Technology for High-Z Direct Converting Detectors

Similar documents
Development of high-z sensors for pixel array detectors

Advances in Compound Semiconductor Radiation Detectors. a review of recent progress

Development of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy

Development and characterization of 3D semiconductor X-rays detectors for medical imaging

TIMEPIX3 First measurements and characterization of a hybrid pixel detector working in event driven mode

Special SLS Symposium on Detectors

Mass Determination of Rn and Hg isotopes using MASHA

SYNTHESIS OF SUPERHEAVY ELEMENTS USING THE MASS SPECTROMETER MASHA

Lecture 8. Detectors for Ionizing Particles

DEPFET sensors development for the Pixel Detector of BELLE II

Semiconductor X-Ray Detectors. Tobias Eggert Ketek GmbH

Silicon Detectors in High Energy Physics

Energy calibration of the threshold of Medipix for ATLAS

Components of a generic collider detector

Lecture 18. New gas detectors Solid state trackers

Semiconductor-Detectors

Performance of semi-insulating. insulating GaAs-based radiation detectors: Role of key physical parameters of base material

New trends in CdTe detectors for X and γ-ray applications

Pixels GaAs Detectors for Digital Radiography. M.E. Fantacci. and. Abstract

1) CMOS-Sensors for vertex-detectors 2) CMOS-Sensors for X-ray imaging 3) Sensor with a 3-T-preamplifier 4) Sensor with nearly full depletion

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Silicon Detectors. Particle Physics

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Enhanced lateral drift sensors: concept and development. TIPP2017, Beijing

3.1 Introduction to Semiconductors. Y. Baghzouz ECE Department UNLV

Advantages / Disadvantages of semiconductor detectors

Outline. Introduction, motivation Readout electronics, Peltier cooling Input J-FETsJ

Development of a Radiation Hard CMOS Monolithic Pixel Sensor

Radiation Detector 2016/17 (SPA6309)

Detection of X-ray spectra and images by Timepix

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor

Solid State Detectors Semiconductor detectors Halbleiterdetektoren

High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy

Semiconductor Detectors

Chem 481 Lecture Material 3/20/09

Abstract: J. Urbar [1], J. Scheirich [2], J. Jakubek [3] MEDIPIX CR tracking device flown on ESA BEXUS-7 stratospheric balloon flight

DOUBLE BETA DECAY OF 106 Cd - EXPERIMENT TGV (Telescope Germanium Vertical) EXPERIMENT SPT (Silicon Pixel Telescope)

Double Sided Diffusion and Drift of Lithium Ions on Large Volume Silicon Detector Structure

Edgeless sensors for full-field X-ray imaging

Solid State Detectors

Characterization and Directional Visualization of Space Radiation Quanta in Low Earth Orbit with the compact Spacecraft Payload SATRAM

Peter Fischer, ziti, Universität Heidelberg. Silicon Detectors & Readout Electronics

High-performance direct conversion X-ray detectors based on sintered hybrid lead triiodide perovskite wafers

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations

Development of HPDs. for applications. in physics and medical imaging

The Silicon-Tungsten Tracker of the DAMPE Mission

Gamma and X-Ray Detection

Characterization of 3D thermal neutron semiconductor detectors

EECS130 Integrated Circuit Devices

EECS143 Microfabrication Technology

SLS Symposium on X-Ray Instrumentation

Measurement of the Ionizing Energy Depositions after Fast Neutron Interactions in Silicon

EE495/695 Introduction to Semiconductors I. Y. Baghzouz ECE Department UNLV

Study of Solder Ball Bump Bonded Hybrid Silicon Pixel Detectors at DESY

Graphene films on silicon carbide (SiC) wafers supplied by Nitride Crystals, Inc.

Development of Radiation Hard Si Detectors

EE 5344 Introduction to MEMS CHAPTER 5 Radiation Sensors

Study of Edgeless TimePix Pixel Devices. Dylan Hsu Syracuse University 4/30/2014

High-resolution photoinduced transient spectroscopy of radiation defect centres in silicon. Paweł Kamiński

New perspectives in X-ray detection of concealed illicit materials brought by CdTe/CdZnTe spectrometric detectors

EE143 Fall 2016 Microfabrication Technologies. Evolution of Devices

Direct Detection of >15 kev X-ray Photons on a Hybrid-CMOS Imager

Multi-energy CT: Future Directions. Acknowledgements. Overview 7/23/2014. Taly Gilat Schmidt, PhD. Kevin Zimmerman Franco Rupcich Steven Haworth

Germanium Detectors. Germanium, a special material. Detectors, big is beautiful. Operational features. Applications. Iris Abt

The Hermes Recoil Silicon Detector

Charge sharing in silicon pixel detectors

Spatial resolved efficiency determination of CdZnTe semiconductor detectors with a collimated gamma-ray source for the C0BRA experiment

