TELEDYNE S HIGH PERFORMANCE INFRARED DETECTORS FOR SPACE MISSIONS. Paul Jerram and James Beletic ICSO October 2018

Size: px
Start display at page:

Download "TELEDYNE S HIGH PERFORMANCE INFRARED DETECTORS FOR SPACE MISSIONS. Paul Jerram and James Beletic ICSO October 2018"

Transcription

1 TELEDYNE S HIGH PERFORMANCE INFRARED DETECTORS FOR SPACE MISSIONS Paul Jerram and James Beletic ICSO October 2018

2 Teledyne High Performance Image Sensors Teledyne DALSA Waterloo, Ontario (Design, I&T) Bromont, Quebec (CCD fab) Teledyne e2v Space Imaging Chelmsford, England (Design, Fab, I&T) Grenoble, France (Design, I&T) Teledyne Imaging Sensors Camarillo, California (Design, Fab, I&T) Teledyne Judson Technologies Montgomeryville, Pennsylvania (Design, Fab, I&T) Teledyne utilizes leading CMOS foundries for fabrication of CMOS image sensors Including staff who work in machine vision (locations not shown on map), Teledyne employs 100 CMOS image designers and 7 CCD designers 2

3 Teledyne Image Sensors Products Infrared and visible sensors Custom cameras Focal plane electronics Laser eye protection & sensor protection Infrared detectors, photodiodes & arrays Detector packaging Custom sensors for tactical and space Infrared cameras Camera electronics Integration and test of IR camera systems Photodiode 1 D Photodiode Array Array Thermoelectrically cooled packaging Custom Visible & IR Arrays for DoD Space Applications High Speed (1600 Hz) Long Wave IR camera for Lab Instrumentation Space Flight Packaging NASA JWST 4 Mpixel Compact Camera Electronics Micro Cam TM Infrared Microscope Camera Aircrew Laser Eye Protection 16 Million Pixel Infrared Astronomy Array High Speed Camera for Tactical Application 3

4 Tunable Wavelength: Unique property of HgCdTe Hg 1-x Cd x Te Modify ratio of Mercury and Cadmium to tune the bandgap energy HgCdTe crystal is grown by MBE on CdZnTe Substrates 2 E g x 0.81x x T 1 2x G. L. Hansen, J. L. Schmidt, T. N. Casselman, J. Appl. Phys. 53(10), 1982, p Teledyne s High Performance IR Sensors for Space Missions

5 Hybrid CMOS Image Sensor Detector Wavelength (λ) Quantum Efficiency Dark current & Noise Radiation environment Persistence The functionality ( the brains ) of a CMOS based sensor is provided by the readout circuit Readout Circuit Input signal Flux object and background Operating Mode Integration time Frame readout time Shutter (rolling, snapshot) Multiple storage cells per pixel Windows Reset (pixel, line, global) Event driven Interface Input (analog, digital) Output (analog, digital) # of readout ports Environment Temperature Radiation Other Requirements Linearity Anti-blooming Teledyne s High Performance IR Sensors for Space Missions

6 Substrate removed HgCdTe Cosmic Ray Incident Photons 6 Note that the incident photons must first pass through the CdZnTe substrate CdZnTe Substrate Cosmic rays in the CdZnTe substrate give fluorescence that creates signal in the HgCdTe Bulk n-type HgCdTe The substrate will also decrease QE below 1.3µm p-type HgCdTe p-type HgCdTe NB schematic is not to scale epoxy ROIC input indium bump silicon multiplexer Output Signal

7 Substrate removed HgCdTe 7 AR Coating Incident Photons Note that the incident photons must first pass through the CdZnTe substrate Cosmic rays in the CdZnTe substrate give fluorescence that creates signal in the HgCdTe Bulk n-type HgCdTe The substrate will also decrease QE below 1.3µm p-type HgCdTe p-type HgCdTe The substrate is removed down to the HgCdTe layer epoxy ROIC input indium bump silicon multiplexer An AR Coating can now be applied to give excellent QE down to below 400nm Output Signal

8 Substrate removed HgCdTe Provides Simultaneous UV Vis IR Light Detection Atmospheric water vapor absorption bands at 1400 and 1900 nm 2510 nm 380 nm JPL AVIRIS NG Imaging Spectrometer Teledyne s High Performance IR Sensors for Space Missions

9 Promise of Fully Depleted HgCdTe Teledyne s high quality HgCdTe is getting even better! Applications will soon benefit from a major reduction in HgCdTe dark current For high flux (300K scenes), will double operating temperature Less expensive cooling options Longer cooler operating lifetime Able to operate LWIR with mini cryo-coolers For low flux applications Lower dark current at standard oper. Temp. Higher operating temperature Longer cooler operating lifetime Status Demonstrated 10X to 100X reduction in dark current LWIR 128x128, 1280x480, and 640x512 arrays have been tested MWIR operated up to 250K LWIR operated up to 160K Strong funding for development Developing partnerships with aerospace primes for system insertion Will utilize for commercial instrumentation products 9

10 CHROMA TM (Configurable Hyperspectral Readout for Multiple Applications) Optimized for imaging spectrometers (hyperspectral imaging) Programmable, digital input: clocks and biases generated on chip Analog output, one output every 160 columns (10 MHz pixel rate) Snapshot, integrate while read, nearly 100% duty cycle CTIA unit cell + 30 x 30 micron pixel pitch + High linearity (>99% linear over full range) + Full well sizes (700 ke, 1 Me, or 5 Me ) Formats (columns by rows; spatial by spectral pixels) Delivered in Delivered in ROICs fabricated Focal plane electronics (16 bit, 10 MHz ADCs, CameraLink interface) Windowing available in row direction Frame readout time scales with number of rows read out + Row readout time is 16.8 microsec + Full frame rate (480 rows) is 125 Hz + Half frame rate (240 rows) is 250 Hz Low power: 90, 150, 180 mw for CHROMA 640, 1280 and 1600 formats Performance (advertised specs): Array Format CDS Noise Well = 0.7M e Well capacity & Readout Noise CDS Noise Well = 1M e CDS Noise Well = 5M e Teledyne s High Performance IR Sensors for Space Missions Power dissipation at 125 Hz [mw] Focal Plane Electronics (FPE) ROIC dimensions [mm] No. Outputs CHROMA e 145 e 600 e x CHROMA e 145 e 600 e x CHROMA e 145 e 600 e x CHROMA e 145 e 600 e x Actual noise performance is 15%-20% lower (better) than listed above CHROMA Sensor Chip Assembly (SCA) CHROMA used by: Several JPL spectrometers CLARREO Pathfinder on ISS Available support equipment: Focal Plane Electronics (FPE): engineering/lab grade only Flex Cables: warm and cold cables, engineering/lab grade only 1 0

