![]() | ![]() |
Astron. Astrophys. 336, 925-941 (1998) 4. Reddening and the (
|
![]() | Fig. 6. The composite (H-K,K-L) diagram for variable and non-variable stars in the fields studied. The small points represent the complete set of uncrowded, non-variable objects in all fields, the large open squares are the variable LWHN OH/IR stars, large open triangles are variable Sjouwerman OH/IR stars and large open circles are new variables from Table 3. The short, thick continuous line at the bottom-left represents the unreddened giant branch in Baade's window while the thick dashed line represents the position of red variables in Baade's window. The arrow shows the reddening that would result from 30 mag. of visual extinction. |
It is clear from Fig. 6 that the vast majority of objects seen
in the infrared are highly reddened with
12 to
30 magnitudes. An examination of individual (
)
fields showed that the reddening varied distinctly between fields. A
median E(H-K) was derived for each field as follows.
Firstly, the median H-K of all isolated stars with
14 and H-
0.7 was
computed for each field (stars with H-
0.7 are clearly foreground objects). The extinction was derived from
H-K rather than K-L because of the large
number of stars detected in both H and K. It was then
assumed that the majority of the stars detected in each field were red
giants with intrinsic H-K=0.25. The difference between
the median H-K and 0.25 gave the median
E(H-K) for each field.
The points shown in Fig. 6 were dereddened using the following
procedure. From Fig. 6 we find that in our photometric system
E(K-L) = 0.72 E(H-K). This relation was
used to calculate a median E(K-L) for each field from
the E(H-K) derived above. Then we used the relation
= 2.07 E(K-L) from Rieke &
Lebofsky (1985) to calculate the extinction. The dereddened points are
shown replotted in Fig. 7. The scatter of the non-variable stars
along the reddening vector is now greatly reduced although a residual
scatter in reddening exists due to reddening variations on spatial
scales less than one arcminute.
![]() | Fig. 7. The stars shown in Fig. 6 after dereddening. |
The OH/IR stars are well separated from the non-variable stars in
Fig. 7. The majority of the OH/IR stars discovered by LWHN lie
beyond the sequence occupied by the LPVs in the Baade's Window while
the Sjouwerman sources and the newly-discovered variables mostly lie
near the bulge LPV sequence. Those LWHN variables lying beyond the
bulge sequence presumably have thicker and/or cooler circumstellar
shells than the variables (including IRAS sources) in Baade's window.
However, very red objects similar to the LWHN sources are known to
exist in the direction of the bulge - about a dozen of them were found
by Whitelock et al. (1991) who monitored IRAS sources in a 60
deg2 area of the bulge between
=
to
. Massive, variable
OH/IR stars which are even redder are known to occur along the
Galactic plane (eg. Engels et al. 1983)
A similar separation of the non-variable stars and the variable
stars is seen in the (K, K-L) diagram,
Fig. 8. The non-variable red giant branch occurs in the position
expected for a Baade's window giant branch reddened by
20-25 mag. of visual extinction. Once again, the
large circumstellar reddening and/or cool shells of the OH sources of
LWHN is apparent. The Sjouwerman OH sources and the newly discovered
variables are mostly less extreme in their K-L colours
than the OH/IR stars discovered by LWHN and they bridge the gap
between the non-variable and the OH/IR sequences.
![]() | Fig. 8. The composite (K,K-L) diagram for variable and non-variable stars in the fields studied. The symbols and lines are as in Fig. 6. |
© European Southern Observatory (ESO) 1998
Online publication: July 27, 1998
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