Preliminary measurements of charge collection and DLTS analysis of p + /n junction SiC detectors and simulations of Schottky diodes

Tests of the BURLE 64-anode MCP PMT as the detector of Cherenkov photons

arxiv: v1 [physics.med-ph] 21 Nov 2013

Contents. General Introduction Low background activities Pixel activities Summary and Outlook. Kai Zuber

Study of semiconductors with positrons. Outlook:

Lecture 7: Extrinsic semiconductors - Fermi level

Hybrid X-ray Area Detectors for High-Flux Applications

12/10/09. Chapter 18: Electrical Properties. View of an Integrated Circuit. Electrical Conduction ISSUES TO ADDRESS...

Introduction to Semiconductor Physics. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

GaN for use in harsh radiation environments

Halbleiter. Prof. Yong Lei. Prof. Thomas Hannappel.

ISSUES TO ADDRESS...

M. De Napoli, F. Giacoppo, G. Raciti, E. Rapisarda, C. Sfienti. Laboratori Nazionali del Sud (LNS) INFN University of Catania. IPRD Oct.

CVD Diamond History Introduction to DDL Properties of Diamond DDL Proprietary Contact Technology Detector Applications BDD Sensors

Study of the radiation fields in LEO with the Timepix detector

ISPA-Tubes with YAP:Ce Active Windows for X and Gamma Ray Imaging.

Nanoscience galore: hybrid and nanoscale photonics

Hall effect in germanium

Inelastic soft x-ray scattering, fluorescence and elastic radiation

EV Group. Engineered Substrates for future compound semiconductor devices

EE130: Integrated Circuit Devices

Introduction to Semiconductor Integrated Optics

Scientific astrophysical payloads for pico and nano-satellites

A t XFEL experiment, sensors should have. Capacitance calculations in p + n silicon pixel sensors using three dimensional TCAD simulation approach

A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced.

Diffraction: spreading of waves around obstacles (EM waves, matter, or sound) Interference: the interaction of waves

Integrated measuring system for MEMS

GEM at CERN. Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM

Currently, worldwide major semiconductor alloy epitaxial growth is divided into two material groups.

Au-Ti THIN FILMS DEPOSITED ON GaAs

Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies.

Chap. 11 Semiconductor Diodes

Chemistry Instrumental Analysis Lecture 8. Chem 4631

Transcription:

Technology for High-Z Direct Converting Detectors Michael Fiederle Freiburger Materialforschungszentrum ANKA KIT

Outline Background high-z detector materials High-Z semiconductor production High-Z semiconductors technology The early bird gets the worm - I hate worms High-Z pixel detectors with Medipix3 Summary and Outlook 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 2

Radiation detectors with high-z materials Single detectors with high energy resolution for isotope identification Compact Systems Pixel detectors: combination with electronics Spatially resolving systems Tracking of charged particles 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 3

Potential applications of high-z pixel detectors X-ray Imaging (2D imaging): - Pixel detectors with µm resolution X-ray Diffraction: - Large areas detectors High flux X-ray CT applications: - Pixel detectors with 200 µm and higher spatial resolution - High photon fluxes: 10 9 mm 2 /s and higher - Medical CT: Protytypes by GE Health Siemens Philips 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 4

High Z direct converter X-ray detectors Direct converter => semiconductor material combination with Photon Counting Chip: Counting instead of integration Hybridisation of detector and electronic: Flip-chip bonding technology Semiconductor materials: - CdTe - CdZnTe - GaAs 03.04.13 MRS 2013- M. Fiederle, GaAs Pixeldetectors 5

High-Z semiconductors X-ray detectors X-ray sensor = bulk device: active volume = sensor thickness Absorption (efficiency) correlated with thickness Efficiency of Silicon above 20 kev too low => Compound semiconductor Required material properties: High resistivity > 10 8 Ohmcm (intrinsic) High mobility-lifetime product Homogeneity of electronic properties (µm-range) 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 6

Potential candidates high-z semiconductors S. Del Sordo et al., 2009, Sensors 2009, 9, 3491-3526 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 7

Potential candidates high-z semiconductors Absorption Resistivity Charge Transport Quality Technology Si + ++ +++++ +++++ +++++ Ge ++ + +++++ +++++ +++ cooling GaAs ++ +++ +++ ++++ +++ CdTe +++ +++ +++ +++ +++ CdZnTe +++ ++++ +++ ++ +++ HgI 2 Most ++++ promising ++++ candidates: ++ CdTe, CdZnTe + and GaAs + TlBr Compromise ++++ ++++ of: - Efficiency ++ + + - Quality - Stability Efficiency - Available Noise planar Spectr. technology Size Pixel Performance detectors 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 8