11 GeoSnap 18 (Stichable to 3k x 3k) GeoSnap / CHROMA D Design 18 micron pitch pixel CTIA unit cell with 2 gains / full well 100 ke- and 1 Me- or 180 ke- and 2.7 Me- Stitchable design, up to 3K 3K pixels Snapshot, integrate while read Fully digital chip, 14 bit ADCs Full frame rate: 120 Hz for 2K 2K, 250 Hz for 3K 512 ROIC formats fabricated: 2K 2K, 2K 512, 3K 512 Focal plane arrays made and tested with several types of detectors: Visible (Silicon), MWIR (5.3 µm HgCdTe), VLWIR (14.5 µm HgCdTe) GeoSnap 3K 3K GeoSnap 2K 2K ROIC Focal Plane Module CHROMA D 3K 512 CHROMA D 1K 512 ROIC passed radiation tests (no latchup) GeoSnap 2K 2K space flight package developed GeoSnap 2K 2K in production (TRL 6) Being used for Visible, MWIR, VLWIR CHROMA D 2K 512 and 3K 512 being developed for Earth Science applications 11

12 Detectors and missions

13 Teledyne Visible and IR detectors for Euclid Euclid is the European Space Agency s next flagship astronomy mission. Target launch date is Euclid has a 1.2 m diameter large field of view telescope with visible and infrared arrays produced by Teledyne: 600 million visible pixels 36 4K 4K (16 Mpix) CCDs 64 million infrared pixels 16 H2RG (4 Mpix) SWIR arrays 16 SIDECAR ASIC modules Largest IR focal plane array when it launches 24 flight candidate H2RGs delivered to NASA NASA tested and delivered 20 flight grade H2RG arrays to ESA, all of which greatly exceed requirements e2v CCD Quantum Efficiency of 24 flight candidate H2RGs Measured by Goddard SFC Detector Characterization Laboratory Teledyne Imaging Sensors H2RG 2K 2K pixels, 18µm pitch 13

14 H2RG IR Detectors for Euclid Dark Current at 100K Median = e /pix/sec More than 5X better than specification (0.07 e /pix/sec) 2.3 µm cutoff wavelength Readout Noise Median = 6.8 e 40% better than specification (11.5 e ) 14

15 NASA WFIRST Mission H4RG 10: 4K 4K pixels, 10 µm pixel pitch 2.4 meter telescope Technology Maturation ( ) achieved all goals Reduced H4RG 10 noise Increased operability of 16 megapixel IR arrays Demonstrated H4RG 10 flight performance Demonstrated yield for flight production Made the arrays flatter (smaller peak to valley) Reduced image persistence Flight Production commenced in June 2018 Measured by the Detector Characterization Lab, Goddard Space Flight Center 15

16 Missions for Jupiter and it s neighborhood JUICE MAJIS VIS IR Spectrometer Jupiter + Ganymede, Calisto & Europa Lucy L Ralph Vis IR spectrometer Trojan Asteroids Europa Clipper MISE Vis IR spectrometer Europa Europa Image Here 1 H1RG SWIR array 1 H1RG MWIR array 2 SIDECAR ASIC Modules 1 H2RG MWIR array MWIR CHROMA A Focal Plane Electronics 16

17 NEOCam Asteroid Survey Mission Image Sensor Requirements Wavelength (µm) 6 10 Operating temperature range (K) Integration time (s) 10 Dark current (e /s/pixel) <200 Read noise (correlated double sample; e ) <30 Quantum efficiency (%) >60 Well depth (e ) >45,000 Pixel operability (%) (with all above properties) >90 NEOCam will fly two mosaics 2K 8K MWIR (5 µm cutoff) 2K 8K LWIR (10 µm cutoff) MWIR H2RG produced for several years for ground-based astronomy and JWST LWIR now made in 2K 2K format (H2RG) Largest high performance LWIR detectors ever made Each mosaic will be 4 H2RGs Mission will fly 8 H2RGs and 8 SIDECAR ASIC modules Teledyne has developed a new H2RG package and qualified to TRL-6 Active program of continued development 17

18 Avaris NG First Measurements in Europe Switzerland June 2018 AVIRIS-NG Imaging Cube Calibrated Radiance Spectra Instrument Calibration LAEGERN Test Site 380 to 2510 nm 5 nm resolution Teledyne s High Performance IR Sensors for Space Missions

19 High Speed MWIR LWIR Multi Spectral Focal Plane Array JPL FPA measurements (William Johnson & the PHyTIR team) Cutoff wavelength = 12.9 µm Operating temp = 60 K Dark current = 183 e-/pix/sec (spec is <283 e-/pix/sec) Full well optimized per channel, from 6 to 8 million electrons pixels 40 micron pixel pitch 8 spectral channels (4 to 12 µm) Full well optimized per channel 4 rows (selected) read out per channel 30,000 Hz frame rate Developed for HySpIRI TIR Being deployed in ECOSTRESS, installed on the ISS Teledyne s High Performance IR Sensors for Space Missions 19

20 ECOSTRESS first results First light results from ECOSSTRESS. Showing the temperature variation over LA at different times of the day. The ECOsystem Spaceborne Thermal Radiometer Experiment on Space Station (ECOSTRESS) will measure the temperature of plants and use that information to better understand how much water plants need and how they respond to stress Image Courtesy NASA/JPL Caltech

21 If you are interested in this technology please come and talk to Teledyne e2v about how we can meet your needs 21

22 Questions?

ABSTRACT 1. INTRODUCTION

ABSTRACT 1. INTRODUCTION Teledyne s High Performance Infrared Detectors for Space Missions Paul Jerram a and James Beletic b a Teledyne e2v Space Imaging, Chelmsford, UK, CM7 4BS b Teledyne Imaging Sensors, Camarillo, California,

More information

Detectors that cover a dynamic range of more than 1 million in several dimensions

