Issue |
A&A
Volume 501, Number 1, July I 2009
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|
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Page(s) | 321 - 333 | |
Section | The Sun | |
DOI | https://doi.org/10.1051/0004-6361:20078664 | |
Published online | 30 October 2008 |
Relationship between the topological skeleton, current concentrations, and 3D magnetic reconnection sites in the solar atmosphere
R. C. Maclean1 - J. Büchner2 - E. R. Priest1
1 - Institute of Mathematics, University of St Andrews, The North Haugh, St Andrews, Fife, Scotland, KY16 9SS, UK
2 - Max-Planck-Institut für Sonnensystemforschung, Max-Planck-Str. 2, 37191 Katlenburg-Lindau, Germany
Received 12 September 2007 / Accepted 26 September 2008
Abstract
Aims. The aim of this work is to determine the relationship between the 3D structure of the coronal magnetic field, diagnosed by the topological skeleton, and current concentrations as potential sites of 3D reconnection.
Methods. We utilised the results of 3D numerical MHD simulations of an observed EUV bright point (BP) in the solar atmosphere. The simulations are based on MDI line-of-sight magnetogram data from 13 June 1998. We analysed the results of the simulations using the method of magnetic charge topology. Three different methods of reducing the magnetogram to a set of point magnetic sources are tested.
Results. Observations of the BP show a rotation of one of its main magnetic source regions. Numerical simulations of this rotational motion result in a localised build-up of parallel electric current, which is dissipated by anomalous resistivity, causing 3D magnetic reconnection and BP heating. The magnetic topological structure of the simulated BP was also calculated, and a portion of the topological separatrix surface bounding the magnetic flux of the rotating source region is found to correspond to the locations of current build-up and heating. All three magnetogram reduction methods produce similar results for the large-scale magnetic field structure.
Conclusions. Magnetic topology is a useful method for predicting the locations of coronal current concentrations, insofar as the results of our simulations show that strong integrated parallel electric fields are found only along topological separatrix surfaces. However, further investigation is necessary to determine exactly which parts of the reconstructed separatrices will host the electric currents. Topological magnetic field reconstructions also cast light on the location of coronal BP heating, which occurs as a result of the dissipation of the currents by 3D reconnection. The choice of the magnetogram reduction algorithm does not greatly affect the large-scale topological features of the resulting reconstructed magnetic field. Further work is required to compare these results with data for other observed BPs.
Key words: Sun: atmosphere - Sun: corona - Sun: magnetic fields - magnetohydrodynamics (MHD) - methods: numerical
1 Introduction
Topological properties of the coronal magnetic field such as separators and separatrices, and geometrical features such as quasi-separatrix layers, are potential sites for magnetic reconnection and heating in the solar atmosphere, because electric currents can easily build up along them (Priest & Titov 1996; Démoulin et al. 1996; Priest & Démoulin 1995; Büchner 2006a; Priest et al. 2005). Coronal currents indicate that excess energy is stored in the magnetic field and, according to present theory, can be released by collisionless dissipation (e.g. Büchner & Daughton 2007; Büchner & Elkina 2006; Shay et al. 1998). Once a certain critical drift velocity of the current carriers is attained collisionless dissipation starts and reconnection becomes possible (e.g. Büchner 2007). Consequences can be a heating of the corona, the acceleration of particles to high energies and the formation of plasma jets (e.g. Yokoyama & Shibata 1996). Different methods have been proposed to model the geometrical and topological features associated with the formation of current concentrations. This includes the concept of quasi-separatrix layers (QSLs) (Titov et al. 2002; Titov 1999) as well as the magnetic charge topology (MCT) method (Brown & Priest 1999; Longcope 1996).
Coronal bright points (BPs) were first observed by Vaiana et al. (1970). They
appeared to be closely related to bipolar magnetic features
(e.g. Golub et al. 1977). This lead to the development of
reconnection scenarios of bright point heating, first in two dimensions
(e.g. Priest et al. 1994).
Later three-dimensional reconnection models were suggested. In order to
verify 3D reconnection near BPs it is appropriate to analyse BP related
magnetic fields using appropriate analysis methods of the field geometry and
topology. Here we apply the MCT method to the case of a coronal bright point
which was simulated by Büchner et al. (2004) based on observations by
Brown et al. (2001). SoHO/MDI and TRACE both observed a bright point
from its birth around 20:00 UT on 13 June 1998 until its disappearance
around 16:00 UT the next day. These observations were
used as a starting point for 3D numerical MHD simulations of the plasma and
magnetic field in the solar atmosphere. The observed rotation
of one of the magnetic sources (the main negative polarity rotated radians clockwise over the course of 2 h from 09:41 UT) was applied as
a boundary condition and compared to the results of the simulated
consequences of rotating the other main source region. The results of the
simulation give valuable clues about which parts of the magnetic field are
most important in determining the behaviour and evolution of the bright
point.
In modelling the coronal potential magnetic field caused by an observed normal magnetic field at the photosphere, a choice of approaches is available. First, one could regard the photospheric field as continuous (the QSL method). With the magnetic field values at every point on a spatial grid one could then obtain both the skeleton (of separatrices) and a quasi-skeleton (of quasi-separatrix layers), which is quite difficult to do to high accuracy. Or, one could approximate the photospheric field by a series of point sources (the MCT method). In such approach the quasi-nulls (regions of weak magnetic fields) and quasi-separatrices of the QSL approach become exact nulls and separatrices. The strengths and weaknesses of both approaches were discussed by (Démoulin et al. 1996) and the choice of method will depend on the aim and purpose of the modelling effort, as well as what type of feature is being modelled.
In fact, the QSL method was developed in response to a limitation of the MCT method (for details, see Démoulin et al. 1996). In an MCT field reconstruction, there will exist about the same number of photospheric null points as the number of point sources. This is an artefact of the model and does not mean that all these photospheric nulls will exist in the real field; in fact it is highly unlikely that a real null would be sitting exactly in the photospheric plane. Fields constructed using the QSL method replace these photospheric nulls and their separatrix surfaces (across which the fieldline connectivity is discontinous) with quasi-separatrix layers. These are thin layers in which the fieldline connectivity gradient is very steep but not discontinuous. This is likely to be a more accurate representation of the real magnetic field on the Sun. In fact, in the real coronal magnetic field, it is likely that both QSLs and true separatrix surfaces exist together. Some true magnetic null points might still exist in the solar atmosphere high above the photosphere, and each of these nulls is associated with a true separatrix surface. For these reasons, the QSL method is often the better choice.
