The Challenges Associated with Imaging Technology in Space

Centre for Electronic Imaging The Challenges Associated with Imaging Technology in Space Jason Gow 30th October 2012 Radiation Damage Workshop 2012 ...
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Centre for Electronic Imaging

The Challenges Associated with Imaging Technology in Space Jason Gow 30th October 2012

Radiation Damage Workshop 2012 Image credit: NASA

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Current Missions • Future Missions

Imaging Technology in Space

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Current Missions • Future Missions

Imaging Technology in Space

Three main sources of radiation •

Radiation Belts – High flux environment – High radiation dose



Solar Particle Events – Damaging events are sporadic in nature



Galactic Cosmic Rays – Low flux – High energy Image Credit: E. Daly ESA

Imaging Technology in Space

Radiation Belts •

Inner belt – – –

Dominated by protons Approximately static 100’s of MeV



The Slot – –

Low intensity of electrons Occasional injections of more particles



Outer belt – – –

Dominated by electrons Very dynamic Few MeV

Imaging Technology in Space

Radiation Belts Io

An ultraviolet image of Jupiter's aurora taken with the Hubble Space Telescope in 2007 Europa Ganymede

Jupiter's radiation belts as mapped by Cassini, based on the strength of their radio emissions

Imaging Technology in Space

Solar Particle Events •

The Sun (images from NASA Solar Dynamic Observatory)

Image credit: Imaging Technology in Space NASA

Solar Particle Events •

The Solar Wind – – – –

A stream of charged particles from the Sun’s Corona Velocity of around 670,000 to 2,000,000 mph The solar wind consists of protons and electrons of a few MeV Typically less than 2 keV.nucleon-1, therefore not generally a problem for spacecraft components – Extends over a region of space known as the heliosphere which extends out past the orbit of Pluto.

Solar wind resulting in a geomagnetic storm Credit: NASA

Imaging Technology in Space

Solar Particle Events •

Solar Flares – – – –

During a solar flare the sun ejects radiation across the entire electromagnetic spectrum The flares are classified by the peak X-ray flux in units of Watts per square metre (W.m-2) The soft X-ray flux of large flares can interfere with short-wave radio communication, Hard X-rays can be damaging to spacecraft electronics.

Credit: NASA Stereo

Credit: NASA SOHO

Imaging Technology in Space

Solar Particle Events •

Coronal Mass Ejections – Release around 110 tons of material into space – Often associated with solar flares – The size of an event can be approximated by the soft X-ray emission which precedes them, • Typically the proton shower reaches maximum intensity two or more hours after the soft X-ray emissions • However in January 2005 a shower of protons peaked after only fifteen minutes

Credit: NASA SOHO

Credit: NASA SOHO

Imaging Technology in Space

Solar Particle Events

Imaging Technology in Space

Galactic Cosmic Rays •

Credit: MIT OpenCourseWare

Typically composed of – – – –

85% protons 14% alpha particles 1% nuclides with Z greater than 4 Heavy ions with Z greater than 26 are rare



Cosmic rays are omnidirectional



Accelerated by supernova



Flux rate outside of the Earths magnetic field at 1 AU – 4 protons.cm-2.s-1 – 0.4 helium ions.cm-2.s-1 – 0.04 HZ.cm-2.s-1



Interact with the interstellar medium to produce -rays

Credit: NASA

Credit: Energetic Gamma Ray Experiment Telescope Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad

~42 krad ~30 krad

~34 krad

~6 krad Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad ~150 mrad one year on the International Space Stattion ~2 krad one year in low Earth orbit ~5 krad one year in Mars orbit

~42 krad ~30 krad

~34 krad

~6 krad Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad

~50% chance of nausea (5% chance of death within 8 weeks)

~30 krad

~42 krad ~34 krad

~6 krad Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad 50-100% chance of nausea, mild headache, slight fever, cognitive impairment (5-95% chance of death within 6 weeks)

~50% chance of nausea (5% chance of death within 8 weeks)

~30 krad

~42 krad ~34 krad

~6 krad Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad 50-100% chance of nausea, mild headache, slight fever, cognitive impairment (5-95% chance of death within 6 weeks)

