It is evident from Table 6.3 and Table 6.3 that both procedures, that of Fabregat and
Torrejon (1998) (hence forth FT) and that of this chapter (hence forth HSP), are
valid at the 3
level. It can also be seen however that the results produced by FT
are overwhelmed by their associated errors, with HSP producing errors smaller
than their associated results but still too large to enable further work. FT also
allows derivation of the intrinsic star flux, whilst HSP relies on the literature for
this.
Both procedures therefore have their merits, with slightly more secure results about the disc coming from HSP, whilst a more overall picture is produced by FT. However it necessary to ask whether Strömgren photometry is a valid approach for observing Be star discs, as it may not be possible to achieve more accurate results due to the excesses being overwhelmed by the continuum. This effect can be plainly seen in Figure 6.2.
This chapter must conclude by stating that unless more accurate methods of separating the circumstellar excess from the continuum can be derived Strömgren photometry of Be stars is not viable. Any method used must be less iterative than that of FT to reduce the compounding of errors, but preferably rely more on the observations in hand, unlike the HSP procedure. Without such methods the advantages of the Strömgren filters outlined in Chapter 6 will remain beyond the grasp of Be stars.