Detectors that cover a dynamic range of more than 1 million in several dimensions Detectors that cover a dynamic range of more than 1 million in several dimensions Detectors for Astronomy Workshop Garching, Germany 10 October 2009 James W. Beletic Teledyne Providing the best images

More information

Scientific Detectors for Astronomy

Scientific Detectors for Astronomy Scientific Detectors for Astronomy 1 December 2008 James W. Beletic Teledyne Imaging Sensors Teledyne NASA s s Partner in Astronomy HST WISE JWST Chart 2 NICMOS, WFC3, ACS Repair Bands 1 & 2 NIRCam, NIRSpec,

More information

High Performance SWIR HgCdTe 320x256/30µm FPAs at Teledyne Judson Technologies

High Performance SWIR HgCdTe 320x256/30µm FPAs at Teledyne Judson Technologies High Performance SWIR HgCdTe 320x256/30µm FPAs at Teledyne Judson Technologies Henry Yuan, Jiawen Zhang, Jongwoo Kim, Carl Meyer, Joyce Laquindanum, Joe Kimchi, JihFen Lei 221 Commerce Drive, Montgomeryville,

More information

Tunable wideband infrared detector array for global space awareness

Tunable wideband infrared detector array for global space awareness Tunable wideband infrared detector array for global space awareness Jonathan R. Andrews 1, Sergio R. Restaino 1, Scott W. Teare 2, Sanjay Krishna 3, Mike Lenz 3, J.S. Brown 3, S.J. Lee 3, Christopher C.

More information

High Resolution 640 x um Pitch InSb Detector

High Resolution 640 x um Pitch InSb Detector High Resolution 640 x 512 15um Pitch InSb Detector Chen-Sheng Huang, Bei-Rong Chang, Chien-Te Ku, Yau-Tang Gau, Ping-Kuo Weng* Materials & Electro-Optics Division National Chung Shang Institute of Science

More information

CCDs for Earth Observation James Endicott 1 st September th UK China Workshop on Space Science and Technology, Milton Keynes, UK

CCDs for Earth Observation James Endicott 1 st September th UK China Workshop on Space Science and Technology, Milton Keynes, UK CCDs for Earth Observation James Endicott 1 st September 2011 7 th UK China Workshop on Space Science and Technology, Milton Keynes, UK Introduction What is this talk all about? e2v sensors in spectrometers

More information

CCD and CMOS Imaging Devices for Large (Ground Based) Telescopes. Veljko Radeka BNL SNIC April 3, 2006

CCD and CMOS Imaging Devices for Large (Ground Based) Telescopes. Veljko Radeka BNL SNIC April 3, 2006 CCD and CMOS Imaging Devices for Large (Ground Based) Telescopes Veljko Radeka BNL SNIC April 3, 2006 1 Large Telescopes Survey telescope Deep probe Primary Mirror dia.=d m, Area= A Large (~8m) Very large

More information

Jan Bogaerts imec

Jan Bogaerts imec imec 2007 1 Radiometric Performance Enhancement of APS 3 rd Microelectronic Presentation Days, Estec, March 7-8, 2007 Outline Introduction Backside illuminated APS detector Approach CMOS APS (readout)

More information

2K 2K InSb for Astronomy

2K 2K InSb for Astronomy 2K 2K InSb for Astronomy Alan W. Hoffman *,a, Elizabeth Corrales a, Peter J. Love a, and Joe Rosbeck a, Michael Merrill b, Al Fowler b, and Craig McMurtry c a Raytheon Vision Systems, Goleta, California

More information

Imaging devices in space

Imaging devices in space Imaging devices in space Roland Meynart Earth Observation Projects European Space Agency Noordwijk, The Netherlands Foreword Imaging devices in space a very wide subject This presentation gives the perspective

More information

Adaptive Focal Plane Array - A Compact Spectral Imaging Sensor

Adaptive Focal Plane Array - A Compact Spectral Imaging Sensor Adaptive Focal Plane Array - A Compact Spectral Imaging Sensor William Gunning March 5 2007 Report Documentation Page Form Approved OMB No. 0704-0188 Public reporting burden for the collection of information

More information

Dynamic Range. Can I look at bright and faint things at the same time?

Dynamic Range. Can I look at bright and faint things at the same time? Detector Basics The purpose of any detector is to record the light collected by the telescope. All detectors transform the incident radiation into a some other form to create a permanent record, such as

More information

Infrared detectors for wavefront sensing

Infrared detectors for wavefront sensing Infrared detectors for wavefront sensing Jean-Luc Gach et al. The project has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 673944 First

More information

Hyperspectral Systems: Recent Developments and Low Cost Sensors. 56th Photogrammetric Week in Stuttgart, September 11 to September 15, 2017

Hyperspectral Systems: Recent Developments and Low Cost Sensors. 56th Photogrammetric Week in Stuttgart, September 11 to September 15, 2017 Hyperspectral Systems: Recent Developments and Low Cost Sensors 56th Photogrammetric Week in Stuttgart, September 11 to September 15, 2017 Ralf Reulke Humboldt-Universität zu Berlin Institut für Informatik,

More information

NOAA EON-IR CubeSat Study for Operational Infrared Soundings

NOAA EON-IR CubeSat Study for Operational Infrared Soundings NOAA EON-IR CubeSat Study for Operational Infrared Soundings Dan Mamula National Oceanic and Atmospheric Administration National Environmental Satellite, Data, and Information Service Office of Project,

More information

Based on lectures by Bernhard Brandl

Based on lectures by Bernhard Brandl Astronomische Waarneemtechnieken (Astronomical Observing Techniques) Based on lectures by Bernhard Brandl Lecture 10: Detectors 2 1. CCD Operation 2. CCD Data Reduction 3. CMOS devices 4. IR Arrays 5.

