High Throughput Large Area Silicon Drift Detectors

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KETEK GmbH High Throughput Large Area Silicon Drift Detectors J. Knobloch, T. Eggert, R. Fojt, L. Höllt, A. Pahlke, R. Stötter EPS-TIG Workshop Advanced Radiation Detectors for Industrial Use 1

Outlook KETEK Company Overview History and Basics of Silicon Drift Detectors Small to large area Silicon Drift Detectors New CUBE-ASIC as first pre-amplification stage New 7 channel large area SDD array SDD read out electronics Future requirements for solid state XRF detectors How science and industry can better collaborate (KETEKs view) 2

KETEK at a Glance Family owned enterprise, formation 1989 by Dr. Josef Kemmer Number of employees: 75 Company headquarters & facilities: Munich, Germany Major product lines: SDD-Modules, Arrays, Detector Electronics and Complete Detector Systems; Silicon Photo Multiplier Modules (SiPM) since 2012 Sales and distribution: worldwide Global market share (SDD) 2013: approx. 45% 3

KETEK History 1970-76 Josef Kemmer develops planar Silicon technology for semiconductor detectors 1983 E. Gatti and P. Rehak introduce principle of silicon drift detector 1983 Cooperation between J. Kemmer, P. Rehak and MPI, first SDDs produced at TU München 1985 Cooperation with MPI to develop new detector concepts: SDD with homogeneous entrance window, DEPMOS, DEPFET 1989 KETEK founded by Josef Kemmer 1991 Qualification of Kemmer s planar Silicon process completed 1998 First commercial SDD systems available 2003 2000 th KETEK SDD sold 2010 80mm² KETEK SDD with 120.6eV FWHM in commercial application, just 1eV above the theoretical limit 2012 KETEK SDD on the Mars as part of the NASA rover Curiosity; Words largest (circular) SDD with 150mm² collimated area by KETEK 2013 More than 30.000 KETEK SDD systems in the field; KETEK is the global SDD technology and commercial market leader 4

Industry Applications and Requirements for Silicon Drift Detectors Application XRF Benchtops XRF Handhelds Micro-XRF TXRF EDX in SEM & TEM Major Requirements to X-ray Detector good energy resolution, high throughput, compact housing, low cost high thermal budget, low power consumption, compact housing, high throughput, low cost very good energy resolution and P/B, large area and high throughput for shorter imaging times good energy resolution, large detector area (large solid angle) excellent energy resolution, very good low energy performance, large area, high count rate capability, compact housing, non magnetic materials (TEM) Silicon Drift Detectors fullfill most specific detector requirements replace Si(Li) detectors in high end applications replace Pin Diodes in low end applications 5

KETEK VITUS SDD Silicon Drift Detectors from KETEK 6

Advantage of SDDs performance independent from detector size Very low overall capacitance of SDD modules independent of detector area Spectroscopic performance independent of detector area Extremly large solid angles achievable High count rate / fast measurement applications 7

Silicon Drift Detector with Circular Geometry GN D U OR Driftfield -V U IR Anode Al SiO 2 n + Si n - Si U BACK Homogeneous thin entrance window p + Si Small size of output capacitance: high energy resolution high count rate capability Low leakage current level: operation at moderate cooling no liquid nitrogen necessary 8

SDD Function Principle 9

Basic Construction of a Silicon Drift Detector 10

VITUS Silicon Drift Detectors 2013 VITUS Silicon Drift Detectors X-Ray Detectors for XRF & EDX VITUS H30 40mm² SDD chip; 30mm² active area; multi-layer collimator; 8µm Be window Sizes from 7 150 mm² active area Energy resolutions down to 121eV (Mn K ) Peak to Background > 20.000 Sensitive for soft x-rays from 100eV up to 30keV (detection down to Lithium K line possible) VITUS H50 65mm² SDD chip; 50mm² active area; multi-layer collimator; 12.5µm Be window Vacuum types with high thermal budget: T > 100K No detector fluorescence lines State of the art product in the analytic market 11

Evolution and status of VITUS SDD performance Continuous improvement of typical energy resolution and peak to background ratio FWHM (MnK ): 121.3 ev Peak to Background 25.357 P/T 4.427 30mm² collimated to 20mm² operated at -55 C 2004 : < 139 ev* P/B > 5,000 2006: < 136 ev P/B > 8,000 2008: < 133 ev P/B > 10,000 2010: < 129 ev P/B > 15,000 *FWHM MnK Performance 2013 FWHM down to 121 ev Typical FWHM < 126 ev Typical P/B > 20,000 Perfect gaussian shape of peaks 12

