A possible mechanism for the formation of an eastward moving auroral spiral

Abstract

The generation process of auroral spirals is described by different theories varying for their morphology and surrounding conditions. Here, a possible mechanism is proposed for an eastward moving auroral spiral, which was observed in Tromsø, Norway, during the expansion phase of a substorm on 18 September 2013. Measurements from the THEMIS-A and Cluster spacecraft were analyzed, which were located up to ∼10 R_E duskward from the spiral generator region in the magnetosphere. Precursory to the spiral observation, concurrent magnetic field dipolarizations, flow bursts and electron injections were measured by the Cluster satellites between 13.6 and 14.2 R_E radial distance from Earth. A local Kelvin-Helmholtz-like vortex street in the magnetic field was detected at the same time, which was likely caused by bursty bulk flows. The vortex street was oriented approximately in the X-Y (GSE) plane and presumably propagated towards the source region of the spiral due to a high dawnward velocity component in the flow bursts. The observations suggest that the spiral can have been generated by an associated vortex in the magnetotail and then mapped along the magnetic field lines to the ionosphere. To better understand the role of the ionosphere in auroral spiral generation, in future more mesoscale observations are required.

1 Introduction

As the optical manifestation of atmospheric ionization through precipitating electrons from the magnetosphere, auroral arcs are commonly observed as narrow bands in the nightside auroral oval. They can, however, reshape and distort into numerous small- and meso-scale structures, among those auroral spirals (Paschmann et al., 2003). An auroral spiral can occur as an individual structure or in a vortex street with multiple spirals (Hallinan, 1976). On average they have diameters of 25–75 km (Partamies et al., 2001b), but can reach sizes up to 1,300 km and thereby they are the largest vortical forms found in an auroral arc (Davis and Hallinan, 1976). As stated by Partamies et al. (2001b), spirals develop primarily during quiet magnetospheric conditions. In the course of a substorm, they occur mainly during the expansion and beginning of the recovery phase (Hallinan, 1976).

Partamies et al. (2001b) observed that the drift motion of auroral spirals coincides with the direction of the ionospheric convection. As viewed from above in the northern hemisphere, auroral spirals wind in a counterclockwise direction around upward field-aligned currents (FACs). Increased auroral precipitation in the FACs connected to brighter aurora is correlated with the winding of the spiral, while its brightness decreases with unwinding (Partamies et al., 2001b). Instead of unwinding, spirals can also decay into patchy auroral structures (Davis and Hallinan, 1976). While the auroral spiral was subject to several ground observations (Davis and Hallinan, 1976; Partamies et al., 2001b) and theoretical approaches (Hallinan, 1976; Partamies et al., 2001a), correlated space and ground measurements as performed by Keiling et al. (2009b) have rarely been done. This is due to a lack of events during which satellites were positioned in a magnetospheric region conjunct by magnetic field lines with the region of a spiral observation. Therefore, the exact generation mechanism and location, which may also vary for different magnetospheric states, is not yet established. In this paper we study an eastward moving spiral event with space measurements and propose a spiral generation mechanism following from the theory by Keiling et al. (2009b).

2 Observations

2.1 Ground-based

2.1.1 Auroral spiral

At 22:58 UT on 18 September 2013, an auroral spiral (see Figure 1 22:58 UT) was observed in Tromsø, Norway (67.176° and 115.627° geomagnetic latitude and longitude). The auroral arc along with the spiral was moving approximately towards east (see Figure 1) with the spiral itself exhibiting anti-clockwise rotation. The sense of rotation here is defined as viewed from above. From Figure 1 22:58 UT, the spiral was estimated to have a diameter of approximately 189 ± 45 km. This estimation was made by determining the zenith angle for the far (72 ± 3°) and near end (50 ± 2°) of the spiral by comparing the positions of star constellations in the photograph with the astronomy software Stellarium (Version 23.2, Zotti et al. (2021)). These angles were then used for trigonometric calculations, taking the auroral spiral to be in an approximate height of 100 km and thus reaching a diameter value of 189 ± 45 km. The spiral was observed during the expansion phase of a substorm. The onset of this substorm was taking place at approximately 22:20 UT, marked by a sharp growth of the AE index to values of ∼500 nT. The expansion phase lasted until about 23:40 UT, when the IMF turned from an entirely southward orientation to exhibiting northward peaks and the AE index decreased rapidly. No records of the duration of the spiral display or its development and decay could be obtained. At 23:27 and 23:34 UT, the photographs in Figure 1 show east-west aligned decreasing auroral activity coinciding with the end of the expansion phase.