More information

Multi-function InGaAs detector with on-chip signal processing

Multi-function InGaAs detector with on-chip signal processing Multi-function InGaAs detector with on-chip signal processing Lior Shkedy, Rami Fraenkel, Tal Fishman, Avihoo Giladi, Leonid Bykov, Ilana Grimberg, Elad Ilan, Shay Vasserman and Alina Koifman SemiConductor

More information

Short Wave Infrared (SWIR) Imaging In Machine Vision

Short Wave Infrared (SWIR) Imaging In Machine Vision Short Wave Infrared (SWIR) Imaging In Machine Vision Princeton Infrared Technologies, Inc. Martin H. Ettenberg, Ph. D. President martin.ettenberg@princetonirtech.com Ph: +01 609 917 3380 Booth Hall 1 J12

More information

Where detectors are used in science & technology

Where detectors are used in science & technology Lecture 9 Outline Role of detectors Photomultiplier tubes (photoemission) Modulation transfer function Photoconductive detector physics Detector architecture Where detectors are used in science & technology

More information

Advanced ROIC designs for cooled IR detectors. Xavier Lefoul, Patrick Maillart, Michel Zécri, Eric Sanson, Gilbert Decaens, Laurent Baud

Advanced ROIC designs for cooled IR detectors. Xavier Lefoul, Patrick Maillart, Michel Zécri, Eric Sanson, Gilbert Decaens, Laurent Baud Advanced ROIC designs for cooled IR detectors Xavier Lefoul, Patrick Maillart, Michel Zécri, Eric Sanson, Gilbert Decaens, Laurent Baud Outline Introduction Presentation of latest FPA currently available

More information

Scientific Imaging Sensors

Scientific Imaging Sensors Scientific Imaging Sensors A Short Course presented at the Detectors for Astronomy workshop Garching, Germany 12 October 2009 James W. Beletic and Markus Loose 1 2009 Nobel Prize in Physics awarded to

More information

CCDS. Lesson I. Wednesday, August 29, 12

CCDS. Lesson I. Wednesday, August 29, 12 CCDS Lesson I CCD OPERATION The predecessor of the CCD was a device called the BUCKET BRIGADE DEVICE developed at the Phillips Research Labs The BBD was an analog delay line, made up of capacitors such

More information

Title: HgCdTe Optical & Infrared Focal Plane Array Development in the Next Decade. Abstract:

Title: HgCdTe Optical & Infrared Focal Plane Array Development in the Next Decade. Abstract: Title: HgCdTe Optical & Infrared Focal Plane Array Development in the Next Decade. Abstract: We lay out a comprehensive plan for OIR FPA technology development over the coming decade that promises order-of-magnitude

More information

TAOS II: Three 88-Megapixel astronomy arrays of large area, backthinned, and low-noise CMOS sensors

TAOS II: Three 88-Megapixel astronomy arrays of large area, backthinned, and low-noise CMOS sensors TAOS II: Three 88-Megapixel astronomy arrays of large area, backthinned, and low-noise CMOS sensors CMOS Image Sensors for High Performance Applications TOULOUSE WORKSHOP - 26th & 27th NOVEMBER 2013 Jérôme

More information

TEST RESULTS WITH 2KX2K MCT ARRAYS

TEST RESULTS WITH 2KX2K MCT ARRAYS TEST RESULTS WITH 2KX2K MCT ARRAYS Finger, G, Dorn, R.J., Mehrgan, H., Meyer, M., Moorwood A.F.M. and Stegmeier, J. European Southern Observatory Abstract: Key words: The performance of both an LPE 2Kx2K

More information

Selecting the NIR detectors for Euclid

Selecting the NIR detectors for Euclid National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Selecting the NIR detectors for Euclid Stefanie Wachter Michael Seiffert On behalf of the Euclid

More information

DEVELOPMENT AND CHARACTERISATION OF MCT DETECTORS FOR SPACE ASTROPHYSICS AT CEA

DEVELOPMENT AND CHARACTERISATION OF MCT DETECTORS FOR SPACE ASTROPHYSICS AT CEA DEVELOPMENT AND CHARACTERISATION OF MCT DETECTORS FOR SPACE ASTROPHYSICS AT CEA O. Boulade 1, N. Baier 2, P. Castelein 2, C. Cervera 2, P. Chorier 3, G. Destefanis 2, B. Fièque 3, O. Gravrand 2, F. Guellec

More information

Simulation of High Resistivity (CMOS) Pixels

Simulation of High Resistivity (CMOS) Pixels Simulation of High Resistivity (CMOS) Pixels Stefan Lauxtermann, Kadri Vural Sensor Creations Inc. AIDA-2020 CMOS Simulation Workshop May 13 th 2016 OUTLINE 1. Definition of High Resistivity Pixel Also

More information

Three Ways to Detect Light. We now establish terminology for photon detectors:

Three Ways to Detect Light. We now establish terminology for photon detectors: Three Ways to Detect Light In photon detectors, the light interacts with the detector material to produce free charge carriers photon-by-photon. The resulting miniscule electrical currents are amplified

More information

High Definition 10µm pitch InGaAs detector with Asynchronous Laser Pulse Detection mode

High Definition 10µm pitch InGaAs detector with Asynchronous Laser Pulse Detection mode High Definition 10µm pitch InGaAs detector with Asynchronous Laser Pulse Detection mode R. Fraenkel, E. Berkowicz, L. Bykov, R. Dobromislin, R. Elishkov, A. Giladi, I. Grimberg, I. Hirsh, E. Ilan, C. Jacobson,

More information

Charged-Coupled Devices

Charged-Coupled Devices Charged-Coupled Devices Charged-Coupled Devices Useful texts: Handbook of CCD Astronomy Steve Howell- Chapters 2, 3, 4.4 Measuring the Universe George Rieke - 3.1-3.3, 3.6 CCDs CCDs were invented in 1969

More information

Recent Progress on Developments and Characterization of Hybrid CMOS X-ray Detectors

Recent Progress on Developments and Characterization of Hybrid CMOS X-ray Detectors Recent Progress on Developments and Characterization of Hybrid CMOS X-ray Detectors A. D. Falcone a, Z. Prieskorn a, C. Griffith a, S. Bongiorno a, D. N. Burrows a a Penn State University, Dept. of Astronomy

More information

VII. IR Arrays & Readout VIII.CCDs & Readout. This lecture course follows the textbook Detection of

VII. IR Arrays & Readout VIII.CCDs & Readout. This lecture course follows the textbook Detection of Detection of Light VII. IR Arrays & Readout VIII.CCDs & Readout This lecture course follows the textbook Detection of Light 4-3-2016 by George Rieke, Detection Cambridge of Light Bernhard Brandl University

More information

Minimizes reflection losses from UV-IR; Optional AR coatings & wedge windows are available.

