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Evolution of the current system during solar wind pressure pulses based on aurora and magnetometer observations
© The Author(s) 2016
- Received: 4 April 2016
- Accepted: 28 July 2016
- Published: 11 August 2016
We investigated evolution of ionospheric currents during sudden commencements using a ground magnetometer network in conjunction with an all-sky imager, which has the advantage of locating field-aligned currents much more accurately than ground magnetometers. Preliminary (PI) and main (MI) impulse currents showed two-cell patterns propagating antisunward, particularly during a southward interplanetary magnetic field (IMF). Although this overall pattern is consistent with the Araki (solar wind sources of magnetospheric ultra-low-frequency waves. Geophysical monograph series, vol 81. AGU, Washington, DC, pp 183–200, 1994. doi:10.1029/GM081p0183) model, we found several interesting features. The PI and MI currents in some events were highly asymmetric with respect to the noon–midnight meridian; the post-noon sector did not show any notable PI signal, but only had an MI starting earlier than the pre-noon MI. Not only equivalent currents but also aurora and equatorial magnetometer data supported the much weaker PI response. We suggest that interplanetary shocks impacting away from the subsolar point caused the asymmetric current pattern. Additionally, even when PI currents form in both pre- and post-noon sectors, they can initiate and disappear at different timings. The PI currents did not immediately disappear but coexisted with the MI currents for the first few minutes of the MI. During a southward IMF, the MI currents formed equatorward of a preexisting DP-2, indicating that the MI currents are a separate structure from a preexisting DP-2. In contrast, the MI currents under a northward IMF were essentially an intensification of a preexisting DP-2. The magnetometer and imager combination has been shown to be a powerful means for tracing evolution of ionospheric currents, and we showed various types of ionospheric responses under different upstream conditions.
- Sudden commencement
- Solar wind dynamic pressure pulse
- Field-aligned current
- Dayside aurora
Sudden commencements (SCs) are abrupt changes in the magnetic field that occur on a global scale and are caused by solar wind dynamic pressure jumps. Because of their distinct nature in magnetometer records, SCs have been used to study the response of the magnetosphere–ionosphere coupling system to solar wind disturbances. In addition to enhanced magnetopause currents that increase the low-latitude horizontal magnetic field (DL component, disturbance at lower latitudes), ionospheric currents and field-aligned currents (FACs) play an important role in characterizing ground magnetic field distributions (Nishida 1964; Tamao 1964; Araki 1994; Zesta et al. 2000; Chi et al. 2001; Kikuchi et al. 2001; Shinbori et al. 2009; Han et al. 2010). The main impulse (MI) of SCs is caused by two-cell ionospheric currents of the DP-2 (disturbance polar of the second type) type as well as a pair of region-1 (R1)-sense FACs. MIs are often preceded by a reversed sense of smaller magnetic field deflections called a preliminary impulse (PI), which corresponds to two-cell ionospheric currents of a reversed DP-2 type and a pair of R2-sense FACs. The initiation of both PI and MI magnetic field variations is considered to occur simultaneously across the entire latitude range including the magnetic equator, and this is attributed to rapid changes in large-scale electric fields (Boudouridis et al. 2011) and their instantaneous penetration to lower latitudes (Araki 1977; Kikuchi 1986). Recently, Kikuchi (2014) presented a comprehensive model of signal transmission from the magnetosphere to the equatorial ionosphere through the ionosphere–ground waveguide.
Global MHD simulations predict that an R2-sense FAC pair during the PI forms equatorward of preexisting DP-2 currents near noon and propagates azimuthally away from noon during its lifetime of a few minutes (Slinker et al. 1999; Fujita et al. 2003; Kim et al. 2009; Samsonov et al. 2010; Sun et al. 2015). An R1-sense FAC pair follows a similar sequence during the MI. The locations and propagation of the FACs provide useful information about the magnetospheric drivers, where the PI and MI currents are related to inertial currents of the compressional wave propagating through the magnetosphere and diamagnetic currents of tailward-propagating pressure structures behind the compressional wave, respectively. In addition, the interplanetary magnetic field (IMF) B y, B z, and Alfvén Mach number are known to alter FAC locations (Yu and Ridley 2011; Peng et al. 2011).