However, reconnection and heating may occur both at sites of enhanced current concentrations for which separators and separatrices are indicative as well as quasi-separators and quasi-separatrices. The main aim of this work is to determine to which degree enhanced current concentrations are related to the separatrix positions as they can be obtained by the MCT method which is simpler, even though it produces some spurious nulls. Furthermore, it is often the case that the main magnetic flux in the photosphere is given in the form of discrete fragments (each made up of several MDI pixels but separated by tens of pixels). In this case the MCT method is very much appropriate. Of course, the sources could be given also with finite size, but, again for simplicity, we choose to adopt a point-source model.
The paper is structured as follows. In Sect. 2 we describe the methods used for the numerical simulation and give an overview of the technique of magnetic topology and the assumptions we have used to construct the topological models. Section 3 contains a topological analysis of the initial magnetic structure of the bright point region. The main results are in Sect. 4 where we look at the topological consequences of rotating the main magnetic source regions of the bright point, and how that matches up with the observed locations of brightenings in the corona. Then in Sect. 5 we deal with the question of the robustness of the topological model we are using and how it is affected by the level of accuracy chosen. Finally in Sect. 7 we present and discuss our conclusions.
2 Modelling techniques
2.1 Numerical simulations
A 3D numerical MHD code was used to simulate the plasma in the photosphere,
chromosphere, transition region, and corona. A full description of the code
can be found in Büchner et al. (2005); here we give a short overview of its
essential features. The numerical simulation approach consists of three
parts. First, the observed longitudinal (line-of-sight) photospheric
magnetic field component is used to obtain an initial three-dimensional
force-free magnetic field configuration. An appropriate extrapolation method,
compatible with the requirements of the boundary conditions of MHD simulation
boxes, is described in Otto et al. (2007). The essence of this method is
that at the boundaries the horizontal components (Bx and By) are related to the vertical component Bz through fulfilling the
force free condition (3), and at the same time, fulfilling
.
For this sake a periodicity in the horizontal
(X and Y) directions is assumed to obtain a solution in a
non-periodic region which is a quarter of a fully periodic one. For a
solution in the domain
,
the
fully periodic region would be
,
.
Within the latter the total magnetic flux is balanced to a
high degree. Since the solution of MHD equations, however, requires a locally
symmetric boundary condition for the current as well as for the plasma
density which should not create an artificial discontinuity in the
field-aligned current flows. To meet this condition we use instead a Green's
function approach which satisfies line-symmetric boundary conditions. Using
this extrapolation technique the simulation model is initialised with a
Fourier-filtered photospheric magnetic field, based on MDI observations of the
longitudinal components of the solar magnetic field. The filtering is applied
since the numerically stable solution of the partial differential MHD
equations requires a sufficient resolution of magnetic field gradients by the
finite grid distances (about 8-16 grid points resolving the shortest
wavelength of the spatial Fourier modes). Without additional information
about the photospheric currents or vector magnetic fields, we assume in the
beginning, at t=0,
i.e. we start with a potential field
extrapolation.
Because the plasma-
is small throughout the chromosphere and corona,
the physics of the solar atmosphere is determined by the magnetic field and
not by the plasma pressure. Hence, we can just ``fill'' the extrapolated
magnetic field configuration with plasma. We choose to start with an initial
density and temperature stratified with height following the equilibrium VAL model of Vernazza et al. (1981) in its version ``C''. Deviating from VAL we
assume, however, somewhat smaller values for the plasma density in the lower
chromosphere, limiting it to 100 times the coronal density. This is done
partly for numerical reasons because larger densities correspond to larger
collision frequencies which would require significantly smaller simulation
time steps than desirable for large scale three-dimensional simulations. This
limitation of the density is justified since we do not draw special attention
to the processes in the lower chromosphere, we just want to ensure a
sufficiently strong coupling between the neutral gas and plasma. Further, in
order to resolve the transition region well (by at least ten grid points, see
Sect. 2.1), we enhanced the width of the transition region
artificially to about 1500 km. For the side boundaries of the simulation box,
we assume the same line symmetry across the X and
Y boundaries for plasma density and the density of a neutral gas
component, which we also take into account, as well as for the velocities and
currents. At the lower (photospheric) boundary the tangential velocity is
defined by strongly coupled plasma and neutral gas motion, and the boundary
normal velocity is set to zero (no emerging or submerging flux). The normal
magnetic field uses
and the horizontal
components are computed from
.
Density and pressure are assumed symmetric (zero normal derivative). At
the top (coronal) boundary symmetric conditions (zero normal derivatives) are
assumed. Based on the changes of the photospheric magnetic field, a
consistent horizontal velocity profile is imposed as a boundary condition at
the simulation. In order to avoid plasma emergence and submergence we apply a
vortex motion satisfying
,
where un is
the neutral gas velocity. This way the density is conserved. It is contained
in the X, Y directions so it can be expressed as a potential
function U with
.
The
motion is imposed for the neutral gas throughout the whole simulation box.
However only in the chromosphere, where the collision frequency is
sufficiently large, it effectively couples to the plasma.
We solve the following set of MHD equations:
In Eqs. (1)-(4) the subscript e denotes the equilibrium variables. In the energy Eq. (4) the pressure p is substituted by the internal energy



We solve the partial differential MHD Eqs. (1)-(4) by means of a finite difference
approximation. We apply a Leapfrog scheme which is second order in accuracy
and very low in numerical dissipation. As usual in schemes, based on the
Flux-Corrected Transport (FCT) paradigm, un-physical oscillations are damped
on the grid scale. Second order derivatives are treated with a Dufort-Frankel
scheme allowing the consideration of small resistivities. We choose a
non-uniform grid to meet the requirement of a high plasma-
(higher
plasma/gas pressure than magnetic pressure) at the lower boundary
reaching the much lower-
corona via the low-
chromosphere. We
also choose a non-uniform grid to be able to spatially resolve the
chromosphere and the steep gradients in the transition region well enough.
Our grid has 49 points in the vertical direction (Z), and 131 points in
each of the horizontal (periodic) X and Y directions.
The code was verified, e.g., by investigating the bulk plasma acceleration due to perpendicular electric fields based on Soho observations on October 17, 1996 (Büchner et al. 2005) and in preparation of the Hinode data analysis (Büchner 2007).