Minimizes reflection losses from UV-IR; Optional AR coatings & wedge windows are available. Now Powered by LightField PyLoN:2K 2048 x 512 The PyLoN :2K is a controllerless, cryogenically-cooled CCD camera designed for quantitative scientific spectroscopy applications demanding the highest possible

More information

NGC user report. Gert Finger

NGC user report. Gert Finger NGC user report Gert Finger Overview user s perspective of the transition from IRACE to NGC Performance of NGC prototypes with optical and infrared detectors Implementation of two special features on the

More information

Charge-Coupled Device (CCD) Detectors pixel silicon chip electronics cryogenics

Charge-Coupled Device (CCD) Detectors pixel silicon chip electronics cryogenics Charge-Coupled Device (CCD) Detectors As revolutionary in astronomy as the invention of the telescope and photography semiconductor detectors a collection of miniature photodiodes, each called a picture

More information

Basic principles of photon detectors used in Astronomy

Basic principles of photon detectors used in Astronomy Basic principles of photon detectors used in Astronomy Reinhold J. Dorn ESO Instrumentation Division 11 September, 2008 1 There are many ways to sense light, but.. these notes will focus on detectors used

More information

A 3 Mpixel ROIC with 10 m Pixel Pitch and 120 Hz Frame Rate Digital Output

A 3 Mpixel ROIC with 10 m Pixel Pitch and 120 Hz Frame Rate Digital Output A 3 Mpixel ROIC with 10 m Pixel Pitch and 120 Hz Frame Rate Digital Output Elad Ilan, Niv Shiloah, Shimon Elkind, Roman Dobromislin, Willie Freiman, Alex Zviagintsev, Itzik Nevo, Oren Cohen, Fanny Khinich,

More information

Vision 2016 Highlights

Vision 2016 Highlights 10 Vision 2016 Highlights Contributions to the Press map. Jan Vermeiren, Business Development Manager Your Presentation Title 2 Caeleste Mission Statement THE Supplier of Beyond state-of-the-art Custom

More information

Properties of a Detector

Properties of a Detector Properties of a Detector Quantum Efficiency fraction of photons detected wavelength and spatially dependent Dynamic Range difference between lowest and highest measurable flux Linearity detection rate

More information

CMOS sensor for TAOS 2

CMOS sensor for TAOS 2 CMOS sensor for TAOS 2 Shiang-Yu Wang ( 王祥宇 ) Academia Sinica, Institute of Astronomy & Astrophysics Taiwan American Occultation Survey Institute of Astronomy & Astrophysics, Academia Sinica, Taiwan Sun-Kun

More information

Near-IR cameras... R&D and Industrial Applications

Near-IR cameras... R&D and Industrial Applications R&D and Industrial Applications 1 Near-IR cameras... R&D and Industrial Applications José Bretes (FLIR Advanced Thermal Solutions) jose.bretes@flir.fr / +33 1 60 37 80 82 ABSTRACT. Human eye is sensitive

More information

Digital-pixel focal plane array development

Digital-pixel focal plane array development Digital-pixel focal plane array development The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published Publisher Brown,

More information

Summary Report for FIRE Spectrometer HgCdTe Detector Array

Summary Report for FIRE Spectrometer HgCdTe Detector Array Summary Report for FIRE Spectrometer HgCdTe Detector Array Craig W. McMurtry, Judith L. Pipher and William J. Forrest University of Rochester, Rochester, NY, USA ABSTRACT This is a summary report covering

More information

Microbolometers for Infrared Imaging and the 2012 Student Infrared Imaging Competition

Microbolometers for Infrared Imaging and the 2012 Student Infrared Imaging Competition Microbolometers for Infrared Imaging and the 2012 Student Infrared Imaging Competition George D Skidmore, PhD Principal Scientist DRS Technologies RSTA Group Competition Flyer 2 Passive Night Vision Technologies

More information

Challenges in Imaging, Sensors, and Signal Processing

Challenges in Imaging, Sensors, and Signal Processing Challenges in Imaging, Sensors, and Signal Processing Raymond Balcerak MTO Technology Symposium March 5-7, 2007 1 Report Documentation Page Form Approved OMB No. 0704-0188 Public reporting burden for the

More information

The superconducting microcalorimeters array for the X IFU instrument on board of Athena Luciano Gottardi

The superconducting microcalorimeters array for the X IFU instrument on board of Athena Luciano Gottardi The superconducting microcalorimeters array for the X IFU instrument on board of Athena Luciano Gottardi 13th Pisa meeting on advanced detectors Isola d'elba, Italy, May 24 30, 2015 Advance Telescope for

More information

ACTIVE PIXEL SENSORS VS. CHARGE-COUPLED DEVICES

ACTIVE PIXEL SENSORS VS. CHARGE-COUPLED DEVICES ACTIVE PIXEL SENSORS VS. CHARGE-COUPLED DEVICES Dr. Eric R. Fossum Imaging Systems Section Jet Propulsion Laboratory, California Institute of Technology (818) 354-3128 1993 IEEE Workshop on CCDs and Advanced

More information

METimage an innovative imaging radiometer for Post-EPS

METimage an innovative imaging radiometer for Post-EPS METimage an innovative imaging radiometer for Post-EPS Dr. Christian Brüns 1, Dr. Matthias Alpers 1, Dr. Alexander Pillukat 2 1 DLR German Space Agency, Königswinterer Straße 522-524, D-53227 Bonn, Germany

More information

Detectors for microscopy - CCDs, APDs and PMTs. Antonia Göhler. Nov 2014

Detectors for microscopy - CCDs, APDs and PMTs. Antonia Göhler. Nov 2014 Detectors for microscopy - CCDs, APDs and PMTs Antonia Göhler Nov 2014 Detectors/Sensors in general are devices that detect events or changes in quantities (intensities) and provide a corresponding output,

More information

Multiple shutter mode radiation hard IR detector ROIC

Multiple shutter mode radiation hard IR detector ROIC Multiple shutter mode radiation hard IR detector ROIC A.K.Kalgi 1, B.Dierickx 1, D. Van Aken 1, A. Ciapponi 4, S.Veijalainen 1, K.Liekens 1, W. Verbruggen 1, P. Hargrave 2, R. Sudiwala 2, M. Haiml 3, H.