While ground magnetometers are widely used to study ionospheric currents during SCs, their evolution has been examined only in a limited number of studies (Araki et al. 1985; Stauning and Troshichev 2008; Han et al. 2010), and the predictions by global MHD simulations have not been tested comprehensively by observations. The current systems are often drawn using a few snapshots without addressing their propagation or PI–MI transition. Moreover, owing to the limited number of magnetometer stations, it has been difficult to show relative locations of currents prior to SCs and during PIs and MIs. Engebretson et al. (1999) reported an event showing dynamic evolution of equivalent ionospheric currents including a longitudinally propagating PI current by ~15°. Since magnetometers now cover a wide area on Earth, equivalent current motion can be traced over a larger spatial scale.
Another interesting behavior of the SC-related current system is that some SCs do not have a PI or show a PI only in a limited region. The peak occurrence probability of PIs at midlatitude is about 80 %, and the occurrence at low latitude is even lower (~50 %) (Araki et al. 1985; Yamada et al. 1997). Sastri et al. (2001) reported an event where a PI was not symmetric with respect to the noon meridian; the PI was detected only in the pre-noon sector. These studies indicate that PI currents do not always evolve in the conventional way described above, but that PI currents could be highly asymmetric or do not occur in some cases. By using equivalent current maps, we can determine how differently currents in such SCs evolve compared to currents during SCs with PIs in both pre- and post-noon sectors.
Although spatial resolution of ground magnetometers is not always sufficiently high to resolve relative locations of SC-related currents, this limitation can be mitigated by auroral measurements. Imaging from space and ground has demonstrated the capability of detecting auroral intensifications associated with solar wind dynamic pressure enhancements (e.g., Zhou and Tsurutani 1999; Boudouridis et al. 2003; Meurant et al. 2004; Liou et al. 2007; Holmes et al. 2014). A proton and electron diffuse aurora intensifies in the post-noon and pre-noon sectors and propagates antisunward. A discrete aurora poleward of diffuse aurora then intensifies in the post-noon sector. Motoba et al. (2009) and Liu et al. (2011) suggested that auroral behaviors are different during the PI and MI, potentially indicating that these differences can be used as an optical counterpart of SC-related FACs.
In the present study, we combine ground magnetometer and auroral observations to examine locations and propagation of preexisting DP-2, PI, and MI currents using four events for understanding evolution of SC-related currents. These four cases have different IMF and PI conditions: (1) a negative IMF B z with a PI both pre- and post-noon, (2) a negative IMF B z with a PI only pre-noon, (3) a positive IMF B z with a PI both pre- and post-noon, and (4) a positive IMF B z with a PI only pre-noon. We present and discuss similarities and differences in evolution of equivalent currents and auroral emissions.
The Time History of Events and Macroscale Interactions during Substorms (THEMIS) (Russell et al. 2008) and SuperMAG (Gjerloev 2012) magnetometer data in the Northern Hemisphere were used to obtain 2-D equivalent current patterns (in a 1-min cadence) by rotating horizontal magnetic field perturbations by 90° clockwise when viewing from above. Data just before the onset of SCs were used to subtract baselines (the time used for a baseline is indicated in figure captions). To remove magnetopause current effects (DL component), the H-component variations at the dayside low latitude at San Juan multiplied by the cosine of each station latitude divided by the cosine of the San Juan latitude (29.1° in AACGM) were subtracted from the H-component data of each station at each time. Because of the northern daylight conditions in our events (between late April and July), it is reasonable to assume that the ionospheric conductance in the dayside polar ionosphere is high and its spatial gradients are small. Under such conditions, equivalent currents have been widely used as an indicator of ionospheric Hall currents (e.g., Richmond and Kamide 1988), and effects of FACs are limited to ~10 % of magnetic field perturbations (Sun et al. 1985). In this condition, the electric field associated with a clockwise Hall current cell should point away from the center of the current cell. Pedersen currents flow parallel to the electric field and thus connect to downward FACs at the center of the Hall current cell. Similarly, upward FACs are inferred at the center of a counterclockwise Hall current cell. When upward FACs are located near the imager, they are expected to correspond to auroral brightenings in both the red and green lines, as those are carried by precipitating electrons. Downward FACs may correspond to a diffuse auroral brightening in the green line if sufficient proton precipitation occurs. Such a relation can validate the accuracy of equivalent current maps because auroral imaging can specify FAC locations at a much higher spatial resolution even though the spatial coverage is limited. The use of ground magnetometers has an advantage compared to satellite-based magnetic field measurements because of fast temporal variations in SC-related currents. Nevertheless, we validated FAC locations for the first event using Defense Meteorological Satellite Program (DMSP) data (Hardy et al. 1984; Rich 1984) to assist with the interpretation of the auroral signatures. We also referred to Active Magnetosphere and Planetary Electrodynamics Response Experiment (AMPERE) data for the second event. Equatorial magnetometer data from the Magnetic Data Acquisition System/Circum-pan Pacific Magnetometer Network (MAGDAS/CPMN, 1 s) (Yumoto and the MAGDAS Group, 2006) and SuperMAG (1 min) were also used to find effects of penetration electric fields.
