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7.10 Fringes in the data

 

In the first data that was obtained with the LWS instrument it became clear that there were fringes in the spectra. During the Performance verification phase the fringing was seen in a number of spectra of different sources. It has been shown that the fringes are strongest in extended sources and in point sources that are observed off-axis. Also sources on a strong background will have strong fringing. The exact cause of the fringing is not yet known. The period of the fringes is constant in wavenumber in all sources at about 3.6 cm tex2html_wrap_inline5251 . The fringe period can be described with an interference formula:

equation1430

where d is the gap that causes the fringes, n is the order of the fringe and tex2html_wrap_inline5221 is the wavelength of the fringes. For two adjacent fringe peaks at wavelengths tex2html_wrap_inline5221 1 and tex2html_wrap_inline5221 2 we get:

equation1434

The gap that was derived from the data taking in PV phase that contained fringes was 1.455 mm. The observers can use this gap to identify the fringes. the amplitude of the fringes depends on the wavelength they are observed at, the extend of the source, the strength of the source and the position of the source in the beam.

Currently a procedure is being written that can correct the data for fringes. This procedure may later be implemented in the ISO Spectrometer Analysis Package (ISAP), see also Chapter refch-post.



N.Trams, ISO Science Operations Team
Using inputs from:
C.Gry, T. Lim, LWS Instrument Dedicated Team
A.Harwood, P.E.Clegg, B.Swinyard, K.King, LWS Instrument Team
S.Lord, S.Unger, IPAC.