2.2 Overview of magnetic topology
Studying the magnetic topology of a magnetic field is an excellent way to
extract vital information about the shape and connectivity of that field,
reducing it to only its essential structural features. For this work, we
decided for simplicity to reduce the magnetograms to point magnetic sources
and use potential magnetic fields. Each point magnetic source represents a
concentration of positive or negative flux in the magnetogram. The integrated
flux corresponds to the strength of the point source, which is located at the
centre of mass of the flux concentration; flux concentrations with a peak
value below
are neglected. Brown & Priest (2000)
showed that potential fields are a good approximation to the real coronal
field in cases where the nonlinearity in the field is not too severe and
hence the current remains relatively low, which holds in quiet Sun regions
like the one we study here. Although the exact shape (geometry) of the real
field may differ from our results, the important topological features will be
the same.
The analysis begins by finding the locations of the magnetic null
points of the field, where
.
These can be either in the
photosphere (on the base of our 3D simulation box) or in the corona (within
the 3D volume). Figure 1 shows the structure of the magnetic
fieldlines near a first-order generic potential null point, i.e. the
type of null found in the current scenario. The structure can be found by
linearising the expression for
near the null and using the three
eigenvalue-eigenvector pairs to give starting points for extrapolation of
the spine and fan fieldlines (Parnell et al. 1996). A
null is called positive if its fan fieldlines are directed outwards
and negative otherwise. For a null in the photosphere, it is called
prone if its spine fieldline lies in the photosphere and
upright otherwise.
![]() |
Figure 1: Structure of a first-order generic potential magnetic null point. |
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When many magnetic sources are present, the number of nulls in a topology
will also be large. The exact number is governed by two Euler characteristic
equations. In the photosphere,
where S is the number of magnetic sources,


where S+/- is the number of positive/negative magnetic sources and n+/- is the number of positive/negative nulls. Note that for these equations to hold, the total flux from the sources must be in balance; this condition is generally fulfilled by the addition of a ``balancing'' source at infinity. These equations provide a useful check that all nulls in the topology are likely to have been detected.
Extrapolation of all the spine and fan fieldlines is the next step in the topological analysis. The fieldlines of the fans extend out to form curved surfaces called separatrix surfaces. Where two such separatrices intersect, a separator fieldline is formed, which joins the two null points. Both separatrices and separators define the boundaries between regions of different magnetic connectivity in the topology. This makes them prime locations for magnetic reconnection to take place (Priest et al. 2005). In Sects. 3 and 4, we construct the initial magnetic topology of the bright point region just as described here, and use our assumptions about the motion of the sources to predict on which separatrix surfaces signatures of reconnection should be observed.
2.3 Assumptions in the topological models
Before this topological modelling can commence, the magnetogram must be reduced to a set of point magnetic sources. In this bright point investigation, we experiment with three different methods of producing the set of sources from a magnetogram. Section 5 describes how analysis of the results of all three methods can determine to what extent the calculated topology is affected by the method of picking point sources. Here, we simply explain the actual methods used.
![]() |
Figure 2:
Initial photospheric magnetic field. Above: raw MDI
magnetogram, with greyscale shading indicating magnetic field strengths
between |
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Two of the methods involve Fourier filtering. The magnetogram data is
Fourier-filtered to either 8th or 16th order. This means that only
lower-order terms are included, so only magnetic field sources that are
spatially relatively large are detected, automatically getting rid of the
small-scale fluctuations. This technique picks out the regions of strongest
``signal'', i.e. strongest line-of-sight magnetic flux, and each region
is represented by a point source, with strength proportional to the magnetic
flux of the region. 16th-order Fourier filtering is more accurate and so
picks out many more source regions than the 8th-order method does.
Any source with strength less than
is neglected. This
threshold value may seem high compared to a typical noise level for the MDI
instrument. However, the choice of threshold is always a compromise between
values so high that only a handful of source regions are identified and
important information about the magnetic field configuration is lost, and
values so low that you are down in the noise and the selected ``source
regions'' become meaningless. In this case, the choice of
was made in order to select a reasonable number of the strongest magnetic
features visible in the vicinity of the bright point.
In the third alternative method, the raw magnetogram data is smoothed to get
rid of small-scale numerical fluctuations which would introduce tiny spurious
sources. Each point magnetic source represents a concentration of positive or
negative flux in the smoothed magnetogram. The integrated flux corresponds to
the strength of the point source, which is located at the centre of mass of
the flux concentration; again, flux concentrations with a peak value below
are neglected.
3 Magnetic structure of the bright point region
Figure 2 shows an MDI magnetogram taken just before the rotation
phase of the negative source begins. The bright point itself is located in
the corona directly above the two central sources. Some extrapolated
potential magnetic fieldlines are shown, which highlight part of the
structure of the field. The scale on the axes is in units of 500 km, so
that the total box size is
Mm or
.
This
scaling is used throughout the paper.
Topological analysis (using the 8th-order Fourier-filtering method) reduces this complex photospheric field to fifteen point magnetic charges, five of which are positive and ten negative. This number of sources is not imposed as part of the model, but is a natural result of the choice of threshold magnetic field value for defining the source regions. Due to the imbalance in the total magnetic flux, we also insert a compensating negative source at infinity. This is a standard and integral part of the MCT model, as flux balance is required for the divergence of the magnetic field to be zero. The source is added at infinity, rather than at some finite distance away from the other sources, to minimise its influence on the topology and avoid bias. The two magnetic sources that represent the BP bipole are the strongest sources in the chosen region, but not by orders of magnitude; all the magnetic charges in the topology are strong enough to be important for the topological structure in some way or another. The BP sources do not dictate the whole magnetic structure of the region. Although they are dominant in the centre of the simulation box, towards the edges of the box the other sources dominate the magnetic field structure.
Fifteen null points are found in this configuration; nine positive and six negative. One of the positive nulls is in the corona and all the other nulls are prone, sitting on the photospheric boundary. Note that the Euler Eqs. (5) and (6) are satisfied since the coronal null has a ``mirror image'' below the photosphere which is not physically meaningful but must be included in the equations. Extrapolation of the spine and fan fieldlines shows that eighteen separators are present. The photospheric footprint of the topology is shown in Fig. 3.
4 Simulation of magnetic reconnection
4.1 Observed motion: the main negative source rotates
The photospheric magnetograms of the bright point region show the main
negative source (S1) rotating about
radians clockwise over the
course of 2 h from 09:41 UT. In this section we look at the effects of
the magnetic reconnection caused by this rotation, and how they are reflected
in the magnetic topology of the region.
Figure 4 is a contour plot of the parallel electric field integrated along the magnetic field, 90 min after the start of the MHD simulation of the main negative source rotating (Büchner et al. 2004). The parallel electric fields are due to enhanced currents flowing parallel to the magnetic field that exceeded the threshold of anomalous resistivity (Büchner & Elkina 2005; Büchner & Daughton 2007).
