a photon of 20 keV produces about 4700 e - in GaAs)

NSS Toronto 11/11/'98K.M.Smith Measurement of contrast ratio Signal Contrast Ratio: SCR = Signal to Noise: SNR= Distinguishing low contrast objects means:  Earlier recognition of tumours  Reduction of dose to patient Incident photons n n’ Object Detector | n - n’| n n

NSS Toronto 11/11/'98K.M.Smith Comparison of Experimental and Measured Contrast Ratios: Objects with Contrast Ratio of 1.9% can be Identified Results of Contrast Ratio Measurements

NSS Toronto 11/11/'98K.M.Smith Summary and Conclusions 4 Successful bump-bonding of 64 x 64 pixel array to ROIC 4 Measured threshold of ~2000 e - with ~125 e - rms 4 Images of a variety of objects illuminated with 241 Am- and 109 Cd-sources 4 Correctly identified objects of low contrast (1.9 %) 4 The system enables the evaluation of the potential and limitations of the photon counting method

NSS Toronto 11/11/'98K.M.Smith Gain map: detector X2:3 Image correction method

NSS Toronto 11/11/'98K.M.Smith Image correction beforeafter

NSS Toronto 11/11/'98K.M.Smith Hybridized GaAs pixel detector Sens-A-Ray Si-CCD

NSS Toronto 11/11/'98K.M.Smith Source Measurements: 241 Am (  -photons of 60 keV) Steel locking nut; Steel screw  m thick 6 mm long; 1mm slot

NSS Toronto 11/11/'98K.M.Smith Pixelcell Layout Photo 170  m

NSS Toronto 11/11/'98K.M.Smith First Measurement of an Organic Sample with 109 Cd source  Fish Tail irradiation

NSS Toronto 11/11/'98K.M.Smith Measurements with sources: 109 Cd (photons of 22 and 25 keV) Tungsten wire,  500  m 300  m thick copper mask, 300 mm

NSS Toronto 11/11/'98K.M.Smith Contrast Measurements

NSS Toronto 11/11/'98K.M.Smith Electrical performance

NSS Toronto 11/11/'98K.M.Smith Source Measurements: 241 Am (  -photons of 60 keV) Steel screw Steel locking nut; 6 mm long; 1mm slot  m thick

NSS Toronto 11/11/'98K.M.Smith Pixel cell

NSS Toronto 11/11/'98K.M.Smith Hybrid Pixel Detector

NSS Toronto 11/11/'98K.M.Smith Simulated response of ERD1 Si pixel detector

NSS Toronto 11/11/'98K.M.Smith Simulated response of Si pixel detector to 137 Cs

NSS Toronto 11/11/'98K.M.Smith Preliminary evaluation of MEDIPIX read-out chip on Glasgow LEC GaAs pixel detector