FIGURE 1

Met Office, 2010 - 2015). (B) Photographs of the aurora taken in Tromsø on 18 September 2013 (E. Kronberg, personal communication, 22 March 2021). 22:58 UT: Auroral spiral formation. 23:27 UT and 23:34 UT: decreasing auroral activity with increasingly quiet auroral arcs.

2.1.2 Equivalent ionospheric currents

Equivalent ionospheric currents (J_eq) here are defined as sheet currents that generate magnetic field variations at the Earth’s surface that are equivalent to the measured ground horizontal field perturbations (Untiedt and Baumjohann, 1993). With the simplified assumptions that the currents flow near the Earth’s surface, approximated as a plane, the equivalent ionospheric currents can be defined as times unit surface area. The vector B_h represents the horizontal magnetic disturbance and is the unit vector that points vertically downward. This equation then corresponds to J_eq being equal to the horizontal magnetic field vector rotated 90° clockwise (Untiedt and Baumjohann, 1993).

J_eq directions as seen in Figure 2 were retrieved from 10 s IMAGE magnetometer data by the Spherical Elementary Current System (SECS) method as described by Juusola et al. (2016). Three time steps around the observation of the auroral spiral (22:58 UT) are shown. Tromsø was located in the westward current region with magnitudes of ∼500 A km⁻¹. The field of view from Tromsø with a zenith angle of 72° is marked by a green dotted ellipse in the middle panel of Figure 2. There, the solid green ellipse shows an estimate of the spiral size with 189 ± 45 km in diameter. The spiral thus occurred in the region of downward field-aligned currents. During the occurrence of the optical auroral spiral, no equivalent ionospheric current vortices could be identified and the currents did not vary much in strength or direction throughout the shown time interval.

FIGURE 2

2.2 Cluster and THEMIS measurements

Measurements from three of the Cluster spacecraft (in the following called Cl1, Cl2 and Cl4) and the THEMIS-A (TH-A) satellite were obtained from Cluster Science Archive (Laakso et al., 2010) and NASA CDAweb, respectively. At the time of the spiral observation the Cluster and THEMIS-A spacecraft were positioned in the magnetotail (see Figure 3). The retrieved magnetic field measurements, plasma flow velocity and electron flux, temperature and density are displayed in Figure 4 for the time period of 22:40 UT to 23:10 UT.

FIGURE 3

FIGURE 4

The magnetic field (see Figures 4A–D) measured by FGM instruments shows dipolarization signatures for the Cluster spacecraft starting from ∼22:54 UT. The Cl1 data show a short peak in the B_Z component around 22:55 UT, then a longer lasting increase with further peaks of the B_Z component at 22:57 UT. These signatures known as dipolarizations are understood as the change of the magnetotail field from a stretched to a more dipolar configuration. Cl4 shows less distinct signatures than Cl1 around 22:55 UT, but also a peak of the B_Z component at 22:57 UT. The satellite located farthest from Earth, Cl2, shows less variation than the other Cluster spacecraft in all magnetic field components, but also enhancements at 22:57 UT. In the TH-A magnetic field data no large perturbations are visible over the whole regarded time period. The Y component is near zero for the whole interval with a slight increase at ∼22:53 UT. The X and Z components constantly decrease from 22:40 UT to 23:10 UT.

The plasma flow velocities (see Figures 4E, F) were obtained from measurements by the Cl4 CIS-CODIF instrument and the TH-A ESA instrument. For the examined time interval, only the Cl4 CIS-CODIF instrument was operational. Enhanced quasi-periodical plasma flows can be discerned in its data from ∼22:50 to ∼22:58 UT. With a period of ∼2 min, the velocity in X direction (GSE) increases repeatedly to over ∼500 km s⁻¹ before receding to ∼0 km s⁻¹. The Y component shows the same development, with peak velocities of up to ∼500 km s⁻¹ in negative Y direction (GSE). From about 2 min before the development of the optical auroral spiral in Tromsø, the deviations in X and negative Y direction (GSE) were most pronounced and the Z component showed enhanced flows of up to ∼500 km s⁻¹. TH-A measured plasma flow that was slower than the Cl4 flow by one order of magnitude. Flow enhancements in the TH-A data starting at ∼22:49 UT can be seen in Figure 4F, which approximately concurs with the start of the high-speed flows visible in the Cluster data. The TH-A plasma velocity fluctuated between ∼40 km/s in positive and negative X directions (GSE). The Y component also fluctuated with peak velocities of ∼40 km s⁻¹ and ∼70 km s⁻¹ in dawn and dusk direction, respectively. These deviations in the TH-A flow velocity last only up to ∼22:56 UT.

