monitoring capabilities of the earth charged particle...

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Monitoring capabilities of the Earth charged particle environment J.-A. Sauvaud 1 , S. Bourdarie 2 , R. Ecoffet 3 CESR/CNRS, Toulouse, France ONERA-DESP, Toulouse, France CNES-CST, Toulouse, France First European Space Weather Week ESTEC, Noordwijk, 30 th November 2004

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Monitoring capabilities of the Earth charged particle environment

J.-A. Sauvaud1, S. Bourdarie2, R. Ecoffet3

CESR/CNRS, Toulouse, France

ONERA-DESP, Toulouse, France

CNES-CST, Toulouse, France

First European Space Weather Week

ESTEC, Noordwijk, 30th November 2004

HIGH ENERGY PARTICLES

XMM - EPIC Radiation Monitor

SAC-C Icare

DEMETER IDP

ESA X-ray Multi Mirror Mission (XMM)Launch: December 10, 1999

Orbit: 7000×114,000 km, i= 70°

European Photon Imaging Camera, EPIC EPIC radiation Monitor, ERM

Boer et al.,IEEE Transc. Nucl. Sci., vol.42, n°6, 1995

EPIC Particle Sensors

87 mm

EPIC Low Energy Sensors

Electron energy range: 0.16 – 1.55 MeV

Proton energy range: 1.05 – 2.85 MeV

EPIC Low Energy Sensors

e-

Inci

dent

Ene

rgy

(MeV

)

Deposited Energy (MeV)GEANT4

EPIC HIGH ENERGY SENSORS

Electron energy range: 0.95 – 2.54 MeV

Proton energy range: 8.7 – 76 MeV

EPIC HIGH ENERGY SENSORSIn

cide

ntE

n erg

y(M

eV)

Deposited Energy (MeV)

GEANT4

HIGH ENERGY TABLES

GOES versus XMM proton fluxes at 44.6 MeV

Solar proton eventG

OE

S F

L UX

XMM FLUX

XMM-2001

H+

>4.5 MeV

>17.4

>44.6

SAC-C (CONAE, Argentina)

• Orbit: - 715 x 715km, inclination: 98.2o

• Launch : - 21 Nov 2000 Delta-2 from VAFB

• Instrument : ICARE-CNES - Detector heads derived from the CESR ERM/XMM instrument- Development, operations: CNES- Calibration, science : ONERA- Investigators : R. Ecoffet (CNES), D. Boscher (ONERA)

• Purpose of the instrument: - Space environment - Radiation effects on components (SEE, dose)

ICARE

CPU, data processing (multi-channel analysers) and TM/TC

Component test bed

DC/DC converter board

Acquisition chainsDetectors

Mass: 2.4 kgMean power: 2.5 W281 x 155 x 71 mm Sampling rate: 64s

ICARE detectors“E” detection head

50 µm Siwindow

500 µmAl casing

500 µmSi diode

“P” detection head

150 µmSi diode

500 µmAl casing

6 mm Si/Lidiode

“I” detection head

500 µmSi diode

500 µmAl casing

500 µmSi diode

GEANT-4 simulations

e- Protons

Cross calibration with GOES

y = 0.9303x

0.001

0.01

0.1

1

10

100

1000

10000

0.001 0.01 0.1 1 10 100 1000 10000

flux GOES-P3 (MeV-1cm-2s-1sr-1)

flux

P1

(MeV

-1cm

-2s-

1sr-

1)

Protons, 10.5 MeV

Energy channelsE P IE1 electrons 260 keVE2 electrons 320 keVE3 electrons 360 keVE4 electrons 420 keVE5 electrons 480 keVE6 electrons 560 keVE7 electrons 620 keVE8 electrons 700 keVE9 electrons 820 keVE10 electrons 1200 keV*E11 electrons 1400 keV*

PE0 electrons > 0.9MeVP1 protons 10.5 MeVPE1 electrons 1.5 MeV*PE2 electrons 2. MeV*PE3 electrons 2.4 MeV*PE4 electrons 2.9 MeV*PE5 electrons 3.4 MeV*PE6 electrons 3.9 MeV*P2 protons 15.5 MeVP3 protons 23 MeVP4 protons 33.5 MeV

I1 ions 54 MeV*I2 ions 65 MeVI3 ions > 100 MeV

* contaminated

0

10

20

30

0.1 1 10 100energy (MeV)

e pc

ps pc

electrons

protons

Mirror point in South hemisphere in loss coneDrift shell inside the Earth in SAA

Ele. 300-2500 keV NOAA-15 (825 km 98o)

L* @ 825 km

Ele. 0.5 MeV PROBA (553x677 km 98°)

Jan-Feb 2003

Ele. 0.4 MeV SAC-C (700 km 98°)

