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1 Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineeri K.-U. Eichmann , C. von Savigny, G. Rohen, J. Kaiser, H. Bovensmann, J.P. Burrows First retrieval of NIR CH4 profiles from SCIAMACHY measurements? Institute of Environmental Physics University of Bremen Germany

Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering 1 K.-U. Eichmann, C. von Savigny, G. Rohen, J. Kaiser,

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

K.-U. Eichmann, C. von Savigny, G. Rohen, J. Kaiser, H. Bovensmann, J.P. Burrows

First retrieval of NIR CH4 profiles from SCIAMACHY measurements?

Institute of Environmental PhysicsUniversity of Bremen

Germany

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

• vertical resolution: 2.6 km• horizontal resolution in

azimuth direction: 240 km (120 km min.)

• horizontal resolution in flight direction: approx. 400 km

• Duration of Limb sequence: 60 sec.

SCIAMACHY Limb Measurements

Limb view for SOLSE/LORE instruments

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

Requirements UV-VIS-SWIR RTM Limb

SCIATRAN/CDIPI

(A. Rozanov 2001)

SCIARAYs

(Kaiser 2001)

Refraction

Full Sphericity

Multiple Scattering (double scattering)

Ground Reflection

Rayleigh, Mie-Scattering

Analytical Weighting Functions

(In progress)

Computational fast for global analysis of data

Occultation included

Modelling the Radiative Transfer

SCIARAYS: LBL mode, SFC included

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

Optimal Estimation

x0: ln of the a priori O3 profile xn: ln of the nth estimatey: ln of the measured Chappuis-Triplettsyn: ln of the modelled Chappuis-Tripletts for xn

Sx: covariance matrix of the a priori S: covariance matrix of yK: Weighting function matrix

n3

mcmn zOln

THlnyK

yn and K will be determined by the radiative transfer model SCIARAYS [Kaiser, 2001]

xn+1 = x0 + SxKnT[KnSxKn

T + S] -1 (y - yn - Kn(x0-xn))

S = Sx - SxKT[KSxKT + S]-1 KSx

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

Rozanov: Differential retrieval employing O3 Huggins and Chappuis bandsSavigny: 3 wavelength retrieval employing O3 Chappuis bands

10

20

30

40

50

0 1x1012 2x1012 3x1012 4x1012 5x1012 6x1012 7x1012

10 - 40 km O3 columns:

SCIAMACHY: 378 DUPOAM III: 384 DU

Total O3 column:

GOME: 459 DUTOMS: 456 DU

SCIAMACHY - POAM III coincidence on April 25, 2002

SCIA, Rozanov Lat: 56o-59o N, Long: 238o-253o, 18:30 UTC

SCIA, Savigny Lat: 56o-59o N, Long: 238o-253o, 18:30 UTC

POAM, Lat: 62o N, Long: 253o, 2:50 UTC

O3 density [cm -3]

Altitu

de

[km

]

Is SCIARAYS good enough?

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CH4 x-section

Ch. 6 (1000-1750 nm, 1.5 nm)

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CH4 x-section channel 8

Ch. 8 (2265-2380 nm, 0.26 nm)

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Convoluted x-section of CH4

Hitran 2000 database

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VMR profiles of NIR absorbers

Profiles from ACE study

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Radiance at 6 km Tangent height

CH4 (using SCIARAYS in LBL mode)

CH4 (after slit function convolution)

Red: H2OBlue: CO2

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Radiance without CO2 and H2O

Dotted Line: without CO2 and H2O

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High resolution

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Modelled Radiances after SFCTangent heightsevery 3 km between3 and 30 km (from top to bottom), Using SCIARAYS as a RTM.

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Smoothed WF

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WF @ 1666 nm

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Different THs @ Channel 6

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SCIAMACHY Level 1 measurementsat 10 and 16 km

TH = 10 km(twilight measurements)

TH = 10 km(daytime measurements)

TH = 16 km(daytime)

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SCIAMACHY Level 1 measurementsat 10 and 16 km

TH = 10 km(twilight measurements)

TH = 10 km(daytime measurements)

TH = 16 km(daytime)

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SCIA L1: 20 and 26 km

With dead/bad pixels

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Without dead/bad pixel

20 km

26 km

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SCIAMACHY Channel 6: TH=65.8 km

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One state (Ch. 6) at 85 km

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Mesospheric OH emission lines

Black:Night

Red:Twilight

Blue:Day

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Institute for Environmental Physics and Remote Sensing (IUP/ife) Physics/Electrical Engineering

Conclusions

• NIR retrieval chain is not ready yet, but will be in the next few weeks.

• If it is possible to retrieve CH4 from Channel 6 (or Channel 8) from Limb measurements is still an open question.

• OH (both night and day emissions) seems to be a good candidate for further studies.