High-Z detectors applications Strong need for high-z detectors but.. Most scientists do not like high-z materials Why? High-Z technolgy High-Z is Alchemy: Alchemy, Voodoo, Black Magic Crystal growth only at full moon Bonding around midnight. 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 9

Facts high-z semiconductor materials Facts high resistivity >10 9 Ohmcm sensitive to temperature and force complex equillibrium of shallow and deep levels (impurites + defects) Constant improvement of material and technology (since 1960) Suitable planar technology available Myth unpredictable performance unstable materials undoped semiconductor promised performance but no improvement in recent years no technology available (different to Si-technology!) wafers with 3 diameter available 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 10

High-Z detector material Compensation of shallow levels: - Complex situation of several defects + impurities - Adjustment of doping within a few ppb 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 11

CdTe and CdZnTe crystal grower Merge of material supplier + technology + system suppliers: - Orbotech with GE - GammaMedica / IDEAS with GE - ev with Kromek, UK - AJAT with XCounter - Acrorad owned by Siemens 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 12

CdTe detector wafers CdTe crystals from Acrorad 3 (75 mm) diameter single crystals High resistivity: 5 x 10 9 Ohmcm Good homogeneity of electrical properties 3 wafers for planar technology processing 1 and 2 mm thickness Resistivity map 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 13

GaAs for X-ray sensors Long term history Different approaches: Bulk material LEC GaAs undoped LEC GaAs Cr doped (Thick) thin films: Vapor Phase epitaxy GaAs Liquid Phase Reminder: epitaxy GaAs - GaAs is commercial available material - GaAs wafers up to 8 inch diameter - Growth methods: Liquid Encapsulated Czochralski LEC and Vertical Gradient Freeze VGF - Semi-insulating (undoped using EL2 defect) 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 14

GaAs X-ray detectors A. Owen et al. 2001 P. Kostamo et al. 2008 R. Irsigler (ACREO) et al. 2001 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector L. Tlustos, C. Fröjdh (MSU) et al. 2007 15

GaAs X-ray detectors LEC GaAs: - dislocation network - instable performance - small depletion width Epi - GaAs: - small area - no flat surface - small thickness M. Fiederle et al. 2006 M. Fiederle et al. 2011 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 16

Pixel detectors produced at FMF Processing 3 inch wafers: Metallization Passivation UBM deposition Backside preparation Backside contact (CdTe) Dicing Hybridization Module assembling Medipix2/3: - Mounting assembly - Wirebonding - Testing In-house processing FMF 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 17

Flip chip bonding CdTe / GaAs at FMF Bumps deposited on detector wafer Low temperature bumps using In-Sn alloy Low temperature and low stress polymer passivation Limitations: - Minimum size of bump: 15 µm diameter - Dead area between pixels and sensor edge: 200 µm - Maximum size of monolithic sensor limited by wafer diameter of 75 mm Maximum CdTe/ GaAs module: 28x43 mm 2 400.000 pixels (Medipix) 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 18

Improvement of technology Medipix bump Detector 25.05.2013 Synchrotron Laminography of bump-bonds (GaAs flip-chip technique) Feng Xu, KIT HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 19

Medipix detectors Developed by Medipix2 / Medipix3 Collaborations @ CERN Medipix detector: Electronics chip (ASIC) + sensor Medipix3 single 14x14 mm² Medipix2 Hexa 28x42 mm² 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 20

Technical data: MPX2 vs. MPX3 MPX2 MPX3 Technology: 0.25 µm CMOS 0.13 µm CMOS Pixels: 256x256 256x256 Pixel dimens.: 55 µm 55 µm 110 µm Color Mode Pixel area: 14.08x14.08 mm² 14.08x14.08 mm² Active IC area: 87.1 % 88.4 % bottom WB 94.3 % TSV Counter: 1x 13.5 bit 2x 12 bit (11,810) (2x 4,096 / 16,777,216) 8x 12 bit Color Mode Thresholds: THL + THH 2x THL 8x THL Color Mode R. Ballabriga et al., Medipix3: A 64 k pixel detector readout chip working in single photon 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector counting mode with improved spectrometric performance, NIM A 2011 21

MPX3 front-end operating modes Single Pixel Mode (SPM) every pixel works independently of its neighbours, behaving in a way similar to the working mode of traditional detectors Charge Summing Mode (CSM) The charge in every cluster of 4 pixels is added and assigned to the pixel with the largest charge deposition. Colour Mode The readout pixels are grouped in clusters of four and become a single detection unit. In this mode, the pixel pitch is 110 µm x 110 µm and only one readout pixel in four is bump bonded. Colour Mode can be programmed for Single Pixel operation and Charge Summing operation. R. Ballabriga et al., Medipix3: A 64 k pixel detector readout chip working in single photon 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 22 counting mode with improved spectrometric performance, NIM A 2011