More information

Minimizes reflection losses from UV to IR; No optical losses due to multiple optical surfaces; Optional AR coating and wedge windows available.

Minimizes reflection losses from UV to IR; No optical losses due to multiple optical surfaces; Optional AR coating and wedge windows available. SOPHIA: 2048B The SOPHIA : 2048B camera from Princeton Instruments (PI) is fully integrated, ultra-low noise 2048 x 2048, 15 µm pixel CCD camera designed expressly for the most demanding quantitative scientific

More information

IR Detectors Developments for Space Applications

IR Detectors Developments for Space Applications CMOS Image Sensors for High Performance Applications Toulouse, France, 6 th & 7 th December 2011 IR Detectors Developments for Space Applications Harald Weller SELEX GALILEO Infrared Ltd, Southampton,

More information

Back-illuminated scientific CMOS camera. Datasheet

Back-illuminated scientific CMOS camera. Datasheet Back-illuminated scientific CMOS camera Datasheet Breakthrough Technology KURO DATASHEET Highlights The KURO from Princeton Instruments is the world s first scientific CMOS (scmos) camera system to implement

More information

Three Ways to Detect Light. Following: Lord Rosse image of M33 vs. Hubble image demonstrate how critical detector technology is.

Three Ways to Detect Light. Following: Lord Rosse image of M33 vs. Hubble image demonstrate how critical detector technology is. Three Ways to Detect Light In photon detectors, the light interacts with the detector material to produce free charge carriers photon-by-photon. The resulting miniscule electrical currents are amplified

More information

Compatible with Windows 8/7/XP, and Linux; Universal programming interfaces for easy custom programming.

Compatible with Windows 8/7/XP, and Linux; Universal programming interfaces for easy custom programming. NIRvana: 640LN The NIRvana: 640LN from Princeton Instruments is a scientific-grade, deep-cooled, large format InGaAs camera for low-light scientific SWIR imaging and spectroscopy applications. The camera

More information

Abstract. Preface. Acknowledgments

Abstract. Preface. Acknowledgments Contents Abstract Preface Acknowledgments iv v vii 1 Introduction 1 1.1 A Very Brief History of Visible Detectors in Astronomy................ 1 1.2 The CCD: Astronomy s Champion Workhorse......................

More information

High-end CMOS Active Pixel Sensor for Hyperspectral Imaging

High-end CMOS Active Pixel Sensor for Hyperspectral Imaging R11 High-end CMOS Active Pixel Sensor for Hyperspectral Imaging J. Bogaerts (1), B. Dierickx (1), P. De Moor (2), D. Sabuncuoglu Tezcan (2), K. De Munck (2), C. Van Hoof (2) (1) Cypress FillFactory, Schaliënhoevedreef

More information

MR-i. Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements

MR-i. Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements MR-i Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements FT-IR Spectroradiometry Applications Spectroradiometry applications From scientific research to

More information

MR-i. Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements

MR-i. Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements MR-i Hyperspectral Imaging FT-Spectroradiometers Radiometric Accuracy for Infrared Signature Measurements FT-IR Spectroradiometry Applications Spectroradiometry applications From scientific research to

More information

Advanced CCD and CMOS Image Sensor Technology at MIT Lincoln Laboratory

Advanced CCD and CMOS Image Sensor Technology at MIT Lincoln Laboratory Advanced CCD and CMOS Image Sensor Technology at MIT Lincoln Laboratory Vyshnavi Suntharalingam American Physical Society March Meeting 27 February 2012 CCD Focal Planes on Astronomical Telescopes Lincoln

More information

The first uncooled (no thermal) MWIR FPA monolithically integrated with a Si-CMOS ROIC: a 80x80 VPD PbSe FPA

The first uncooled (no thermal) MWIR FPA monolithically integrated with a Si-CMOS ROIC: a 80x80 VPD PbSe FPA DOI 10.516/irs013/i4.1 The first uncooled (no thermal) MWIR FPA monolithically integrated with a Si-CMOS ROIC: a 80x80 VPD PbSe FPA G. Vergara, R. Linares-Herrero, R. Gutiérrez-Álvarez, C. Fernández-Montojo,

More information

Last class. This class. CCDs Fancy CCDs. Camera specs scmos

Last class. This class. CCDs Fancy CCDs. Camera specs scmos CCDs and scmos Last class CCDs Fancy CCDs This class Camera specs scmos Fancy CCD cameras: -Back thinned -> higher QE -Unexposed chip -> frame transfer -Electron multiplying -> higher SNR -Fancy ADC ->

More information

CMOS Today & Tomorrow

CMOS Today & Tomorrow CMOS Today & Tomorrow Uwe Pulsfort TDALSA Product & Application Support Overview Image Sensor Technology Today Typical Architectures Pixel, ADCs & Data Path Image Quality Image Sensor Technology Tomorrow

More information

Stability of IR-arrays for robotized observations at dome C

Stability of IR-arrays for robotized observations at dome C Stability of IR-arrays for robotized observations at dome C 27.3.2007, Tenerife Page Nr. 1 IR wide field imaging MPIA IR projects and studies OMEGA2000: NIR WFI Calar Alto NACO: NIR AO-supported Imager

More information

Low temperature measurements of the large-area, backthinned, and lownoise TAOSII CMOS sensors

Low temperature measurements of the large-area, backthinned, and lownoise TAOSII CMOS sensors Low temperature measurements of the large-area, backthinned, and lownoise TAOSII CMOS sensors Steven Johnson, Jérôme Pratlong, Amr Ibrahim, Paul Jerram, Paul Jorden (e2v technologies) Shiang-Yu Wang and

More information

Fundamentals of CMOS Image Sensors

Fundamentals of CMOS Image Sensors CHAPTER 2 Fundamentals of CMOS Image Sensors Mixed-Signal IC Design for Image Sensor 2-1 Outline Photoelectric Effect Photodetectors CMOS Image Sensor(CIS) Array Architecture CIS Peripherals Design Considerations

More information

Improving the Collection Efficiency of Raman Scattering

Improving the Collection Efficiency of Raman Scattering PERFORMANCE Unparalleled signal-to-noise ratio with diffraction-limited spectral and imaging resolution Deep-cooled CCD with excelon sensor technology Aberration-free optical design for uniform high resolution

More information

Characterization of HgCdTe MWIR Back-Illuminated Electron-Initiated Avalanche Photodiodes (e-apds)