Event 1 (southward IMF with post-noon PI)
The event in Fig. 1 has a large SYM-H amplitude of 42 nT associated with a solar wind dynamic pressure pulse preceded by a steady SYM-H level (Fig. 1b, c). This interplanetary shock was measured by both WIND and ACE and was the only shock event around this time (see Additional file 1: Figure S1 for details). Thus, this is an isolated SC event. The IMF was directed slightly southward before the shock (with large B y, Fig. 1a) and then became almost zero for the first few minutes after the shock at WIND, while IMF B z remained negative at ACE. The onset times of the PI and MI can be identified from the 1-s resolution of the magnetometer data in the post-noon polar region (Fig. 1d) as 1835:10 and 1836:50 UT as an abrupt drop and rise in the H-component. However, the PI in the pre-noon sector was initiated slightly later at 1836:09 UT, and the duration of the PI was ~1 min shorter (Fig. 1e). This is not because of the choice of stations but can also be seen in the equivalent currents below. The meridional chains of the magnetometer data pre- and post-noon shown in Additional file 1: Figure S1 confirm the differences in the PI onset time and duration. The equatorial magnetometer data in the post-noon sector show a typical PI and MI (Fig. 1f), and the ratio of the PI and MI amplitudes relative to the level just before the SC (~−5 nT) was 0.23. Here, differences in the magnetic fields between Huancayo (0.62° MLAT) and Villa Remedios (−4.89° MLAT) are used to extract dayside equatorial ionospheric effects since both stations see essentially the same magnetospheric current effects but equatorial electrojet effects are confined within a few degrees from the magnetic equator (Kikuchi et al. 2001).
The aurora data of this event have been presented by Motoba et al. (2009), and we use this as a reference event. The South Pole station was located near 15-h MLT. Figure 1g–j shows geomagnetic north–south keograms of the South Pole imager data for the 630.0- and 557.7-nm wavelengths in the central and western portions of the imager field of view (FOV). Two-dimensional snapshots at five instances are displayed in the right columns. Prior to the SC, a steady discrete auroral arc and a faint diffuse auroral band were present at ~−76° and −72° MLAT, respectively. The diffuse aurora equatorward of −75° MLAT for the 557.7-nm wavelength suddenly brightened during the PI (Fig. 1l, highlighted by the pink arrow), whereas the discrete aurora for both wavelengths did not show any notable change. This brightening was seen more predominantly near the western edge of the imager FOV, i.e., close to magnetic noon. Then, the diffuse auroral brightness further increased during the MI and was later also seen in the eastern portion of the imager FOV. The discrete aurora for the 630.0-nm wavelength also brightened during the MI phase in the western portion of the imager FOV (Fig. 1m, right), and this brightening was connected to a new faint arc that formed equatorward of the preexisting discrete auroral arc. The brightening extended to the east along the newly formed equatorward arc (Fig. 1k, right), and the new equatorward arc then became the dominant auroral structure after the poleward arc merged with the equatorward arc (Fig. 1o, right).