KETEK VITUS SDD Portfolio 2013 13

Further improved thermal budget of VITUS SDDs Corresponds to < 140 ev @ 2 µs PT with new FET Vacuum encapsulated Operation at high ambient temperatures up to 80 C without secondary cooling Low power consumption RoHS compliant 14

New VITUS-CUBE SDD series with ASIC as FET replacement VITUS CUBE series ASIC replaces FET in SDD module: charge sensitive pre-amplification done inside the SDD module directly at the SDDs anode SDD ASIC Advantages 1. extremely low capacitance of total sensor system 2. amplified signal at detector output 3. no ESD sensitive terminals at SDD 4. supports long signal paths -> high count rates in combination with very good energy resolution 15

FWHM @ 5.9 kev (ev) counts VITUS SDD with CUBE-ASIC as FET replacement 190 185 180 175 170 165 160 155 150 145 140 135 130 VITUS SDD with very low capacitance ASIC as primary amplification stage -20 C -10 C 0 C H30 detector 125 0.0 0.5 1.0 1.5 2.0 Peaking Time (µs) Excellent performance at very short peaking times and high chip temperatures Optimum Peaking Time at 0.5 to 1.0 µs 1000000 100000 0 1000 2000 3000 4000 5000 6000 7000 8000 High count rate capability with very good FWHM: < 150 ev with 1 Mcps ICR 10000 1000 100 10 1 Fe 55 test at 1 Mcps ICR 0.44 Mcps OCR 0.45 Peaking Mcps Time OCR 0.1 µs FWHM < 150 ev at 1 Mcps ICR Peaking Time 0.1 µs P/B 17,000 FWHM 152 ev P/B 17,000 Very high count rates without resolution and P/B loss! Energy (ev) 16

VITUS-CUBE SDD Performance FWHM vs ICR < 145 ev @ 1 Mcps and 0.2µs PT 17

VITUS-CUBE SDD Performance Dead Time vs ICR 18

VITUS 150mm² SDD World s Largest Circular Silicon Drift Detector 150 mm² active, collimated chip area 25 µm Dura Coat Beryllium Window Multilayer collimator Housing diameter 22 mm Fill factor ~40% Very efficient built-in peltier element: delta T > 110K at +60 C heat sink temperature Pin layout identical to 80 mm² VITUS SDD 19

FWHM @ 5.9 kev (ev) Counts VITUS H150 210 200 190 180 170 150 mm² SDD 20 kcps ICR FET version -60 C -50 C -40 C -35 C 100000 10000 1000 100 10 150 mm² active area 20 kcps ICR FWHM 130 ev @ 16 µs FWHM 138 ev @ 2 µs P/B 21365 1 0 1000 2000 3000 4000 5000 6000 7000 Energy (ev) 160 150 140 130 0 2 4 6 8 10 12 14 16 Digital Peaking Time (µs) 20

Events H150 Short Signal Rise Times 1000 800 600 150 mm² active area Signal rise time distribution 10%-90% Fe55 signal Medium 130 ns 400 200 0 0 50 100 150 200 250 300 Fe55 signal rise time (ns) 22

Temperature ( C) H150 Cooling Performance KETEKs 150 mm² SDD is vacuum encapsulated allowing for chip temperatures below -60 C at heat sink temperatures of +20 C Maximum Peltier current 1 A Maximum Peltier voltage 9 V -60 C achievable with 460 ma / 4.7 V => TEC power 2.16 W 0-10 -20-30 -40 150 mm² SDD module Vacuum encapsulated Heatsink Temperature +20 C -50-60 Minimum temperature -73 C @800 ma/7.7 V (6.14 W) -70-80 0 200 400 600 800 1000 TEC current (ma) 23

H150-CUBE Version: very good FWHM at short digital peaking times Optimum peaking time 2.0 µs 24