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Figure 3: Photospheric footprint (only photospheric fieldlines shown for photospheric nulls) of the initial magnetic field from Fig. 2. The source locations and strengths were determined using the 8th-order Fourier-filtering method. Positive (negative) sources are red (blue) circles. Positive (negative) null points are red (blue) triangles. Spine fieldlines are green and separatrix fieldlines are purple. The main negative and positive sources of the bright point are labelled S1 and S2 respectively, and the three important nulls are labelled N1, N2 (photospheric), and C (coronal). Fieldlines in the topological skeleton that mark the photospheric boundaries of the BP's magnetic flux are highlighted: for S1 in orange and for S2 in pink. |
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![]() |
Figure 4:
Contour plot of parallel electric field (
|
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Strong concentrations of parallel electric field exist in the simulation box
along fieldlines that connect to the photospheric surface at locations
corresponding to both the positive and negative main sources. There is also a
curve of high values of integrated
extending down
and right from the positive source before it twists back around to the left,
along the southern edge of the base of the simulation box.
In fact, the position of this curve corresponds very well to the position of an important separatrix surface in the magnetic topology, as shown in Fig. 5. The negative null N1 has a separatrix surface associated with it. This 3D separatrix forms a dome structure which covers the rotating negative source and encloses all of its flux. The dome is bounded in the photosphere by its own separatrix traces, and more importantly, by the linked spines of several positive nulls (highlighted in orange in Fig. 3).
It has not yet been fully explained why only some sections of the
photospheric trace ``light up'' in
integrated along the magnetic fieldlines, but a possible
theory is that, as most of the magnetic flux from the main negative source
connects to the main positive source, most of the stress is felt along these
fieldlines. As the clockwise rotation proceeds, some of these fieldlines are
forced to reconnect and are pulled out along the separatrix boundary, still
highly stressed and associated with large values of integrated
.
In Sect. 5.4 and Fig. 19 we show and
discuss the calculated quasi-separatrix layers of the magnetic field from the
numerical simulation. It seems that the sections of the topological
separatrix surfaces along which QSLs are detected are close to being the same
sections along which the high values of integrated
show up. Therefore it may be that high values of
integrated along the magnetic fieldlines
are associated with strong gradients
in fieldline connectivity. This makes sense because we would expect magnetic
reconnection to be occurring in just such regions. The QSL model may
therefore have more to say than the MCT model about exact locations of
reconnection and heating within a (quasi-)separatrix surface. An interesting
follow-up, which is outside the scope of the present work, would be to
investigate the exact correlation between the location of the QSLs and the
location of the regions of high integrated
.
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Figure 5:
The photospheric footprint (based on 8th-order Fourier-filtered
sources) of the separatrix dome that covers the rotating negative source
(S1), and how it compares with the contour plot of
|
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Figure 6 shows a 3D view of the separatrix dome. As
you can see, the line of spines along which it connects to the photosphere is
in the same position as the region of high integrated
.
This means that the rotation of the source is causing reconnection and heating
along the separatrix surface which encloses it. Although this line of spines
will not exist in precisely this form in the real coronal field, and most of
the photospheric nulls are spurious, this model still has meaning. The rotation
of the negative source will cause fieldlines to reconnect from the main
positive source along the boundary where the connectivity changes to each
positive source in the line of spines in turn. The magnetogram does not show a
line of isolated point sources, but one long continuous source region of
positive flux - so in the real field the reconnection and change of
connectivity will be continuous rather than discrete, but the model
still shows that this is the separatrix surface where the reconnection will take
place (although it cannot predict exactly where on the surface the current will
be localised).
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Figure 6:
3D view of the separatrix dome covering the rotating negative
source, with sources calculated using the 8th-order Fourier-filtering
technique. To improve ease of visualisation, all spines are shown but only
separatrix fieldlines in the separatrix surface under discussion are also
displayed. The dome is bounded in the photosphere by the set of green spine
fieldlines whose location corresponds to the region of high
|
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Figure 7:
|
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4.2 Model assumption: the main positive source rotates
In this section we look at the effect of rotating the main positive source
(S2) instead of the negative one (S1). Figure 7 shows the
integrated parallel electric field that results, 90 min
into the simulation. There are similarities and differences when this result
is compared to the previously discussed simulation of the negative source
rotating. In both, there are strong buildups of integrated
at the sites of the two main sources themselves.
However, there are two new regions of high integrated
in this simulation; one reaching
diagonally up and left away from the negative source, and one horizontal
strip above and to the right of the positive source. Interestingly, the
region from the previous simulation that stretches away from the positive
source below and to the right of it still exists in this simulation, although
it is the weakest region detected.
In the previous simulation, the rotating negative source is covered by one
separatrix dome whose photospheric traces surround the source. However, the
positive source considered here requires not one but two separatrix surfaces
to completely surround it. This seems strange at first, but essentially the
point-source model is just a simple way to find out where the changes in
fieldline connectivity are. It doesn't matter how many separatrix traces it
takes to surround the rotating source in the photosphere, what matters is
that it should be these separatrices and no others that show the signature of
reconnection (in terms of heightened values of
integrated along the magnetic fieldlines). Anyway, in this model, one of the
separatrices is associated with the positive coronal null point C. This
separatrix touches the photosphere all the way along the line of spines of
negative nulls running approximately from left to right across the upper part
of the footprint (highlighted in pink on the photospheric footprint,
Fig. 3). The other important separatrix is that
associated with the positive prone photospheric null N2. This separatrix
touches the photosphere first along its own purple separatrix traces and then
along the connecting spines directly out to the edge of the diagram. The
photospheric footprint of these two separatrices is given in
Fig. 8, which also shows the contour plot of
integrated along the magnetic fieldlines
for comparison.
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Figure 8:
The photospheric footprint (based on 8th-order Fourier-filtered sources) of the separatrix surfaces that surround the rotating positive
source, and how it compares with the contour plot of
|
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In fact, the figure confirms that the two regions of high integrated
above the sources lie along parts of the two
separatrix surfaces that surround the positive source. The region above and
to the left of the negative source lies along part of one of the spines that
bounds both of the separatrix surfaces in the photosphere. The region above
and to the right of the positive source follows almost exactly part of the
spine lines of a negative null lying in the footprint of the coronal null's
separatrix. A 3D view of these separatrices is shown in
Fig. 9.