The electron flux data from the Cluster RAPID instrument and the TH-A SST instrument is shown in Figures 4G–J. In the Cl2 data plots, strong signatures of dispersionless electron injections are discernible around 22:57 UT. Only the TH-A electron flux measurements with good data quality are displayed. The presented energy levels are not equal, but comparable to the Cluster energy channels. In the intervals where data with good quality was available, no variations in electron flux can be observed, while for the time of most interest no measurements are available.

In the interval between 22:49—22:56 UT the Cl1 electron total temperature and density (Figures 4J, K) measured by the PEACE instrument show quasi-periodical spikes in the electron density at the same time as sharp dips in the temperature. This dense and cold plasma alternates periodically with depleted and hot plasma, which is a typical signature of Kelvin-Helmholtz vortices (Hasegawa et al., 2009).

Overall, the Cluster data show deviations in all observed parameters up to 9 min precursory of the development of the visible auroral spiral in Tromsø.

3 Methods

3.1 Mapping

To correlate the spiral observations with their respective source regions in the magnetosphere, magnetic field line mapping was applied. Firstly, to determine the ionospheric footprints of the Cluster and TH-A satellites for the 18 September 2013 substorm, and, in particular, the time of the auroral spiral observation (22:58 UT). Secondly, a possible source region of the spiral was determined to evaluate if the structures observed by the spacecraft can have been correlated with the auroral spiral.

For these processes, the Python-based module IrbemPy, which is based on the IRBEM-lib library (Boscher et al., 2010) was used. It is part of the Python package SpacePy (Morley et al., 2010). As input options for the computation, the International Geomagnetic Reference Field (Erwan et al., 2015) was chosen as the internal magnetic field model and set to be updated on 18 September 2013. As the external magnetic field model, the Tsyganenko 1996 (T96) (Tsyganenko, 1995; Tsyganenko, 1996) magnetospheric model as stated below was selected. It was chosen above newer models, because it is also used in similar research (e.g., Keiling et al. (2009a)) and the T02 and T05 models primarily represent stormy or quiet conditions, while the here regarded event occurred during a substorm (Tsyganenko, 2002; Tsyganenko and Sitnov, 2005). For the mapping, the hourly values of the Kp, Dst and AL indices, as well as the solar wind density, velocity and dynamic pressure and the IMF B_Y and B_Z components were obtained from the NASA/GSFC’s OMNI data set through the OMNI module (Morley et al., 2010).

3.1.1 Ionospheric footprints

The footprints of the magnetic field lines conjunct with the Cluster and TH-A spacecraft were derived using IrbemPy and position data retrieved from the Cluster Science Archive and NASA CDAweb. They are defined here as intercept points of these field lines and the ionosphere at an altitude of 100 km in the northern hemisphere. From 21:00 UT to 02:00 UT, the footprints lie in the area of the auroral oval in the dusk sector (see Figure 5). At 22:58 UT, the time of the auroral spiral observation, the footprints are located at longitudinal distances from Tromsø of for Cluster and for TH-A. The results from T96 were compared with newer models for quiet and stormy conditions (T02 and T05). These models delivered no footprints for the northern hemisphere for the time interval of 21 UT to ∼23 UT, placing the satellites on open field lines that were only connected to the southern hemisphere. These different results can be due to all these models not well representing substorm conditions of the magnetosphere and the area in which the satellites were located.

FIGURE 5

3.1.2 Spiral generator region

A possible magnetospheric generator region of the auroral spiral was derived with the constraint of it being conjunct with Tromsø by a magnetic field line. As explained below, the Cluster satellites observed Kelvin-Helmholtz vortices and it is suggested that after encountering the satellites these vortices possibly traveled to the generator region mentioned here, where they mapped down to the ionosphere to produce the optical spiral. Starting from the location of the Cl4 satellite at 22:58 UT, the coordinates were iteratively varied until their footprint was located in a radius of less than 50 km around Tromsø using the T96 model and IrbemPy. A potential source region of the spiral is thus located at around X_GSE = −3.8 R_E, Y_GSE = −1.7 R_E and Z_GSE = 2.4 R_E. The absolute distance of this area to the Cluster satellites amounts to ∼12.1 R_E.