Summary: High Throughput Large Area 150mm² SDD Worlds largest circular SDD now available from KETEK No ballistic deficit, even at very short peaking times of 0.2 µs Excellent energy resolution up to 1Mcps ICR Typical FWHM for FET version 130 ev @ 16 µs, < 140 ev @ 2 µs Vacuum encapsulation allows for operation temperatures below -70 C or operation at high ambient temperatures up to +80 C without secondary cooling stage Typical P/B > 20,000 Multilayer collimator 25 µm Beryllium window All electronics available from KETEK for operation and read out of H150 module 25

New KETEK Large Area SDD Array (available 2014) KETEK 7-Channel SDD Array Active area: 7 x 80 mm² Hexagonal chip design for optimal space filling KETEK 7 element array (560mm²) Very compact design with only 50mm head diameter Independent individual channels Possibility to exchange single channels Including preamp, power supplies, water cooling, optional DPP 25 µm Be window Compact Design with 50mm head diameter 26

KETEK Array Components Pin feed through (7 x 12 pins + backup) Finger (Housing, Vacuum, water cooling, preamplifiers) Housing for Pinch-Off, Getter Water cooling, Ion-getter-pump Connectors for Electronics Detector head Mechanical interface For customer specific ports Electronics PCB 27

KETEK Large Area SDD Array Concept Heatsink Kühlfinge (water cooled) r Flexible Detector concept for large area arrays Flexlead Connector to vacuum pin feedthroug Detector VFC100 28 28

Future Requirements for Energy Dispersive Solid State XRF Detectors Room temperature detectors Lower cost detector systems with simple chip-size package New high transmission x-ray windows as alternative to Be and polymers High direct conversion quantum efficiency up to several 100keV Count rate capability of several Mcps Further improved radiation hardness (today: 10E13 photons) Low energy detection down to 100eV without expensive low energy windows Very large area detector arrays with simple modular readout logic Very low cost, low power, high throughput DPPs for mobile spectrometers Highly integrated combinations of excitation source, detector and readout electronics 29

KETEK on Mars KETEK lands on Mars In August 2012, on board of Mars rover Curiosity and as part of a X-ray spectrometer, KETEK s Silicon Drift Detectors have arrived on the Red Planet. This is already the third mission a VITUS SDD has been chosen by the NASA as XRF detector. Source: Nasa/JPL-Caltech 30

KETEK Electronics KETEK Signal Processing Systems & Electronics 31

AXAS-A Analog X-Ray Spectrometer System KETEK AXAS-A Analog SDD system VITUS SDD Power Supply for Peltier (TEC) Power Supply High Voltage for Ring Biasing Exponential Preamplifier AXAS-A For 7 to 50mm² VITUS SDD Standard Finger Lengths available (50 to 300mm Length) 32

AXAS-D Complete Digital X-Ray Spectrometer System KETEK AXAS-D incl. Digital Signal Processor Complete SDD system VITUS SDD Power Supply for Peltier (TEC) Power Supply High Voltage for Ring Biasing Exponential Preamplifier Digital Pulse Processor (DPP) For 7 to 50mm² VITUS SDD AXAS-D Standard Finger Lengths available (50 to 300mm Length) USB 2.0 (Full Speed) Interface to Host PC Software for Windows XP DLL for data read out of DPP from customer software available 33

AXAS-M Maximum spectroscopic performance KETEK AXAS-M KETEK AXAS-M KETEK AXAS-M2 KETEK AXAS-M1 For 7 150mm² VITUS SDD s Peltier Element Cooling Low Noise Pre-Amplifier All power supplies for SDD and TEC Extremely Low Noise Electronics Standard Finger Lengths available (50 to 300mm) Optimized thermal budget Optional KETEK Digital Pulse Processor (DPP) 34

New Compact AXAS-C for Compact XRF Devices AXAS-C AXAS-C1 AXAS-C2 35

New KETEK OEM Kit for XRF Applications VIAMP & VICO OEM Kit 36

How science and industry can collaborate Today many technology companies like KETEK are mainly industry driven How science and industry can better collaborate (KETEKs view) Workshops like this Scientists to proactively meet technology companies to phrase practical needs / future requirements Industry to proactively seek unsolved technical problems in the academic world IP issues can be resolved by involving technology transfer offices Industry to accept also longer return-in-invest times; e.g. it took more than a decade in industry to migrate from PIN diodes to SDDs Generally enforce synergies between basic, funded research and industries R&D 37

KETEK Website www.ketek.net 38

2 4 YEARS 1989-2013 THANK Y O U 39