![]() |
Figure 9: 3D view of the separatrix surfaces surrounding the rotating positive source, with sources calculated using the 8th-order Fourier-filtering technique. |
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It is interesting that rotation of the positive source also causes a small
buildup of integrated
along the
separatrix surface associated
with the negative source. This may be due to the fact that the negative null
where this separatrix originates is connected by separators to both the
positive nulls whose separatrices surround the positive source. Thus, the
surfaces are linked and shear applied to one may have a knock-on effect on
the others. However, this does not explain why no similar effect was observed
in the first simulation. Maybe it existed but was too weak to pick up in the
analysis, or maybe it is determined by the detailed geometry of the magnetic
field. Another obvious question is what the 3D distribution of
looks like; the current work only deals with
integrated along fieldlines, so it shows which
fieldlines are reconnecting, but not at which point along the fieldline the
reconnection actually occurs. We hope to do more work towards resolving these
issues in the future.
5 Robustness of topological model
The details of the magnetic topology that we have been using in this study so far depend on the technique that was chosen to extract the set of point magnetic sources from the magnetogram data. Therefore in this section we consider which features of the topology are robust to changes in the source-calculation technique. To do this, we recalculate the topology under two new sets of assumptions - the smoothed magnetic field and 16th-order Fourier-filtering techniques detailed in Sect. 2.3 - and look for similarities and differences in the results.
5.1 Smoothed magnetic field sources
Figure 10 shows the magnetic footprint of the topology based on smoothed magnetic field sources. This technique for selecting sources produces roughly the same number as before; 21 plus the balancing source at infinity, compared with 15 plus one from 8th-order Fourier-filtering. Of these, there are 14 positive sources and 8 negative, including the source at infinity. The distribution of the sources inside the simulation box is broadly similar to that found for 8th-order Fourier-filtered sources. There is a band of positive sources at the top of the box, connected via a line of spines to another concentration of positive sources at the bottom of the box. The negative sources lie more centrally, positioned to both left and right of the previously mentioned line of spines. However, there are a few significant differences. For example, the smoothed magnetic field method places the upper positive sources further to the left, but fails to detect the positive sources found on the lower left of the Fourier-filtered footprint.
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Figure 10: Photospheric footprint for smoothed magnetic field sources. |
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The new topology contains 13 positive and 7 negative magnetic null points, all of which are prone and photospheric (thus fulfilling the Euler Eqs. (5) and (6)). This contrasts with the previous topology which contains a positive coronal null. It seems that this null still exists in the new topology but has found its way into the photosphere, where it lies at (31, 51) and is labelled N3 on the footprint (Fig. 10). It is clear that this is indeed the same null point in both source approximations when you see that its separatrix still forms the same part of the boundary around the main positive source. We will return to this issue later; for now we consider how well this new topology matches the simulation of the negative source rotating.
The separatrix surface of the negative null N1 forms a dome which covers the
negative source. It touches the photosphere along its own separatrix traces,
one of which leaves the diagram along its lefthand edge. On the other side,
the dome continues along the green spine line that runs right through the
main positive source and continues diagonally down and right until it
encounters the other separatrix trace re-entering the diagram from the lower
edge. Figure 11 shows this photospheric boundary of the
separatrix dome superimposed on the contour plot of
integrated along the magnetic fieldlines, to allow
easy comparison between the two. 3D views of the dome are given in
Fig. 12.
![]() |
Figure 11:
The photospheric footprint (based on smoothed magnetic field
sources) of the separatrix dome that covers the rotating negative source, and
how it compares with the contour plot of
|
Open with DEXTER |
![]() |
Figure 12: 3D view of the separatrix dome covering the rotating negative source, with sources calculated using the smoothed magnetic field technique. |
Open with DEXTER |
Allowing for the relatively small number of sources in this model and the
limitations of using potential fields, there is a good correspondence between
the region of high
integrated along the magnetic
fieldlines and the position of parts of the separatrix surface. The separatrix
leaves the main positive source at exactly the right angle to coincide with the
contours of integrated
,
and turns downwards as they do.
Because the smoothed magnetic field approximation fails to pick up some of the
positive sources in the lower lefthand corner, there is nothing ``pulling'' the
separatrix towards this corner and so it leaves the diagram at a rather
steeper angle than the region of high integrated
does. Nevertheless, the features of the contour plot
are well-explained by current building up along parts of this separatrix dome.
Notice also that the negative null producing the dome lies in almost the same
position under both source approximations studied so far.
Let's now turn to the equivalent question for the simulation of the main
positive source rotating. As in the previous experiment, the positive source
is surrounded in the photosphere by the traces of two separatrix surfaces.
The null points concerned, N2 and N3, are both positive, prone, and
photospheric. Figure 13 is the usual
superposition of these separatrices onto the contour plot of
integrated along the magnetic
fieldlines, for rotation of the positive source.
![]() |
Figure 13:
The photospheric footprint (based on smoothed magnetic field sources) of the separatrix surfaces that surround the rotating positive
source, and how it compares with the contour plot of
|
Open with DEXTER |
![]() |
Figure 14: 3D view of the separatrix surfaces surrounding the rotating positive source, with sources calculated using the smoothed magnetic field technique. |
Open with DEXTER |
In the photosphere, each of the two separatrix surfaces in question follows
what is in fact the only possible path for it; along its own separatrix
traces and then out to each edge of the diagram along the spine lines of the
negative nulls. Figure 14 shows 3D views of
these surfaces in the corona. Again, allowing for the small number of sources
and the inaccuracies of potential field modelling, the regions of high
integrated
are well-aligned with parts of the
separatrix surfaces. In particular, there is an excellent correspondence
between parts of the spines leaving the main negative source (which carries
the separatrix of the lower positive null) and the region of high integrated
also connected to the negative source. The region on
the top right of the diagram is not so obviously well-correlated with any part
of the separatrix surface, but does seem to follow part of the spine of another
close-lying negative null. The reason for this may be that the region is close
to the edge of the simulation box. The magnetogram shows a large active region
directly north of the BP and about
away from it. This AR
is not accounted for in the model, but its magnetic influence at that edge of
the box could force the separatrix of N3 to undergo a bifurcation and lie along
the alternative spine path.
5.2 16th-order Fourier-filtered sources
The last source approximation that we test here is 16th-order Fourier filtering, as described in Sect. 2.3. 47 sources and 46 null points exist in this topology, which can be seen in Fig. 15. 24 of the sources are positive, and 22 are negative, including the balancing source at infinity. Of the nulls, 24 are positive, and 22 are negative, including one coronal null. These numbers satisfy the Euler Eqs. (5) and (6). With this much larger number of sources than the other two models, this topology looks complicated and crowded at first sight. However, we shall soon find that it contains many familiar features.
