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1 Space environment: effect on detectors examples with Integral and Astro-H P. Laurent, A. Claret, A. Meuris, D. Renaud (CEA/IRFU) November, 9 th 2012

Space environment: effect on detectors examples with ... · 1 Space environment: effect on detectors examples with Integral and Astro-H P. Laurent, A. Claret, A. Meuris, D. Renaud

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Page 1: Space environment: effect on detectors examples with ... · 1 Space environment: effect on detectors examples with Integral and Astro-H P. Laurent, A. Claret, A. Meuris, D. Renaud

1

Space environment:effect on detectors

examples with Integral and Astro-HP. Laurent, A. Claret,

A. Meuris, D. Renaud (CEA/IRFU)

November, 9th 2012

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1. Description of the space environment.

2. Effect of radiation on electronic devices.

3. Calibration project for Astro-H.

Plan

November, 9th 2012

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The space environment

November, 9th 2012

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Space constraints

� Launch� Chocks, vibrations

� Space environment� Thermal Variations� Vacuum � Radiations � Contamination � Micrometeorites, space debris

November, 9th 2012

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The radiativeenvironment

November, 9th 2012

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Solar activitySunspot

(Galilée, 1610)

11 ±±±± 2 years cycleCycles are not similar !

flares

November, 9th 2012

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Solar particles

Flux 2 1010 p+/cm2 > 10 MeV

Events occuring on hours to days timescale

Emax 300 MeV – 1 GeV

99,9% (solar wind)

November, 9th 2012

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Cosmic Rays

Composition87% protons, 12% alphas, 1% … Solar modulation

November, 9th 2012

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Trapped particlesTrapping mechanisms:

• rotation (Lorentz force)

• Magnetic mirror.

• East-West drift, due to magnetic field gradient.

November, 9th 2012

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Van Allen belts

Solar particles injected from the magnetosphere tail.

Two belts:• Internal (stable)

• External (dynamic)

Protons and electrons coming from cosmic and solar particles interaction into the atmosphere

November, 9th 2012

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South Atlantic Anomaly (1/2)

Dipole fieldlines

Earth magnetic field: • inclined (~10°)• Center offset (~500 km)

SAANovember, 9th 2012

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South Atlantic Anomaly (2/2)

� The South Atlantic Anomaly(SAA) is an area where the Earth's inner Van Allen radiation belt comes closest to the Earth's.

� This leads to an increased flux of energetic particles in this region.

� The effect is caused by the non-concentricity of the Earth and its magnetic dipole.

November, 9th 2012

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Effect of radiations on electronic devices

November, 9th 2012

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Effects on electronic devicesIncident particule

IONISATION

électron-hole pairs creation

(SEE)

Trapping state création

(TID)

Nucleus Fragmentation

ionisation(SEE, TID)

NUCLEAR COLLISION

Displacementdamage

• TID : “Total Ionising Dose” is a long cumulative effect• SEE : “Single Event Effect” is a transient single effect

November, 9th 2012

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Examples

Transient signal (ISOCAM)

SEE ����

Spectral resolution dégradation (XMM)

Dose ����

November, 9th 2012

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Effect of SEEon electronic devices

� Effect of the ionizing particle depends on the energy deposit in the component (LET):

��� = �

��

� Latch-up (SEL) : parasitic current induce by the particle passage which could produce a short-circuit and potentially destroy the component.

� Single event upset (SEU): bit flip in a register.

� Radhard Technics to immunize the electronics against SEE.

November, 9th 2012

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Component tolerance to SEE (1/3)

SEL and SEU (single event latch-up / upset) cross sections with respect to LET (linear energy transfer) :

= �� �

����

Ninc = number of incident ions which will depose a given LET.

Measures of the circuit properties

November, 9th 2012

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Component tolerance to SEE (2/3)Measures of the circuit properties

November, 9th 2012

LET threshold

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� Convolution of the cross section (cm2) by the LET spectrum (cm−2.s−1) gives the foreseen SEE rate (s−1) :

Failure probability in orbit

Orbite Simbol-X; blindage 3,7 mm Al

49 MeV.cm−2.mg−1

10−10.cm−2.s−1

Component tolerance to SEE (3/3)

49 MeV.cm−2.mg−1

������� = 10������ !"�#$ = 410

�&

'��3)*+�,+-.202112�1��-*-"

November, 9th 2012

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Calibration projectfor Astro-H

November, 9th 2012

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Context: ESA contribution to Astro-H

November, 9th 2012

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ASTRO-H

November, 9th 2012

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ASTRO-H

November, 9th 2012

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HXI and SGDHXI SGD

X-rayHard X-ray

November, 9th 2012

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HXI and SGDSi/CdTE compton Gamma Camera

(40-600 keV)

Mechanical model

of SGDNovember, 9th 2012

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Detector for HXI� DS-CdTe : high detection efficiency thanks its atomic number (48-52)

November, 9th 2012

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Study of Astro-H SGD ASICs

November, 9th 2012

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Astro-H orbitLow Earth Orbit� Orbit Altitude: 550 km� Orbit Inclination: ~31 degrees� Orbit Period: 96 minutes� Launch : 2014� 4 years of operation

November, 9th 2012

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Models used to determinethe Astro-H space environment

a) Trapped protons model is AP-8 MAX (NASA/NSSDC)

b) Trapped electrons model is AE-8 MIN (NASA/NSSDC)

c) Solar protons model is SOLPRO (NASA/NSSDC)

d) Cosmic-ray model is GCR-ISO (ISO 15390)

November, 9th 2012

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Dose curve

100 mm

100 rad

November, 9th 2012

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LET spectrum

LET computed with 10 cm Al shielding

Red : trapped protonsGreen : GCR

November, 9th 2012

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Radiation Test (1/2)

HIF accelerator line at Louvain-la-Neuve (Belgium)

November, 9th 2012

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Radiation tests (2/2)

Red : trapped protons

Green : GCR

⇒ SEE probability !!

November, 9th 2012

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Study of Astro-H HXI and SGD CdTe

detectors

November, 9th 2012

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Test bench in CEA

November, 9th 2012

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test equipment for the diodes

Detector board will be adapted for the kit of 10

diodes

November, 9th 2012

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PSI protons accelerator (Switzerland)

November, 9th 2012

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Thank you !

November, 9th 2012