Characterization of HgCdTe MWIR Back-Illuminated Electron-Initiated Avalanche Photodiodes (e-apds) Draft, version 2.0, 24 Oct 2007 Characterization of HgCdTe MWIR Back-Illuminated Electron-Initiated Avalanche Photodiodes (e-apds) M. B. Reine, J. W. Marciniec, K. K. Wong, T. Parodos, J. D. Mullarkey,

More information

CU-LASP Test Facilities! and Instrument Calibration Capabilities"

CU-LASP Test Facilities! and Instrument Calibration Capabilities CU-LASP Test Facilities! and Instrument Calibration Capabilities" Ginger Drake Calibration Group Manager 303-492-5899 Ginger.Drake@lasp.colorado.edu Thermal Vacuum Test Facilities" 2 Multiple Optical Beam

More information

Specifications Summary 1. Array Size (pixels) Pixel Size. Sensor Size. Pixel Well Depth (typical) 95,000 e - 89,000 e -

Specifications Summary 1. Array Size (pixels) Pixel Size. Sensor Size. Pixel Well Depth (typical) 95,000 e - 89,000 e - Apogee Alta Series System Features 1 High Resolution Sensor 1.0 Megapixel sensor with 13 mm pixels delivers a large field of view with high resolution. Programmable TE cooling down to 50 o C below ambient

More information

Hyperspectral goes to UAV and thermal

Hyperspectral goes to UAV and thermal Hyperspectral goes to UAV and thermal Timo Hyvärinen, Hannu Holma and Esko Herrala SPECIM, Spectral Imaging Ltd, Finland www.specim.fi Outline Roadmap to more compact, higher performance hyperspectral

More information

Wind Imaging Spectrometer and Humidity-sounder (WISH): a Practical NPOESS P3I High-spatial Resolution Sensor

Wind Imaging Spectrometer and Humidity-sounder (WISH): a Practical NPOESS P3I High-spatial Resolution Sensor Wind Imaging Spectrometer and Humidity-sounder (WISH): a Practical NPOESS P3I High-spatial Resolution Sensor Jeffery J. Puschell Raytheon Space and Airborne Systems, El Segundo, California Hung-Lung Huang

More information

ISIS TC Meeting. International Spaceborne Imaging Spectroscopy (ISIS) GRSS Technical Committee Meeting, 16/07/2014, IGARSS 2014

ISIS TC Meeting. International Spaceborne Imaging Spectroscopy (ISIS) GRSS Technical Committee Meeting, 16/07/2014, IGARSS 2014 ISIS TC Meeting International Spaceborne Imaging Spectroscopy (ISIS) GRSS Technical Committee Meeting, 16/07/2014, IGARSS 2014 Andreas Müller (DLR) Cindy Ong (CSIRO) Uta Heiden (DLR) Agenda Hyperspectral

More information

A new Infra-Red Camera for COAST. Richard Neill - PhD student Supervisor: Dr John Young

A new Infra-Red Camera for COAST. Richard Neill - PhD student Supervisor: Dr John Young A new Infra-Red Camera for COAST Richard Neill - PhD student Supervisor: Dr John Young The Cambridge Optical Aperture-Synthesis Telescope: COAST is a

More information

Science Detectors for E-ELT Instruments. Mark Casali

Science Detectors for E-ELT Instruments. Mark Casali Science Detectors for E-ELT Instruments Mark Casali 1 The Telescope Nasmyth telescope with a segmented primary mirror. Novel 5 mirror design to include adaptive optics in the telescope. Classical 3mirror

More information

Detectors for AXIS. Eric D. Miller Catherine Grant (MIT)

Detectors for AXIS. Eric D. Miller Catherine Grant (MIT) Detectors for AXIS Eric D. Miller Catherine Grant (MIT) Outline detector technology and capabilities CCD (charge coupled device) APS (active pixel sensor) notional AXIS detector background particle environment

More information

Light gathering Power: Magnification with eyepiece:

Light gathering Power: Magnification with eyepiece: Telescopes Light gathering Power: The amount of light that can be gathered by a telescope in a given amount of time: t 1 /t 2 = (D 2 /D 1 ) 2 The larger the diameter the smaller the amount of time. If

More information

BACKSIDE ILLUMINATED CMOS-TDI LINE SCANNER FOR SPACE APPLICATIONS

BACKSIDE ILLUMINATED CMOS-TDI LINE SCANNER FOR SPACE APPLICATIONS BACKSIDE ILLUMINATED CMOS-TDI LINE SCANNER FOR SPACE APPLICATIONS O. Cohen, N. Ben-Ari, I. Nevo, N. Shiloah, G. Zohar, E. Kahanov, M. Brumer, G. Gershon, O. Ofer SemiConductor Devices (SCD) P.O.B. 2250,

More information

1 2

1 2 Characterization of a Large Format HgCdTe on Si Focal Plane Array Brandon Hanold 1, Donald Figer 1, Joong Lee 1, Elizabeth Corrales 2, Lynn Mears 2, James Bangs 2, Jonathan Getty 2, Mina Mitani 2, C. Keasler

More information

Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region

Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region Feature Article JY Division I nformation Optical Spectroscopy Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region Raymond Pini, Salvatore Atzeni Abstract Multichannel

More information

Evaluation of the Teledyne SIDECAR ASIC at cryogenic temperature using a visible hybrid H2RG focal plane array in 32 channel readout mode

Evaluation of the Teledyne SIDECAR ASIC at cryogenic temperature using a visible hybrid H2RG focal plane array in 32 channel readout mode Evaluation of the Teledyne SIDECAR ASIC at cryogenic temperature using a visible hybrid H2RG focal plane array in 32 channel readout mode Reinhold J. Dorn *1, Siegfried Eschbaumer 1, Donald N.B. Hall 2,

More information

Low Cost Earth Sensor based on Oxygen Airglow

Low Cost Earth Sensor based on Oxygen Airglow Assessment Executive Summary Date : 16.06.2008 Page: 1 of 7 Low Cost Earth Sensor based on Oxygen Airglow Executive Summary Prepared by: H. Shea EPFL LMTS herbert.shea@epfl.ch EPFL Lausanne Switzerland

More information

Performance of the HgCdTe Detector for MOSFIRE, an Imager and Multi-Object Spectrometer for Keck Observatory