![]() |
Figure 15: Photospheric footprint for 16th-order Fourier-filtered sources. |
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The null point N1 whose separatrix covers the rotating negative source can
still be picked out. Figure 16 shows the photospheric
trace of this separatrix in comparison with the contour plot of
integrated along the magnetic
fieldlines. It follows the line of spines that encloses the main negative
source. Clearly, the higher number of sources present in this model leads to
a greater accuracy in predicting the locations of high integrated
regions found by simulation, as the separatrix
sits almost directly over them and in fact the two lines touch and cross
several times.
![]() |
Figure 16:
The photospheric footprint (based on 16th-order Fourier-filtered
sources) of the separatrix dome that covers the rotating negative source, and
how it compares with the contour plot of
|
Open with DEXTER |
It was not possible to produce 3D separatrix surface plots for this topology as the null point has such strong eigenvectors in the photospheric plane that coronal fieldlines could not be plotted. However, the structure of the topology requires the separatrix to take the path described above. This is purely an effect of the way in which fieldlines in the separatrix surface are found at present and does not in any way reduce the validity of the findings above. Separatrix surfaces are found by starting fieldlines very close to the null in its fan plane. These fieldlines are usually evenly spaced. However in this case, all the fieldlines show such a strong tendency to close down to the nearest sources that it was impossible to find any that did not, down to the limit of numerical accuracy. This does not mean there is no separatrix though. The separatrix acts as a marker for a change in fieldline connectivity, and this change is still there, just as distinctly as in any other case studied here. Our current methods simply prevent us from detecting any of the fieldlines that mark out this change in this particular case.
For the case of the positive source rotating, as ever, two separatrix
surfaces together surround the positive source. These are the separatrices of
the positive prone nulls N2 and N3, as shown in
Fig. 17, where the positions of the separatrices
are compared to the relevant contour plot of integrated
.
In this topology, there is an interesting
difference to the other two models. Instead of both separatrices extending
out to infinity, each one forms part of a finite dome that actually covers
the rotating positive source. The two separatrices meet along the spine line
of the negative coronal null point C. So clearly the two positive nulls can
be said to be the ``same'' nulls that were found in the other two models, but
the topological shape of their separatrix surfaces (although still fulfilling
the same function) has changed.
![]() |
Figure 17:
The photospheric footprint (based on 16th-order Fourier-filtered sources) of the separatrix surfaces that together cover the rotating positive
source, and how it compares with the contour plot of
|
Open with DEXTER |
![]() |
Figure 18: Positions of main nulls in the magnetic field from the MHD simulation. The areas containing the main sources are large green circles and the areas containing the main nulls are large red circles. We have superimposed red and blue triangles showing the locations of the critical nulls from the three topological reconstructions of the region. |
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Comparing the separatrices with the regions of high integrated
,
again the region stretching diagonally up and left
from the main negative source is associated with the spine fieldline
extending in the same direction that carries the separatrix surface of N3.
Although they are not exactly aligned, within the limitations of the model
they are undoubtedly related. Concerning the other region, above and to the
right of the main positive source, there is the same slight issue as for the
smoothed magnetic field model, in that the region seems to follow the wrong
spine. Again, we postulate that this may be due to the strong
positive active region source which exists in the real solar magnetic
configuration but lies outside the simulation box, which could force the
separatrix down onto the other spine.
5.3 Comparison with main nulls in magnetic field from MHD simulation
The locations of the critical null points associated with the separatrices
surrounding the rotating sources are further confirmed by another piece of
analysis of the bright point region. Figure 18 shows the
approximate positions of the three main nulls found in the magnetic field
produced by the MHD simulation discussed in Sect. 2.1, by
searching for regions of minimum field where
is close to
zero. This technique uses the whole 3D field to work out where null points
are likely to be found, although it does not give their exact positions. We
have superimposed on the plot the positions of the three magnetic nulls (N1,
N2, and N3/C) whose separatrices cover the rotating sources, from all three
of our topological reconstructions of the bright point region.
It can be seen from Fig. 18 that five of the nine
nulls from the topological reconstructions overlap with the regions of low
.
The remaining four do not show quite such a good
correspondence but there is a definite trend towards their being located near
the null point regions. This provides a useful confirmation that the nulls
selected as being topologically important in the analysis performed in
previous sections are likely to be the main null points of the region, and
that their locations can be identified by an alternative technique.
5.4 Comparison with calculated locations of QSLs from MHD simulation
The positions of the separatrices are also important as it is at certain locations along these surfaces that strong currents are generated so that as a result of plasma instabilities that cause anomalous resistivity, reconnection can take place (Büchner 2006b). All the separatrices in the topological reconstructions are calculated for the case of a potential field, so it is useful to know how the positions of these separatrices correspond to the positions of the quasi-separatrix layers in the magnetic field from the MHD simulation. The QSLs were calculated numerically and are shown in Fig. 19. Also in this figure we have superimposed the photospheric traces of the separatrices from the 8th-order Fourier-filtered topological model of Sect. 3.
![]() |
Figure 19: QSLs in the magnetic field from the MHD simulation. Blue corresponds to regions of high squashing factor. We have superimposed the separatrices from the 8th-order Fourier-filtered topological model of the bright point region. |
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There is a reasonably good correspondence between the two. The footprints of the domes surrounding both rotating sources can be clearly made out in the QSL plot. Particularly close correlations occur along the line of spines of the negative nulls, that bounds the separatrix of the coronal null, and also along the lower righthand edge of the main negative source's separatrix dome. Similar comparisons for the smoothed magnetic field and 16th-order Fourier-filtered cases can be made as well, and also show a convincing correlation to the locations of the QSLs. Of course, there are certain regions where the correspondence is not so good, but these can be explained as before by edge effects or simply by not enough sources having been included in the topological model to produce sufficient accuracy.
A quick comparison by eye shows that there is, as expected, almost perfect
alignment of the QSLs with the locations of high
integrated along the magnetic field, from Figs. 4
and 7. The high level of agreement between the locations
of potential separatrices and MHD QSLs is good evidence that potential field
modelling is able, even in the presence of currents in the MHD simulations,
to make accurate predictions about the locations of reconnection events, up
to a certain accuracy. We have shown that MCT modelling can predict which
separatrix surface will host the reconnection, and can even predict the shape
of that separatrix with reasonable success. However, the obvious question
remaining is, why does only part of the separatrix surface correspond to the
location of the strong integrated parallel electric field and the QSL?
