![]() | ![]() |
Astron. Astrophys. 333, 1053-1068 (1998) 2. The observationsThe ASP provides precise Stokes spectro-polarimetry from which it
is possible to extract quantitative measures of the vector field in
the photosphere. This is accomplished through the interpretation of
the full state of polarization (the Stokes vector) in
spectrally resolved line profiles observed simultaneously in Fe
I 630.15 and 630.25 nm: members of the same multiplet which
differ in both Zeeman splitting and overall line strength. A
description of this instrument is given by Elmore et al. (1992);
detailed descriptions of the data and its analysis may be found in
Lites et al. (1993, 1994a), and discussion of the calibration of these
data is presented in Skumanich et al. (1997b). We use a least-squares
(hereafter LSQ) line profile fitting technique, based on the
Rachkovsky analytic solution to the transfer equations of polarized
radiation in a Milne-Eddington model atmosphere, to extract measures
of the vector field from these polarization data, as described in
prior papers for analysis of ASP data cited herein. Using analysis of
both simulated and actual data, Westendorp Plaza et al. (1997) have
demonstrated recently that the LSQ technique provides useful measures
of field strength well below that corresponding to a splitting roughly
equal to a typical Doppler width in the 630.25 nm line
( The data presented herein consist of sequences of spatial maps of
Stokes spectra from which we extract two-dimensional images of
magnetic field and thermodynamic parameters. After each spatial map,
we recorded a sequence of monochromatic images of the spectrograph
slit ("slit-jaw" images) as analyzed by the Universal Birefringent
Filter (UBF - Beckers et al. 1975). The wavelengths and polarization
samples of each image may be selected by the observer. The default set
used here includes on- and off-band Table 1 catalogs observations of the three young bipolar active regions (hereafter Regions 1-3) that are the subject of the present investigation. They are young enough to show active emergence of flux in the form of horizontal magnetic fields between the more vertically oriented leading and following polarities. An examination of the record from Solar Geophysical Data for these three regions reveals that none survived into the following rotation. Their history may be summarized as follows: Table 1. Summary of observational data Region 1: NOAA 7195 (1992 11 June): Our observations of this region are from its first day of appearance, as it was not visible in either magnetograms or white light on previous days. Region 2: NOAA 7551 (1993 July 23): This region first appeared on the limb on 1993 July 18, and was visible on that day in white light, magnetograms, and in Yohkoh X-rays. It grew considerably during the 24 hours preceding the observations reported here. The sunspots of this region were gone by July 26, but the region continued to be visible in magnetograms and Yohkoh X-rays until its passage beyond the west limb. This region is somewhat older than the other two regions presented. We present certain aspects of the the vector field measurements distinguish it from the other two. Region 3: NOAA 7781 (1994 Sept. 22-27): The region is first apparent in Mt. Wilson magnetograms on Sept. 21, one day before the start of our observations. Yohkoh SXT images show some evidence of the region on Sept. 20. We observed the development of this region during six consecutive days. This sequence covers the early stages of formation of a pore which develops over the subsequent days into a small sunspot having a penumbra. We are also able to follow the dissolution of another small sunspot in this region, and to track the history of magnetic flux within the confines of the field-of-view (FOV). ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1998 Online publication: April 28, 1998 ![]() |