Performance of the HgCdTe Detector for MOSFIRE, an Imager and Multi-Object Spectrometer for Keck Observatory Performance of the HgCdTe Detector for MOSFIRE, an Imager and Multi-Object Spectrometer for Keck Observatory Kristin R. Kulas a, Ian S. McLean a, and Charles C. Steidel b a University of California, Los

More information

NIST Agency Report May 2012 OUTLINE. The case for traceability NMI capabilities A view to the future the HIP Current/recent NIST activities

NIST Agency Report May 2012 OUTLINE. The case for traceability NMI capabilities A view to the future the HIP Current/recent NIST activities NIST Agency Report May 2012 OUTLINE The case for traceability NMI capabilities A view to the future the HIP Current/recent NIST activities The case for traceability Earth Radiation Budget: Solar irradiance

More information

Lecture 8 Optical Sensing. ECE 5900/6900 Fundamentals of Sensor Design

Lecture 8 Optical Sensing. ECE 5900/6900 Fundamentals of Sensor Design ECE 5900/6900: Fundamentals of Sensor Design Lecture 8 Optical Sensing 1 Optical Sensing Q: What are we measuring? A: Electromagnetic radiation labeled as Ultraviolet (UV), visible, or near,mid-, far-infrared

More information

Optional AR coating and wedge windows are available

Optional AR coating and wedge windows are available TThe PIXIS series from Princeton Instruments (PI) are fully integrated, low noise cameras designed for quantitative scientific imaging optical spectroscopy applications. Designed utilizing PI s exclusive

More information

Advances in microchannel plate detectors for UV/visible Astronomy

Advances in microchannel plate detectors for UV/visible Astronomy Advances in microchannel plate detectors for UV/visible Astronomy Dr. O.H.W. Siegmund Space Sciences Laboratory, U.C. Berkeley Advances in:- Photocathodes (GaN, Diamond, GaAs) Microchannel plates (Silicon

More information

FPA-320x256-K-2.2-TE2 InGaAs Imager

FPA-320x256-K-2.2-TE2 InGaAs Imager FPA-320x256-K-2.2-TE2 InGaAs Imager NEAR INFRARED (1.2 µm - 2.2 µm) IMAGE SENSOR FEATURES 320 x 256 Array Format 28-pin Metal DIP Package Embedded 2-stage Thermoelectric Cooler Typical Pixel Operability

More information

[90.03] Status of the HST Wide Field Camera 3

[90.03] Status of the HST Wide Field Camera 3 [90.03] Status of the HST Wide Field Camera 3 J.W. MacKenty (STScI), R.A. Kimble (NASA/GSFC), WFC3 Team The Wide Field Camera 3 is under construction for a planned deployment in the Hubble Space Telescope

More information

Calibration of a Multi-Spectral CubeSat with LandSat Filters

Calibration of a Multi-Spectral CubeSat with LandSat Filters Calibration of a Multi-Spectral CubeSat with LandSat Filters Sloane Wiktorowicz, Ray Russell, Dee Pack, Eric Herman, George Rossano, Christopher Coffman, Brian Hardy, & Bonnie Hattersley (The Aerospace

More information

Welcome to: LMBR Imaging Workshop. Imaging Fundamentals Mike Meade, Photometrics

Welcome to: LMBR Imaging Workshop. Imaging Fundamentals Mike Meade, Photometrics Welcome to: LMBR Imaging Workshop Imaging Fundamentals Mike Meade, Photometrics Introduction CCD Fundamentals Typical Cooled CCD Camera Configuration Shutter Optic Sealed Window DC Voltage Serial Clock

More information

IV DETECTORS. Daguerrotype of the Moon, John W. Draper. March 26, 1840 New York

IV DETECTORS. Daguerrotype of the Moon, John W. Draper. March 26, 1840 New York IV DETECTORS Lit.: C.R.Kitchin: Astrophysical Techniques, 2009 C.D.Mckay: CCD s in Astronomy, Ann.Rev. A.&A. 24, 1986 G.H.Rieke: Infrared Detector Arrays for Astronomy, Ann.Rev. A&A 45, 2007 up to 1837:

More information

Advanced ROICs design for cooled IR detectors

Advanced ROICs design for cooled IR detectors Advanced ROICs design for cooled IR detectors Michel Zécri, Patrick Maillart, Eric Sanson, Gilbert Decaens, Xavier Lefoul, Laurent Baud SOFRADIR, Technologies and Products Department, ZI, BP21, 38113 Veurey-Voroize.

More information

Compact Dual Field-of-View Telescope for Small Satellite Payloads

Compact Dual Field-of-View Telescope for Small Satellite Payloads Compact Dual Field-of-View Telescope for Small Satellite Payloads James C. Peterson Space Dynamics Laboratory 1695 North Research Park Way, North Logan, UT 84341; 435-797-4624 Jim.Peterson@sdl.usu.edu

More information

The Wide Field Imager

The Wide Field Imager Athena Kickoff Meeting Garching, 29.January 2014 The Wide Field Imager Norbert Meidinger, Athena WFI project leader WFI Flight Hardware Architecture (1 st Draft) DEPFET APS Concept Active pixel sensor

More information

SOLAR CELL INSPECTION WITH RAPTOR PHOTONICS OWL (SWIR) AND FALCON (EMCCD)

SOLAR CELL INSPECTION WITH RAPTOR PHOTONICS OWL (SWIR) AND FALCON (EMCCD) Technical Note Solar Cell Inspection SOLAR CELL INSPECTION WITH RAPTOR PHOTONICS OWL (SWIR) AND FALCON (EMCCD) August 2012, Northern Ireland Solar cell inspection relies on imaging the photoluminescence

More information

Astro-photography. Daguerreotype: on a copper plate

Astro-photography. Daguerreotype: on a copper plate AST 1022L Astro-photography 1840-1980s: Photographic plates were astronomers' main imaging tool At right: first ever picture of the full moon, by John William Draper (1840) Daguerreotype: exposure using

More information

sensors & systems Imagine future imaging... Leti, technology research institute Contact:

sensors & systems Imagine future imaging... Leti, technology research institute Contact: Imaging sensors & systems Imagine future imaging... Leti, technology research institute Contact: leti.contact@cea.fr From consumer markets to high-end applications smart home IR array for human activity

More information