## 4. Analyses## 4.1. 2D singular points in the observed transverse fieldWe take the vector magnetogram observed at 01:44UT on October 27 as an example for determining singular points in the observed transverse field. We make use of Eq. (1) to calculate Poincaré index of singular points from the transverse field. The distributions of computed singular points are shown in Fig. 1, in which figures (a) and (b) are obtained from the raw data, while figures (c) and (d) from the data treated with the lowpass filter technique in the cases, =10 and 5. The singular points with are marked by the symbol, `', and those with are marked by `'. For the raw data, a large number of candidate points are presented, we thus have to tell apart which are real singular points.
To start with, we neglect candidates in the weak-field region, where the average strength of the observed transverse field is lower than 2 (see Fig. 1b). Secondly, we apply the lowpass filter technique to exclude the candidates in the rest, dubiously attributed to the small-scale structures or the noise fluctuation. Thirdly, we confirm the final ones by the 2D field-line pattern, which are traced from the directions of the filtered observed transverse field. Fig. 1c shows that all singular points are well correlated with special field-line patterns; those with correspond to convergence patterns, while those with saddle patterns. In this way, we then obtain the distributions of 2D singular points in the observed transverse fields, taken at 01:44UT and 04:12UT on Oct. 27 (Fig. 2). For both cases, there are six nodes (C1, C2, , and C6) and three saddles (P1, P2, and P3), which are linked by the magnetic lanes demarcating different 2D cells. All cells can be divided into two classes, L and H, based on the difference in the 2D magnetic connectivity patterns. For L cells 2D field lines connect two nodes located in opposite polarity regions, while for H cells 2D field lines converge at a node. This classification will be explained in Sect. 4.3.
## 4.2. Comparison with the inferred linear force-free fieldsIn the previous studies (Wang & Wang 1996; Wang 1997), 2D singular points and magnetic lanes are computed from extrapolated transverse fields based on a specific model such as potential or force-free field model. In this section, we compare these 2D singular features in the computed field with those in the observed field. Using the Fourier Transform Method on a linear force-free field
model (Nakagawa & Raadu 1972; Alissandrakis 1981), we compute
transverse fields in the photospheric plane for four cases,
=0, 0.03, 0.06, and 0.09 in units of
0.69Mm Fig. 3 shows that the 2D topology of the computed field, compared with that of the observed field, is distinctly different. For example, in the observed field, the saddle P3 separates the emerging pole C3 from the main pole C2, while in the computed field P3 disappears, which results in the cells L2 and L3 merging into one cell, L23. In 2D magnetic connectivity patterns, the nodes C1, C4 and C6 are linked to the node C3 in the observed field, while those are linked to the node C2 in the computed field for the cases =0 and 0.03.
We can evaluate the force-free factor, , for the field in 2D cells, from comparisons with 2D magnetic connectivity patterns of the computed fields. The cells H1 and H2 in the main bipole are almost potential (=0). The cells H3, H5 and L4 are of 00.03. Specially, the cells L1, L2, L3 and H4, associated with the drasticly emerging flux, indicate much strong shear (0.09). The 2D topology of the observed field bears more characters than those the constant- field can interpret, which is related to the evolution of magnetic fluxes with different origins. So this offers more chances approaching the real singular structures favorable to the energy release in the flares. ## 4.3. The 3D modeling fieldSince field lines close to a separator or separatrix, which initially close to one another, separate widely in a distance (Démoulin et al. 1996), we can locate intersections of separatrices by tracing these field lines. Fig. 4 shows the connectivity patterns of 3D field lines in the computed fields in the cases, =0 and =0.06. Some special field lines, highlighted in thick solid style, are seen discontinuous at the saddles where they are separated widely. We suppose that the loci of their starting points, portrayed by the dashed lines, represent the intersections of separatrices in the photosphere. For both cases, these intersections are in good agreement with portions of the 2D magnetic lanes in the places close to the saddles. In some places, however, such as region A, they are shown divergent. Fig. 5 shows a side view of these special 3D field lines. The `cavity' structures around the saddles suggest the associated nulls beneath the photosphere.
Since the magnetic connectivities involved in the lanes separating L cell from H cell show no discontinuity (Fig. 4), these lanes do not seem related to separatrices. Fig. 6, however, shows that such lanes demarcate two kinds of magnetic loops different in height and shape. The low loops are confined only in a L cell, while the high ones have long span between H cells. Table 2 lists height and the average ratio between height and horizontal extension of low and high loops.
Moreover, the alignments of the low loops coincide well with those of transverse field components on the photospheric surface (Fig. 4). This may account for the validity of the way we explore the field topology in the low atmosphere in terms of connectivity patterns of the 2D field lines in the photosphere. ## 4.4. The heating of flaring loopsA 1N/M1.1 flare occurred at 01:44UT on October 27. Based on a comprehensive study of the magnetic configuration from the coordinated observations, Wang et al. (1998) found that the event originated from the interaction between two strongly sheared loops. Fig. 7 shows several flaring loops in SXR are spatially related to the 2D singular features, and all the bright kernels in H are located on the footpoints of these loops. The triggering of this flare was on the top (D) of a small loop, but further energy release took place along the loop, especially at its foot regions of A and B (Wang et al. 1998), which may be involved in the separatrices.
Fig. 8 shows a series of small events associated with these singular structures, providing the additional evidence. At 01:28:13UT and 02:33:27UT, a glowing streak was just lying along segment P1P3 of the magnetic lanes (Figs. 8a and 8c). At 01:44:33UT, 02:53:15UT and 03:12:13UT, the SXR emissions disclose the intermittent interaction of two loops at region A (Figs. 8b, 8d and 8e). In Fig. 8f the asterisk (*) marks the position of bright point A in Fig. 8e, which was identified as the interaction site.
This fact may account for a puzzle in Qiu et al. (1997) who found the mixed thermal and nonthermal features of coronal plasma at region A at the onset of the 1N/M1.1 flare. We conjecture that the nonthermal component came from the depositing of nonthermal electrons produced at region D, while the thermal component due to the local heating by reconnection (Fig. 7a or Fig. 8b). The last example to show the heating of flaring loops involved in the separatrices is illustrated in Fig. 8c. A set of bright loops, commonly connecting an emitting SXR locus (G), are coincided with the magnetic lane (P2P3). The reconnection may contribute to the heating process and injected hot plasma into the field loops. Our results agree with those of Parnell, Priest, and Golub (1994) as they show that X-ray bright loops can be considered as being reconnected magnetic loops, and support the viewpoint that magnetic reconnection represents an elementary heating source in various coronal phenomena (Priest, Parnell, & Martin 1994; Mandrini et al. 1997). © European Southern Observatory (ESO) 1999 Online publication: February 23, 1999 |