Clearly there is still another factor at play here which we cannot account
for at present, although we have tentatively suggested in
Sect. 4.1 that the QSLs are primarily located close to the
strong photospheric magnetic source regions, and become spread further along
the separatrix surface boundary due to rotation of the sources.
6 Comparison with TRACE observations
The TRACE satellite observed the bright point region during its -phase,
just after the rotation phase. Figure 20 shows an
observation in the 171 Å passband from 14:02:30 UT.
Most of the emission is concentrated near the two main magnetic polarities
of the bright point, as well as at the strong magnetic sources at the top
left and bottom centre of the observed region.
The contours of the integrated parallel electric field (from the numerical simulations described earlier) have been overlaid onto the TRACE observations. Visually, there seems to be a good correspondence between the areas of strong emission in the TRACE images and the areas where fieldlines with high values of integrated parallel electric field are rooted. This lends weight to the theory that magnetic reconnection is powering the emission from the bright point.
However, the regions of high
integrated
along the magnetic field and the regions of strong 171 Å emission observed
by TRACE are not entirely cospatial. There are a few discrepancies, such as the
integrated electric currents at the lefthand side of the BP, the bright region
on the left that extends further north than the strong integrated electric
currents, and the general shape of the observed BP. The shape does seem to be
matched more closely by some portions of the calculated QSLs than by the high
integrated
regions, although the QSLs are not thick
enough to cover the whole observed brightenings. We believe that these
deviations may be caused by other photospheric motions not included in our model
(which only looked at the rotation of one BP magnetic source region) or by the
influence of the strong magnetic field from the nearby AR (see
Sect. 5.1).
![]() |
Figure 20: Above: TRACE 171 Å observation of the bright point at 14:02:30 UT, after the rotation phase. Brighter regions are shown in green, dimmer in blue, with the same field of view as the earlier figures. This TRACE passband mainly shows up brightenings in the transition region, not coronal loops. Below: the same TRACE observation, with overlaid contours in orange, red, green, and blue showing the values of the parallel electric field integrated along the magnetic fieldlines, from the numerical simulation. |
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7 Discussion
In this work we topologically model the solar atmospheric magnetic field in a region where an EUV bright point was observed in the corona, and compare the results with 3D numerical MHD simulations of rotating the two main photospheric magnetic sources that underlie the bright point. We find that both of the sources are associated with separatrix surfaces that completely surround them in the photosphere. Rotating a source causes large concentrations of parallel currents to build up and, after they exceed a plasma-physical threshold, electric fields can build up in the region that are well-correlated with the positions of the separatrix surfaces.
This means that the shear caused by the rotation of a source in turn causes current buildup, that can be dissipated causing reconnection and plasma heating on the separatrix surfaces associated with that source. Hence, potential magnetic field topological models can provide reasonably accurate predictions of locations where enhanced currents and reconnection might be expected to occur.
We use three different approximations to derive the starting set of point magnetic sources from the continuous magnetogram data: 8th- and 16th-order Fourier filtering, and smoothing the magnetic field. Each approximation leads to a different set of sources, so the aim was to find out how robust the large-scale topology is to these changes. In fact, we find that some elements of the topology are remarkably robust. The null points studied here, whose separatrices are large compared to the average distance between null points, can easily be identified in all three cases. Of course, as the number of sources in the model increases, its accuracy in predicting reconnection sites also increases, except for sites close to the edge of the simulation box which can be affected by sources from outside the box not included in the model.
Despite the widely-held belief that coronal nulls are more robust than their photospheric counterparts, we do not find this to be true for the bright point topology studied here. One case includes a positive coronal null which is photospheric in the other two cases, one case has no coronal nulls, and the last has a negative coronal null with no obvious counterpart in the first two cases. However, we do find that the topology preserves its essential large-scale character, independently of the precise method used to select the source set. This is a welcome validation of the magnetic topology technique, as it is specifically intended to detect and model the large-scale pattern of magnetic connections between source regions. It is not related to the complexity of the field studied here; indeed, it might be expected that the choice of sources would have more impact in a region such as this without an overwhelmingly-strong dominant source pair.
The large-scale topology is independent of the method of choosing source regions (within reason!) because it reflects the real topological properties of the real magnetic field. This is also why the MCT model is in close agreement with the QSL model on the location of the (quasi-)separatrices. However, this should not be taken to imply that the choice of magnetic source regions has no effect at all. The small-scale topology shows fluctations depending on the choice of sources. These fluctuations are artefacts of the model. The results of an MCT reconstruction are only reliable on a large scale compared to the source separation, which is fortunately exactly the scale that interests us in this work.
Comparison of the locations of the nulls and separatrices in a potential field with the nulls and QSLs from the MHD simulations shows that in general, and despite its exclusion of currents, the magnetic topology derived from the extrapolated potential field can be used to determine the locations of the separatrix surfaces along part of which the current concentrations linked to reconnection and BP heating will build up. Further work is required to precisely explain why only certain portions of the separatrix surface coincide with regions of high integrated parallel electric field, as the MCT model cannot predict or explain this. A comparison with the observational data from TRACE showed a strong correlation between the locations of brightenings and the locations where fieldlines with high values of integrated parallel electric field are rooted in the photosphere.
For future work, it would be very interesting to test these results on a wider range of observed coronal bright points, to find out whether the results are general or specific to the case studied here.
Acknowledgements
J. Büchner, R. Maclean and E. Priest gratefully acknowledge the opportunities for interaction provided by the Isaac Newton Institute MRT Workshop in Cambridge, August 2004 and the Workshop on Magnetic Reconnection in Florence, September 2006 as well as of the DAAD-ARC project ARC D/05/26090. R. Maclean is grateful for financial support from the UK Science and Technology Facilities Council. We also thank Gunnar Hornig for helpful discussion and suggestions, and the European Commission for financial support through the SOLAIRE Network (MTRN-CT-2006-035484). J. Büchner would also like to acknowledge the stimulating discussions in the ISSI team lead by G. Poletto on Role of current sheets in solar eruptive events supported by the International Space Science Institute (ISSI) in Bern.