Medipix3 sensors Si: - 300 µm - 700 µm CdTe: (ohmic c.) - 800 µm - 1 mm - 2 mm GaAs: - 500 µm CdTe GaAs Si 300 1000 500 µm µm 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 23

GaAs sensors Sensors by Tomsk S.U. Bonding by FMF GALAPAD Project: Coordinated by H. Graafsma: Partners: Tomsk SU, JNIR Dubna, DESY, KIT and FMF 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 24

Images with GaAs assemblies TPX assembly 25 kv 200 V TH0 20 kev 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 25

Images with GaAs assemblies TPX assembly 25 kv 200 V TH0 20 kev 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 26

Spatial resolution of GaAs assemblies MPX3 assembly 25 kv 200 V TH0 6 kev 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 27

High flux measurements synchrotron 10 8 photons / mm 2 s 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 28

High flux measurements synchrotron 10 8 photons / mm 2 s Limitation by Medipix3 electronics 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 29

Images with GaAs assemblies Bias: -200 V MPX3 GaAs SPM 24-Bit 8x6 tiles image by Simon Procz 25.05.2013 MPX3 assembly 25 kv 200 V TH0 6 kev HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 30

GaAs Medipix3 RX Bias: -200 V MPX3 GaAs SPM 24-Bit 8x6 tiles image by Simon Procz 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 31

Latest version Medipix3RX CdTe 3RX assemblies Charge Summing Mode 55 µm pixel 110 µm pixel 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 32

CdTe Medipix3 RX assemblies 55 µm pixels - Spectroscopy 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 33

CdTe Medipix3 RX 110 µm pixels 2 mm thickness - Spectroscopy 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 34

Energy selective, planar imaging MPX3 CdTe 1mm - Colour Mode 110µm Piezo Lighter Magnification: 1.3x Bias: -320V MPX3 CdTe 1mm Colour Mode 4x11 tiles RGB: 9-50 kev A: Logarithmic grayscale sum B: Coloured X-ray image 9-14 kev 14-23 kev 31-50 kev C: Linear grayscale sum 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 35

High resolution imaging MPX3 CdTe 1mm SPM 55µm CF card Width: 42.8 mm Mag. 1.74x Bias: -290 V MPX3 CdTe SPM 24-Bit 8x7 tiles Intensity image by Simon Procz 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 36

Our first CdTe reconstruction Monkey Skull CT reconstruction width ~40mm MPX3 CdTe 55µm SPM 24-Bit 5x4 tiles image by Simon Procz 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 37

CdTe Hexa Modul Timepix Large module: 28 x 43 mm 2 from 3 wafers Hexa module (3x2 Medipix) 55 µm and 165 µm pixels 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 38

Hexa-Modul with 55 µm pixels Selective pixel median filter algorithm only filters noisy pixels 512x768 pixels ~400000 pixels 28x43 mm² area 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 39

CdTe Hexa 55 µm CdTe Hexa 28x43 mm 2 with Medipix 3RX Assembling of HGF-Cube on LAMDA-boards from DESY First Medipix3 Hexa CdTe assembly

CdTe Hexa 28x43 mm 2 with Medipix 3RX: First image with Helmholtz Cube: Single Pixel Mode Measurements by D. Pennicard DESY)

CdTe Hexa 28x43 mm 2 with Medipix 3RX: First image with Helmholtz Cube: Charge Summing Mode Measurements by D. Pennicard DESY)

Summary & Outlook Summary: - Continous development of high-z pixel detectors: - Pixel detectors with GaAs and CdTe available - Improvement of performance and technology by intensive characterization - Manufacturing of pixel detector systems - High flux up to 10 8 photons/mm 2 /s Outlook: - CdTe and GaAs pixel detector systems with Hexa modules 42x28 mm 2 active area - Medipix3 systems for application at beamlines - Crystal growth of larger diameters 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector 43

Acknowledgement Teams FMF: Martin Pichotka, Leonhard Alaribe, Simon Procz, Andreas Zwerger, Alex Fauler (Processing and Bonding) KIT - ANKA: Angelica Cecilia, Elias Hamann, Thomas König, Tilo Baumbach Medipix2 and Medipix3 collaboration 44 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector

Acknowledgement Funding: BMBF: 05K10CKA Pixeldetektoren Synchrotron EDAS2010 05K10VFA GaAs Pixeldetectors GALAPAD 05K10VFC GaAs Pixeldetectors GALAPAD EU FP7: EU Project No. 218027 LACX Large x-ray detectors for Colored X-ray Imaging Uni Freiburg Anschubfinanzierung BIRD KIT ANKA Finanzierung BIRD Thank you for your attention! 45 25.05.2013 HGF Heräus Seminar - M. Fiederle, Technology High-Z Detector