Jan-Feb 2003

SAC-C electron results: survey plots

e- 260 keV

e- 560 keV

e- 1.4 MeV

e- 2.9 MeV

before

after

Influence of Solar energetic particles on the proton radiation belt

Example of SAC-C measurements E = 10.5 MeV, 31 March 2001 event

4 months

Influence of Solar Energetic Particles on the Proton RBExample of SAC-C measurements E = 10.5 MeV (715km)

.0.01

0.1

1

10

100

2000.9 2001.1 2001.3 2001.5 2001.7 2001.9 2002.1 2002.3 2002.5 2002.7decimal year

Flux

(MeV

-1cm

-2s-

1sr-

1)

L = 1.9L = 2.9

March 31 Nov. 24

τ ~ 6 months

Effect of the 29-31 October 2003 event seen by ICARE / SAC-C

Effect of rotating coronal hole on outer belt

CME and inner belt injection

“SPACECRAFT ANOMALIES”

ICARE SAC-C ELECTRONS 560 keV

Flux

(10^

) [/M

eV.c

m².s

.sr]

0

1

2

3

4

5

6

2003/04/01 2003/05/11 2003/06/20 2003/07/30 2003/09/08 2003/10/18 2003/11/27 2004/01/060

1

2

3

4

5

6

7

8

9

Time (days )

L-va

lue

ICARE - SAC-C . L-Time Diag ram. Channe l:E560ke V. Smo o th:2

ADEOS-II failure

TIME (Days)

For ~2 years, enhanced fluxesin the proton belt.

Solar events Nov. 2001 (flares = magnetic storms) create conditions for aninjection in the proton belt, whose fluxes build up

In Oct/Nov. 2003, magnetic storms« sweep out » excessfluxes.

A possible explanation for the decrease of SPOT5 mass memory SEU rates after the solar event of the 29/09/04

DEMETER: A FRENCH MICRO-SATELLITE ON A LOW POLAR ORBIT

Goals: Study of human electromagnetic emissions, of ionospheric effects of volcanism and earthquakes…

H+

1.0

0.1 10.01.0

10 1001

Incident energy (MeV)

0.1

0.01

10.0

1.00

0.1

1.00

10.0

Dep

osite

d en

ergy

(MeV

)

e-Electrons:

256 channels from 70 keV to 2.5 MeV

Protons:

An integral channel E > 2.5 MeV

DEMETER-IDP

OUTER BELT – SLOT - INNER BELT

FERMI

E (

eV)

L (R

E)

INNER BELT WAVES EFFECT

INNER BELT WAVES EFFECT

INNER BELT ENERGY SPECTRA

0.1 0.3 0.5 0.7 0.9

100 keV

1

10

100

FLU

X

ENERGY (MeV)

Variation of the resonnant energy with L

INNER BELT - WAVE

(Abel and Thorne, JGR, 1998)

SOUTH OF THE ATLANTIC ANOMALY

NON HARMONIQUES Fréquemment observés au sud de l’Afrique

E (e

V)

H+

e-

e-

> 2.4 MeV

0.7-1.0

0.3-0.7

L

L

L

DEMETER - 2004

DEMETER - 2004

10:24 Nov 7

H+

e-

e-

> 2.4 MeV

0.7-1.0

0.3-0.7

L

L

L

DEMETER - 2004

22:30, Sept. 13

> 2.4 MeV

0.7-1.0

0.3-0.7

H+

e-

e-

L

L

L

LOW ENERGY PARTICLES

Satellite charging

Earth orbiting spacecraft can encounter plasma of vastly diversecharacteristics in the energy range: ~ eV - 60 keV

Versatile and reliable particle experiment are needed. To meet the objectives, the instrumentation has to satisfy the following criteria:

- Be immune to UV flux

- Be immune to high energy particle background

- Provide uniform coverage over a large pitch-angle rangewith a good angular resolution

- Have high sensitivity and large dynamic range (~ 107)

LOW ENERGY PARTICLES

Rely as much as possible on well-proven designs by basing sensor

designs on those successfully flown:

LOW ENERGY PARTICLES

ESRO-1A

GIOTTO

AMPTE

VIKING

FREJA

EQUATOR-S

CLUSTER

CASSINI

MEX

STEREO

VEX

ARCAD-1/2/3

INTERBALL

LOW ENERGY PARTICLES

UV: Three reflections, scalloping, coating

High energy particle background: Coincidence or multiplier sample

Uniform coverage: top-hat (Carlson, Paschmann et al., 1982)

LOW ENERGY PARTICLES

SUMMARY

1) We have the necessary tools to measure/model the Earth’s radiation beltsNew improvements are needed to measure pitch-angle distributions

2) We need a framework to build common experiments

3) Past and ongoing missions will be used to define simple low energy sensors