3.2 Minimum variance analysis

To suitably display and analyze the spacecraft data in a local spacecraft coordinate system, Minimum Variance Analysis (MVA) as first proposed by Sonnerup and Cahill Jr (1967), was performed on the magnetic field and ion velocity data sets of Cl1, Cl2, Cl4 and TH-A. For TH-A the results of this method are not presented in the following, because the weak structures it detected were better displayed in the GSE coordinate system.

The method of MVA used here was derived from Sonnerup and Scheible (1998); Dunlop et al. (1995). In the time interval from 22:40 UT to 23:10 UT, the times of the maximum in the B_Z (GSE) component of the Cluster magnetic field measurements were identified. For Cl1 the maximum was at 22:57:06 UT, for Cl2 at 22:57:37 UT and for Cl4 at 22:56:45 UT. A time period of 10 min symmetrically around 22:57:26 UT was selected for all Cluster satellites, this being the medium point in time between the Cl4 and Cl2 B_Z maximum values. This interval was used for MVA calculations for each satellite to enable comparisons and showed reasonably good results for all three spacecraft.

The calculated eigenvalues and eigenvectors of the magnetic variance matrix (Dunlop et al. (1995); Sonnerup and Scheible, 1998) are listed in Table 1. The eigenvalues of the variance matrix describe the deviations of the field in the respective field directions, with the eigenvector n of the smallest eigenvalue (λ₃) pointing in the expected direction of the boundary normal (Sonnerup and Scheible, 1998). The ratio λ₂/λ₃ is a measure for the quality of the direction estimates. Dunlop et al. (1995) give values of two to three for the λ₂/λ₃ ratio as a typical guideline. Here, the λ₂/λ₃ ratios were ∼2.0 for Cl1, ∼3.5 for Cl2 and ∼2.6 for Cl4 (see Table 1). As can be seen, the variance matrix is nearly degenerate for the three satellites, i.e., λ₃ ≃ λ₂. The boundary normal n is therefore not very well defined, although the eigenvector l is a good representation of a tangential direction to the boundary layer (Sonnerup and Scheible, 1998). According to Sonnerup and Scheible (1998), for near-degenerate cases, the eigenvectors m and n are prone to permute when modifying the time period for the calculation. As stated by Sonnerup and Scheible (1998) and Song and Russell (1999), this can be analyzed by executing the above method with different nested time intervals between 22:40 and 23:10 UT. All other time periods essentially showed similar λ₂/λ₃ ratios and highly changing directions of the eigenvectors m and n implying that the observed structure is 3-dimensional. The MVA in this case is not applicable.

For identification of the vortical structures in the magnetic field and ion flow velocity we can use an arbitrary orthogonal coordinate system. We have decided to use the one obtained above because it is orthogonal according to the dot product between the eigenvectors. The axes of the resulting LMN system are shown in Figure 6 with respect to the GSE coordinate system. The axes are defined so that the basis vectors l, m and n are parallel to the equivalent L, M and N axes. As can be seen, the direction of maximum variance l coincides approximately with the X (GSE) direction for all three Cluster satellites. However, the orientation of m and n varies for the satellites because the moving structure is 3D.

FIGURE 6

The transformed magnetic field and ion flow velocity were projected to the L-M plane of the LMN coordinate system (see Figure 7). The TH-A data was accordingly projected to the X-Y (GSE) plane for the whole time period of 22:40 to 23:10 UT (see Figure 8). The Cluster magnetic field vector projections show rotational signatures in the time interval of 22:56 to 22:59 UT. Cl2, the most remote satellite, shows three major variations in sign of the B_L component. Cl1 and Cl4, which were located closer together and nearer to Earth than Cl2, show one rotational signature coinciding with the first change of sign for the Cl2 B_L component. For Cl1, which was closest to Earth, the signature is weaker than for Cl4. The vector projection of the plasma velocity does not show changes in sign for the v_L component, but a change in the predominant v_M direction in the time interval from 22:57 to 22:59 UT. The TH-A magnetic field data shows a change of sign of the B_Y component around 22:57 UT. Its plasma velocity also shows major variations of the v_Y component to positive and then negative values in the time period of 22:52 to 22:55 UT.

FIGURE 7

FIGURE 8

4 Discussion

On 18 September 2013 at 22:58 UT, an auroral spiral was observed in Tromsø during the expansion phase of a substorm. Simultaneously, measurements in the magnetotail by three Cluster and the THEMIS-A spacecraft were obtained.

