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Astron. Astrophys. 363, 279-288 (2000)
6. Conclusions
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There are 3 classes of INBPs
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those that show excess emission and are associated with enhanced IN
magnetic fields 4 Mx cm-2
(these constitute 60% in our study),
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those that show equal excess emission but are associated with
bipoles with flux densities generally
4 Mx cm-2 (these
constitute 25% in our study), and
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those that show weak emission (probably unresolved emission) and
seemingly associated with fields 4
Mx cm-2 which is below the noise level set by us for our
magnetic scans (these constitute 15% in our study). These are probably
the unresolved background fields.
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In particular, this study suggests that cases of magnetic bipole
merging have been discounted in other studies (Nindos & Zirin,
1998; Lites et al., 1999) since these bright points are associated
typically with relatively small (and temporally diminishing) net field
values. When these cases are also included, it is found that the
correlation between bright points and co-located magnetic elements in
the data reported here is as high as 85%.
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Although we have established a spatial correspondence in the
locations of the INBPs and IN magnetic elements, we have not been able
to obtain a correlation between the brightness of the INBPs and the
corresponding IN magnetic elements (if this exists on the sun) because
of the scatter caused by the 3-min. oscillations.
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The results of the present study establish the association of
K2V bright points with magnetic elements
and, so, confirm the findings of Sivaraman & Livingston (1982) and
Nindos & Zirin (1998). The mean field of the IN magnetic elements
associated with the INBPs from our measurements is 7.2
Mx cm-2 above the noise level. Our observations are with
limited spatial resolution as we have averaged the brightness and
magnetic field values over a 2 2
pixel area. If the INBPs and IN magnetic elements are sub-arc-sec
structures in reality then the flux density of the IN elements as per
our measurements could be several hundred Mx cm-2. Such
fields would then become dynamically important since the IN elements
would serve as sites where the 3-minute waves can be excited
(Kalkofen, 1996). Fields of this strength have been measured by Keller
et al. (1994) and Lin (1995). Note that one should normally observe
significantly more IN magnetic elements than INBPs since INBPs, due to
their brightening process (3-minute pulse), could be "dark" at the
time the spectroheliogram is recorded. The apparent lack of IN
magnetic elements is probably due to the averaging process of the
smaller sub-arc-sec unresolved magnetic flux tubes.
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We have identified instances of short fibril (loop) structures
connecting adjacent INBPs from the excellent K spectroheliogram close
to the limb obtained by Bruce Gillespie. This is a direct visual
evidence of the INBPs' association with the IN magnetic elements.
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We are aware that the data we have analysed are not an ideal set of
observations to settle this question - association of INBPs with IN
magnetic elements (or otherwise) indisputably. But this is the best
that can be done with the best facilities that are currently
available. What is needed?
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spectroheliogram time sequence at high cadence (every 5 sec or so)
with a narrow spectral band pass as we have used and under excellent
seeing conditions, and
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magnetic scans with better S/N ratio at high cadence and
simultaneous with the spectroheliograms.
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With these data
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the effect of the 3-min. oscillations can be effectively
eliminated,
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the trajectories of the INBPs and the associated IN magnetic
elements can be monitored to see whether they follow identical
patterns. Zhang et al. (1998a) have done this for many IN magnetic
elements using the BBSO data,
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the oscillation period of the NBPs (low brightness) can be
determined. This would tell us the effect, if any, due to magnetic
field coalescing.
© European Southern Observatory (ESO) 2000
Online publication: December 5, 2000
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