~50% chance of nausea (5% chance of death within 8 weeks)

~30 krad

~42 krad ~34 krad

75-100% chance of nausea, moderate headache, moderate fever, cognitive impairment, 95-100% chance of death within 4 weeks

~6 krad

Imaging Technology in Space

The Space Radiation Environment Cumulative dose per mission phase for JUICE

~100 krad 50-100% chance of nausea, mild headache, slight fever, cognitive impairment (5-95% chance of death within 6 weeks)

~50% chance of nausea (5% chance of death within 8 weeks)

~30 krad

~42 krad ~34 krad

75-100% chance of nausea, moderate headache, moderate fever, cognitive impairment, 95-100% chance of death within 4 weeks

~6 krad

Beyond 3 krad is likely to cause death within 1-2 days

Imaging Technology in Space

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Current Missions • Future Missions

Imaging Technology in Space

Radiation Effects Decrease in solar panel efficiency

Component failure

False stars identified in star trackers

Spacecraft components become radioactive

Spacecraft charging

Single event effects in microelectronics

Decrease in instrument performance, e.g. CMOS and CCD imagers

Surface erosion

Imaging Technology in Space

Radiation Effects

Gate

SiO2

n-type buried channel

p-type epitaxial layer Figure adapted from Janesick 2001 Imaging Technology in Space

Radiation Effects Incoming Radiation

Hole Trap Surface trap (flat band voltage shift) (dark current)

Si interstial

Gate P-V trap (CTI)

Ionisation

Displacement damage (dark spike) SiO2

n-type buried channel

p-type epitaxial layer Figure adapted from Janesick 2001 Imaging Technology in Space

What Image Sensor to Use? •

Often dependant on the mission objectives – Full well capacity – Noise performance – Readout speed



The impact of radiation is dependant on the environment that could be experienced



Charge Coupled Device (CCD) or Complementary Metal Oxide Semiconductor Imaging Sensor? 0V

+ 10 V

0V

0V Electrode or gate

Channelstop

Insulator about 0.1 µm thick Buried channel (n-type) about 1 µm deep Substrate (p-type) typically 600 µm thick

Figure courtesy of David Burt (e2v) Substrate connection (SS)

Stored electrons

Imaging Technology in Space

What Image Sensor to Use? Drive Pulse Connections

Ø1 Ø2 Ø3

Bus lines

+10V

Ø1 Drive Pulses Or “Phases”

0V +10V

Ø2

0V +10V

Ø3

Figure courtesy of David Burt (e2v)

0V

Time

The drive waveforms are sometimes called “clock pulses” with charge transfer achieved by “clocking” the device. Imaging Technology in Space

What Image Sensor to Use? Control region

Irradiated region

X-ray image showing an un-irradiated and irradiated region of a CCD

The CCD was irradiated with protons to level equivalent to 250 years spent at L2. Imaging Technology in Space

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Current Missions • Future Missions

Imaging Technology in Space

Radiation Damage Assessment •

Step 1 – Assess the environment

Imaging Technology in Space

Radiation Damage Assessment Step 2 – Estimate the dose to the sensor 10,000.0 2016 launch, science phase 1,000.0

Dose (krad)



100.0

10.0

1.0

0.1 0

2

4

6 8 10 Aluminium Shielding (mm)

12

14

16

Model of the ESA ExoMars Spacecraft Imaging Technology in Space

Radiation Damage Assessment •

Step 3 – Perform a pre-irradiation characterisation of the sensor

Imaging Technology in Space

Radiation Damage Assessment •

Step 4 – Irradiate the sensor to different levels up to and above the predicted dose

Imaging Technology in Space

Radiation Damage Assessment Step 5 – Perform a post-irradiation characterisation of the sensor

CCD204 2.5E-04 Un-Irradiated

Irradiated with 100% end of life

Serial Charge Transfer Inefficiency



2.0E-04

Irradiated with 200% end of life

1.5E-04

1.0E-04

5.0E-05

0.0E+00 -135

-125

-115

-105 -95 -85 -75 Temperature (oC)Imaging Technology in Space

Radiation Damage Assessment •

Step 6 – Make recommendations for changes to device operation and structure



Change to operating conditions – Change temperature – Change operating speed – Charge Injection