The three Cluster spacecraft measured strong variations in the magnetic field components, the plasma flow velocity and the electron flux approximately 1–2 min prior to the spiral development in Tromsø (see Figure 4). The plasma flow velocity from Cl4 over a time interval of 8 min showed quasi-periodic peaks in velocity up to ∼500 km s⁻¹ in X and Y directions. These measurements correspond to the signatures of bursty bulk flows with intermittent flow bursts (Angelopoulos et al., 1992). As they commonly are (Paschmann et al., 2003), these bursty bulk flows were accompanied by dipolarization signatures seen in the B_Z magnetic field components. The vector plots of the Cluster magnetic field projected onto the L-M plane of the local LMN coordinate system, which varies for each spacecraft, also show vortical signatures (see Figure 7). Cl2 encountered a magnetic field vortex street approximately oriented in the X-Y plane (GSE) with opposed rotating vortices on either side of its trajectory, as shown in Figure 9. Cl1 and Cl4 only measured a pair of opposed rotating vortices located roughly in the X-Z plane (GSE). Cl1 and Cl4 were positioned close together, so it is likely that they observed the same pair of magnetic field vortices.

FIGURE 9

If the frozen-in condition is valid, it is expected that the magnetic field vortices are connected to plasma flow vortices. The plasma flow velocity observed by Cl4 exhibited a change of direction at the occurrence of the magnetic field vortices, which suggests a vortical structure. Clear signatures of plasma vortices were not detected by the Cl4 spacecraft, likely because the CIS instrument used to measure the plasma velocity has a time resolution of ∼4 s. The magnetic field vortices however occurred at a temporal scale of ∼30 s.

These magnetic field vortices were probably associated with the bursty bulk flows that were also measured by Cl4. Bursty bulk flows are known to cause vortical structures in plasma flow in the X-Y (GSM) plane, when they encounter the dipolarized region of the inner magnetosphere (e.g., Panov et al., 2010; Birn et al., 2011). It was also observed by e.g., Volwerk et al. (2007) that Kelvin-Helmholtz instabilities appear together with bursty bulk flows. Hasegawa et al. (2004) detected plasma flow and magnetic field signatures caused by a Kelvin-Helmholtz instability at the magnetopause. Their magnetic field perturbations are different than shown in Figure 7, because the perturbations in our study are probably caused by pairs of oppositely rotating vortices, not by a single vortex street. TH-A was located closer to Earth and did not measure any vortical structures (see Figure 8). As seen in Figures 4J, K, Cl1 observed signatures in the electron temperature and density that are typical for Kelvin-Helmholtz instability, similar to Cluster observations described by Hasegawa et al. (2009). Therefore, the Cluster satellites likely observed a Kelvin-Helmholtz-like vortex street in the magnetic field induced locally by the measured bursty bulk flows. It has however to be taken into account that part of these results are based on the MVA, which produced results that were not ideally reliable.

Keiling et al. (2009b) observed short-lived equivalent ionospheric current vortices of 600–800 km size associated with the appearance of auroral spirals. In this study, such short-lived vortical J_eq structures could not be resolved. This can be due to the size of the auroral spiral (189 ± 45 km) and the comparative spatial resolution of the IMAGE magnetometer network. The stations in the vicinity of Tromsø have an average calculated distance of km to Tromsø, but the coverage in this area is limited by the ocean to the north and west. Therefore, the only station in the spiral region (marked by the green solid ellipse in the middle panel of Figure 2) is Andenes (AND). According to the estimates of the spiral location and size at the time of the photograph in Figure 1 the spiral was not located in the zenith over Tromsø, and only marginally over Andenes. This can potentially lead to the missing deflection of the ionospheric currents during the optical spiral. To better resolve such structures, more mesoscale observations as described by, e.g., Gabrielse et al. (2023) would be helpful. Another possibility for the absence of vortical J_eq structures is that the particle precipitation during this observed spiral event can have been too weak to deflect E-region plasma flows.

