LYRA on-board PROBA2 EUV irradiance inter-calibration workshop M. Dominique + LYRA team October 2011, LASP.

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Presentation transcript:

LYRA on-board PROBA2 EUV irradiance inter-calibration workshop M. Dominique + LYRA team October 2011, LASP

PROBA2 orbit PROBA2 orbit:  Heliosynchronous  Polar  Dawn-dusk  725 km altitude  Duration of 100 min  Occultation season:  Visible:October-February  Maximum duration 20 min per orbit

4 5 mm LYRA highlights 1: View-limiting aperture (Ø 8mm) 2: precision aperture (Ø 3mm) 3: filter 4: LEDs (λ 375 and 465 nm) 5: detector (Ø 4mm)

Diamond detectors

Details of LYRA channels

Filter + detector responsivity Unit 1 Unit 2 Unit 3

Operation: systematic campaigns Integra- tion time UnitsCover status LED status PointingOccur- ence Range10ms  10s max. two at a time open / close off / 375nm / 465nm 0° (Sun)  3° Nominal50 msU2openoffSun N/A Back-up A 50msU2+3openoffSun1 / 2weeks Back-up B 50msU2+1openoffSun1 / 3months Calibra- tion 50ms1) U2+1 2) U2+3 closeoff (DC) on (LED) N/A1/ 2weeks Paving50ms -openoffFrom 0° to 3° occasio- nal

Operation: occasional campaigns  Scientific campaigns  Observation of flares: unit 2 and 3  Occultations in all three units  Eclipses in all three units  Bake-out => no real effect so far

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

Time after first light (days) Uncalibrated signal (counts/ms) Degradation of unit 2 > 95% ~ 90% ~ 25% Corrected signal (counts/ms) Time after first light (days)

Degradation of units 1 and 3 30% 15% / / 10% 20% 10% /

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

Dark current evolution Variations correlated with temperature evolution I. Dammasch + M. Snow A. De Groof Temperature evolution Dark current in Lyman alpha

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

LED signal time series  Very little change over the mission.  Bimodal appearance is due to systematic difference between first and second measurements during each observing sequence. Low detector degradation, if any M. Snow

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

Probing the evolution of bandpasses: occultations ~ 900 nm Unit 3

Long term evolution Work still in progress … Various aspects (to be) investigated:  Degradation due to contaminant layer  Dark current evolution (detector degradation)  Response to LED signal acquisition (detector spectral evolution)  An alternative way to probe the spectral evolution (detector + filter): occultations  Flat-field evolution

Flat-field evolution mm Unit 1 Unit 2 (nominal) Unit 3 5mm substrate

Non-solar features in LYRA data Large Angle Rotations Flat field 1.LAR: four times an orbit 2.SAA affects more Si detectors independently of their bandpass

Non-solar features in LYRA data 1.Occultation: from mid-October to mid- February 2.Auroral perturbation Only when Kp > 3 Only affects Al and Zr channels independently of the detector type Does not affects SWAP (though observing in the same wavelength range) Occultations

Data products Data products and quicklook viewer on

Collaborations