Reduction in serial CTI achieved by the decrease in register width from 50 µm to 20 µm 8.0E-05 7.0E-05

CCD204 CCD273 CCD204 Fit CCD273 Fit

• •

Change to the device structure Change to the mission – Increase shielding – Change orbital parameters

Serial CTI Parallel CTI

6.0E-05 5.0E-05 4.0E-05 3.0E-05 2.0E-05 1.0E-05

Demonstrates a factor 1.7 improvement in the serial CTI

0.0E+00

0.0E+00 2.0E+09 4.0E+09 6.0E+09 8.0E+09 1.0E+10 1.2E+10 1.4E+10 1.6E+10 1.8E+10 10 MeV equivalent proton fluence (protons.cm-2)

Imaging Technology in Space

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Ongoing Missions • Future Missions

Imaging Technology in Space

Hubble •

Hubble Space Telescope 1990 – Wide Field and Planetary Camera (WF/PC) – Wide Field and Planetary Camera 2 (WFPC2), 1993 – Advanced Camera for Surveys (ACS), 2002



M. Sirianni et al, “Radiation Damage in Hubble Space Telescope Detectors”, Radiation Effects Data Workshop, 2007 – Hubble's cameras undergo a monthly anneal to +20 C – A room temperature irradiation would result in these defects not being identified

Imaging Technology in Space

GAIA • • • • •

Catalogue a billion stars with a billion pixel digital camera over a 5 year mission at L2 Launched 2013 Largest array of CCDs ever launched >3Gb/s data generation Requires on-board compression for 3-8Mb/s downlink

106 CCDs forming the GAIA focal plane array Image credit: Airbus Imaging Technology in Space

GAIA •

Increasing charge loss as a result of radiation damage to the CCDs Payload heated

Payload heated

Crowley et al., Radiation effects on the Gaia CCDs in Space after 30 months at L2, Proc. Imaging of SPIETechnology Vol. 9915

Rosetta •

Formation of defects identified by Dr. Neil Murray in images taken with the e2v technologies CCD47-20 used in the NAVigation CAMeras (NAVCAMs)

Image credit: ESA/Rosetta/NAVCAM

Image credit: ESA

Imaging Technology in Space

Contents • Radiation Environment • Radiation Effects • Radiation Damage Assessment

• Past and Current Missions • Future Missions

Imaging Technology in Space

JUpiter ICy moons Explorer (JUICE) • •

JUICE is the first L-class launch slot in the European Space Agencies Cosmic Vision Program foreseen in 2022. The objective of the JUICE mission is the investigation of Jupiter and its icy moons

e2v CIS115

Image credit: Airbus Imaging Technology in Space

Euclid •

Euclid will spend 6 years at L2 where it will study the geometry and nature of the dark Universe through the combination of several techniques of investigation, including – Weak Gravitational Lensing – Baryonic Oscillations



The payload consists of a single telescope and two instruments, the visible imager (VIS) and the near-IR photo-spectrometer (NISP)

Demonstration model of the optical assembly for NISP Image Credit: CNES

Demonstration model of the VIS focal plane array Image Credit: CEA Imaging Technology in Space

Euclid •

Weak Lensing – Measures the change in ellipticity of galaxies to a few percent – Requires the use of multiple galaxies to calculate the amount and distribution of intervening matter 3D reconstruction of the dark matter distribution

Galaxy cluster Abell 2218 and its gravitational lenses, captured by Hubble in 1999

Image courtesy of Richard Massey, R. Massey et al., Dark matter maps reveal cosmic scaffolding, Nature 445 (2007) Imaging Technology in Space

Summary •

It is important to understand the environment in which the sensor will operate to minimise the exposure to extremes. – Increased shielding. – Modify orbital parameters.



By understanding the radiation damage to the sensor it is possible to reduce their impact. – Optimisation of the device operation. – Changes to the design of future devices.



Radiation damage assessments should be performed under mission operating conditions, i.e. temperature, to give the best insight into in-flight performance.



What will the future hold for both CCD and CIS technology for space applications?

Imaging Technology in Space

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