SO2 data and alert service

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Product information

Introduction
 
Slant column density vs.
vertical column density
Geographic regions
Data presentation
and delivery
Solar Zenith Angle
What is the Dobson Unit?
 
Slant column retrieval
Background correction
Reference spectrum
Cloud cover fraction
 
Near-real time service
Criteria for exceptional
SO2 concentrations
 
Air-mass factor using
look-up tables
Air-mass factor using a
chemistry transport model
SO2 column from OMI
 
Time period of
available data
Data format specification
Data and Service
version history
Validation of the
data products
South Atlantic Anomaly
 
Downloading
data & image files
Documentation
References
Acronyms
Acknowledgments


 
NOTE:   This is the OLD product info. Some parts of it are no longer up to date, while other parts are missing -- see the remark on the main product info page.

SO2 slant column retrieval

The SO2 slant column density, usually given in Dobson Units (DU), are retrieved from UV measurements made by satellite based instruments, such as GOME-1, SCIAMACHY (in the nadir-viewing mode) and GOME-2. The retrieval method applied to the measurements of these instruments is the Differential Optical Absorption Spectroscopy (DOAS) technique.

SO2 data based on OMI is derived in a somewhat different way: with a "band residual method" using the residuals of the DOAS-based ozone retrieval. More info and links can be found in the section on the SO2 column from OMI.

 
The retrieval of the SO2 slant column is done from the spectrum in the wavelength range 315-326 nm, where SO2 shows clear absorption features. In the same wavelength range, however, there is also absorption by ozone (O3). The retrieval must therefore take both SO2 and O3 into account. There is, so to say, an "interference" of the two absorption signals when matching the measured spectrum with the absorption cross sections of SO2 and ozone.

Cross section of SO2 and Ozone
Cross sections of SO2 (red) and ozone (blue) in the wavelength range used for the SO2 slant column retrieval.

The result of this "interference" is that when concentrations of SO2 are low, the retrieval may give negative SO2 slant column values, with an error of the same magnitude. This then represents the SO2 background level, i.e. the apparent SO2 absorption in the absence of emissions of SO2. The negative values are, of course, not physical, but due to the fact that it is not possible to retrieve SO2 independently from ozone.

For low Solar Zenith Angles (SZAs), i.e. at low and mid latitudes, the SO2 background level is of the order of 1 Dobson Unit (DU) and emissions of SO2 (by pollution or volcano eruptions) will be visible against this background.

For higher SZAs, however, there is a problem. The higher the SZA, the longer the slant path is along which the retrieval takes place. Because of the vertical and horizontal distribution of ozone in the atmosphere (with a strong concentration in the lower stratosphere, the "ozone layer") a longer slant path means a larger relative absorption by ozone. For SO2 this is much less the case, as SO2 emissions generally show a rather limited distribution horizontally and vertically.

Effectively this means that at higher SZAs the "interference" between the SO2 and O3 absorption results in more negative SO2 slant column values, with large errors. This effect is corrected for by the background correction which is applied to the slant column data.

 

Slant column error

The data files delivered via the website contain the value of the slant column density (SCD) in Dobson Units and an estimate for the retrieval error on the SCD, also in Dobson Units. This error does not take into account any errors in the background correction, the air-mass factor, or other steps in the process: the error just reflects the error due to the DOAS retrieval of the slant column.

 

Slant column retrieval details

In the DOAS retrieval the following trace gases are fitted in the wavelength range 315-326 nm: SO2 and ozone at two temperatures (223 and 243 K). Furthermore two Ring spectra are fitted to correct for the Raman scattering, one to account for the general Ring effect of the Fraunhofer, one for the contribution of ozone (which in fact depends on the solar zenith angle). In addition a correction for polarisation effects and a wavelength calibration using a high-resolution solar spectrum are performed.
 

 


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