References
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- Brown, D. S., & Priest, E. R. 2000, Sol. Phys., 194, 197 [NASA ADS] [CrossRef] (In the text)
- Brown, D. S., Parnell, C. E., Deluca, E. E., Golub, L., & McMullen, R. A. 2001, Sol. Phys., 201, 305 [NASA ADS] [CrossRef] (In the text)
- Büchner, J. 2006a, Space Sci. Rev., 122, 149 [NASA ADS] [CrossRef]
- Büchner, J. 2006b, Space Sci. Rev., 124, 345 [NASA ADS] [CrossRef] (In the text)
- Büchner, J. 2007, in New Solar Physics with Solar-B Mission, ed. K. Shibata, S. Nagata, & T. Sakurai, ASP Conf. Ser., 369, 407 (In the text)
- Büchner, J., & Elkina, N. 2006, Phys. Plasmas, 13
- Büchner, J., & Elkina, N. V. 2005, Space Sci. Rev., 121, 237 [NASA ADS] [CrossRef]
- Büchner, J., & Daughton, W. 2007, in Reconnection of Magnetic Fields: Magnetohydrodynamics, Collisionless Theory and Observations, ed. J. Birn, & E. Priest (Cambridge, UK: Cambridge University Press), 144
- Büchner, J., Nikutowski, B., & Otto, A. 2004, in SOHO 15 Coronal Heating, ed. R. W. Walsh, J. Ireland, D. Danesy, & B. Fleck, ESA SP-575, 35 (In the text)
- Büchner, J., Nikutowski, B., & Otto, A. 2005, in Astrophysical Particle Acceleration in Geospace and Beyond, ed. D. Galagher, & J. Horwitz (Washington DC.: AGU monograph series), 272 (In the text)
- Démoulin, P., Priest, E. R., & Lonie, D. P. 1996, J. Geophys. Res., 101, 7631 [NASA ADS] [CrossRef]
- Golub, L., Krieger, A. S., Harvey, J. W., & Vaiana, G. S. 1977, Sol. Phys., 53, 111 [NASA ADS] [CrossRef] (In the text)
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- Parnell, C. E., Smith, J. M., Neukirch, T., & Priest, E. R. 1996, Phys. Plasmas, 3, 759 [NASA ADS] [CrossRef] (In the text)
- Priest, E. R., & Démoulin, P. 1995, J. Geophys. Res., 100, 23443 [NASA ADS] [CrossRef]
- Priest, E. R., & Titov, V. S. 1996, Phil. Trans. Roy. Soc. A, 354, 2951 [NASA ADS] [CrossRef]
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All Figures
![]() |
Figure 1: Structure of a first-order generic potential magnetic null point. |
Open with DEXTER | |
In the text |
![]() |
Figure 2:
Initial photospheric magnetic field. Above: raw MDI
magnetogram, with greyscale shading indicating magnetic field strengths
between |
Open with DEXTER | |
In the text |
![]() |
Figure 3: Photospheric footprint (only photospheric fieldlines shown for photospheric nulls) of the initial magnetic field from Fig. 2. The source locations and strengths were determined using the 8th-order Fourier-filtering method. Positive (negative) sources are red (blue) circles. Positive (negative) null points are red (blue) triangles. Spine fieldlines are green and separatrix fieldlines are purple. The main negative and positive sources of the bright point are labelled S1 and S2 respectively, and the three important nulls are labelled N1, N2 (photospheric), and C (coronal). Fieldlines in the topological skeleton that mark the photospheric boundaries of the BP's magnetic flux are highlighted: for S1 in orange and for S2 in pink. |
Open with DEXTER | |
In the text |
![]() |
Figure 4:
Contour plot of parallel electric field (
|
Open with DEXTER | |
In the text |
![]() |
Figure 5:
The photospheric footprint (based on 8th-order Fourier-filtered
sources) of the separatrix dome that covers the rotating negative source
(S1), and how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 6:
3D view of the separatrix dome covering the rotating negative
source, with sources calculated using the 8th-order Fourier-filtering
technique. To improve ease of visualisation, all spines are shown but only
separatrix fieldlines in the separatrix surface under discussion are also
displayed. The dome is bounded in the photosphere by the set of green spine
fieldlines whose location corresponds to the region of high
|
Open with DEXTER | |
In the text |
![]() |
Figure 7:
|
Open with DEXTER | |
In the text |
![]() |
Figure 8:
The photospheric footprint (based on 8th-order Fourier-filtered sources) of the separatrix surfaces that surround the rotating positive
source, and how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 9: 3D view of the separatrix surfaces surrounding the rotating positive source, with sources calculated using the 8th-order Fourier-filtering technique. |
Open with DEXTER | |
In the text |
![]() |
Figure 10: Photospheric footprint for smoothed magnetic field sources. |
Open with DEXTER | |
In the text |
![]() |
Figure 11:
The photospheric footprint (based on smoothed magnetic field
sources) of the separatrix dome that covers the rotating negative source, and
how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 12: 3D view of the separatrix dome covering the rotating negative source, with sources calculated using the smoothed magnetic field technique. |
Open with DEXTER | |
In the text |
![]() |
Figure 13:
The photospheric footprint (based on smoothed magnetic field sources) of the separatrix surfaces that surround the rotating positive
source, and how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 14: 3D view of the separatrix surfaces surrounding the rotating positive source, with sources calculated using the smoothed magnetic field technique. |
Open with DEXTER | |
In the text |
![]() |
Figure 15: Photospheric footprint for 16th-order Fourier-filtered sources. |
Open with DEXTER | |
In the text |
![]() |
Figure 16:
The photospheric footprint (based on 16th-order Fourier-filtered
sources) of the separatrix dome that covers the rotating negative source, and
how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 17:
The photospheric footprint (based on 16th-order Fourier-filtered sources) of the separatrix surfaces that together cover the rotating positive
source, and how it compares with the contour plot of
|
Open with DEXTER | |
In the text |
![]() |
Figure 18: Positions of main nulls in the magnetic field from the MHD simulation. The areas containing the main sources are large green circles and the areas containing the main nulls are large red circles. We have superimposed red and blue triangles showing the locations of the critical nulls from the three topological reconstructions of the region. |
Open with DEXTER | |
In the text |
![]() |
Figure 19: QSLs in the magnetic field from the MHD simulation. Blue corresponds to regions of high squashing factor. We have superimposed the separatrices from the 8th-order Fourier-filtered topological model of the bright point region. |
Open with DEXTER | |
In the text |
![]() |
Figure 20: Above: TRACE 171 Å observation of the bright point at 14:02:30 UT, after the rotation phase. Brighter regions are shown in green, dimmer in blue, with the same field of view as the earlier figures. This TRACE passband mainly shows up brightenings in the transition region, not coronal loops. Below: the same TRACE observation, with overlaid contours in orange, red, green, and blue showing the values of the parallel electric field integrated along the magnetic fieldlines, from the numerical simulation. |
Open with DEXTER | |
In the text |
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