To be able to correlate the ground observations and space measurements, the ionospheric footprints of the satellites were derived with the T96 external magnetic field model. They were located in the pre-midnight sector of the auroral oval (see Figure 5). The footprints lay at a distance from Tromsø of and in longitude for Cluster and TH-A, respectively. Since the spiral was developing up to in longitude west of Tromsø, as inferred from the field of view from Tromsø (Figure 1), the longitudinal distance of the footprints to the visible spiral may have been smaller than their distance to Tromsø. In the magnetosphere, the possible source region of the auroral spiral was located ∼10.1 R_E in Y (GSE) direction from the Cluster satellites. It has to be taken into account that topological magnetic mapping is not very reliable during substorm conditions in particular (Paschmann et al., 2003). The T96 model may describe the overall conditions of this event better than the newer models, but it does not specifically represent substorms (Tsyganenko, 1996). For a strongly disturbed magnetosphere, it is known not to display the dawn-dusk asymmetry of the inner magnetosphere and to overstretch the field lines (Tsyganenko, 2001). Also, the discrepancy between the results of the newer models T02 and T05 and the T96 model is very high, since the newer models generate an entirely different field line topology in placing the spacecraft on open field lines. This shows the high uncertainty in the mapping and therefore also in the interpretations. With these aspects considered, the footprints calculated with the T96 magnetospheric model are regarded only as an approximation for the real ionospheric footprints of the spacecraft. The derivation of the magnetospheric source region of the auroral spiral is treated equally. Due to the uncertainty of magnetic mapping during substorm conditions, the Cluster satellites may have been located closer to or further from the source region of the spiral than the computations suggest. Also, the plasma velocity measurements discussed above exhibited significant flow bursts and the electron temperature and density showed signatures typical for KHI. Approximately 2 min before the spiral development, the plasma velocity started to increase to an absolute value of v ≃ 960 km s⁻¹. The flow bursts could have produced the vortices in the magnetic field and plasma. With a distance d = 12.1 R_E between the spacecraft and the possible source region and t = d/v, a propagation time t ≃ 80 s of the vortex street observed by Cl2 to the generator region can be estimated. A schematic illustration of this movement is given in Figure 10. It is assumed that the propagation of the plasma flow in X direction is slowed due to the dipolarized magnetic field near the Earth. In Figure 5, the ionospheric footprints of this motion are depicted.

FIGURE 10

Following from the above calculation it can be possible that the magnetic field vortices, associated bursty bulk flows, KHI and dipolarizations detected by the spacecraft and described above were correlated with the spiral formation. What must be emphasized again, however, is the high uncertainty in the field line mapping during substorm conditions. This makes these interpretations mostly suggestions for a generation mechanism of the auroral spiral, based more on the temporal correlation of the vortices in the magnetotail and the optical spiral than on the exact spatial positions.

This suggestion proposes the spiral formation taking place already in the magnetosphere, not only in the ionosphere. Therefore, taking into account the available data, the spiral generation theory presented by Hallinan (1976) is not applicable to this event, since it states that the spiral only fully develops in the ionosphere.

According to a theory by Keiling et al. (2009b), plasma flow vortices in the magnetosphere are the initiator of a spiral, which then maps to ionospheric altitudes. These vortex structures can in turn be caused by either ballooning instabilities (e.g., Voronkov et al. (1997)) or bursty bulk flows (Keiling et al., 2009a; Panov et al., 2010). On encountering the dipolarized magnetic field in the inner magnetosphere, the high-speed plasma flows are decelerated (Panov et al., 2010; Birn et al., 2011). By their deflection around the dipolar magnetic field, vortices with opposed sense of rotation form on both sides of the flows (Panov et al., 2010).

5 Conclusion

The observations of dipolarizations and bursty bulk flows in this study coincide with the theory by Keiling et al. (2009b). In contrast to the detected structures of this event, Keiling et al. (2009b) also observed opposed rotating J_eq vortices that developed and decayed concomitant with auroral spirals. They associated these vortices with upward and downward field-aligned currents, which were driven in the magnetosphere by a pair of vortical plasma flows. According to Keiling et al. (2009b), the generation of the auroral spiral was likely initiated in the region of strong plasma flows between the plasma flow vortices in the magnetosphere. Here, such conclusions can not be drawn in the same way, because there were no equivalent ionospheric current vortices detected. The evidence of a vortex pair of J_eq in the ionosphere connected to plasma flow vortices in the magnetosphere was also not given. This can be due to the lack of mesoscale observations that can resolve these structures. However, with ∼500 A km⁻¹ the westward electrojet current observed was stronger than an average substorm expansion current (Juusola et al., 2015), which may have helped establish an the instability for the spiral formation. Also, the magnetic field and possibly plasma vortices observed in the magnetotail caused by the eastward bursty bulk flows can have propagated toward the spiral source region and then mapped to the ionosphere as proposed similarly by Keiling et al. (2009b).

For future research on the interaction of magnetosphere and ionosphere in the generation of auroral spirals extended mesoscale observations in the ionosphere are needed. Also, for optical detection of auroral spiral events complementary to all sky cameras, citizen science projects like Aurorasaurus (MacDonald et al., 2015) are helpful.

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