Figure 3b–h shows the equivalent current patterns during the PI and MI phases using the magnetic field deviations from those just before the SC at 1834 UT. During the PI phase, a counterclockwise current cell formed in the pre-noon sector, indicating an upward FAC (Fig. 3b), although no substantial perturbations were seen in the post-noon sector within the available magnetometers (see also Fig. 1d, e). This current formed slightly equatorward and sunward of the preexisting DP-2 currents. The counterclockwise current cell amplified and moved antisunward by ~3-h MLT in 1 min (Fig. 3c), and the post-noon stations detected a clockwise current cell, indicating a downward FAC. The inferred downward FAC is located near the center of the northern conjugate of the South Pole imager FOV, where diffuse auroral intensification is shown in Fig. 1g and h. This current cell also propagated by ~3-h MLT in 3 min and survived longer than the pre-noon PI current cell.
Another pair of DP-2-sense currents formed closer to noon in Fig. 3d, e, and they can be considered as the MI current system. Similar to the PI current system, the current intensity was asymmetric with a larger current cell in the pre-noon sector. In the post-noon sector, the preexisting PI current cell still existed and continued propagating antisunward with a decreasing intensity. The MI currents further intensified and also propagated antisunward (Fig. 3e–h). The antisunward motion of the upward FAC in the MI current system occurred at about the same latitude and timing of the 630.0-nm auroral propagation in Fig. 1k–m, suggesting that the 630.0-nm aurora highlights the evolution of the upward FAC portion of the MI current system.
To summarize this event, the PI and MI current patterns can be characterized by two pairs of current cells that form near noon and then propagate antisunward. Although the PI currents were asymmetric in terms of timing, the behaviors were similar. On the basis of the timing and location, the diffuse auroral intensification during the PI phase can be related to the post-noon downward FACs associated with the PI clockwise equivalent current. Since the diffuse aurora is latitudinally separated from the discrete aurora, the PI current can be seen as a separate current system from the preexisting DP-2 and would be mapped to the dayside magnetosphere on closed magnetic field lines. The upward FAC portion of the MI current system can be represented by the discrete auroral brightening. This has the same sense as the preexisting DP-2 and occurs along the same discrete arc. However, this is a separate current system that forms close to noon and then develops equatorward of the preexisting DP-2 as the currents propagate antisunward, becoming post-SC DP-2 currents. Although the equivalent currents have limitations, as mentioned in the previous section, their use in combination with the imager data allows for the identification of the detailed evolution of the FACs observationally.
Although it is difficult to quantitatively determine the magnetic field mapping accuracy for a dynamically evolving magnetic field geometry during shocks according to our prior work (Nishimura et al. 2013), the accuracy of the model magnetic field mapping is a few degrees in latitude and ~1-h MLT. Since the 630.0-nm auroral arcs spread over ~3° in latitude and elongate in the east–west direction, these model uncertainties would fall within the extent of the large-scale FACs shown in the equivalent current maps. In fact, we showed that the mapped auroral location is within the equivalent current cells.
Event 2 (southward IMF without post-noon PI)
The discrete aurora for the 630.0-nm wavelength abruptly brightened at the onset of the MI, and the center of activity shifted equatorward in a similar manner to the previous event (Fig. 4g, k–o). During the MI, the preexisting arc slowly faded away, and the equatorward arc became the dominant structure (Fig. 4h, k–m), indicating that the MI current system is a separate structure from the preexisting DP-2. On the other hand, the 557.7-nm diffuse auroral intensity slowly increased only during the PI and then abruptly intensified at the onset of the MI (Fig. 4i–m). The lack of clear magnetic and auroral signatures of the PI indicates that the post-noon PI current was not present or much smaller than that in event 1. If we do not have auroral measurements, we cannot rule out the possibility that the lack of a PI in the magnetometer data might be because the PI signal was masked by an MI signal or occurred far away from noon. However, the smaller diffuse auroral luminosity indicates that the PI signal in the post-noon sector was indeed substantially smaller than that in event 1.
The difference in the PI current evolution of these two events raises the question of why the PI currents in event 2 were much smaller and asymmetric than those in event 1, even though they are both comparably large SC events caused by ~8-nPa jumps in the solar wind dynamic pressure. We noticed a difference in the shock normal orientation relative to the Sun–Earth line based on the shock arrival timing at WIND and ACE, and the role of the shock angle is discussed in “Shock orientation” section. Although the IMF B y may also contribute to the asymmetric responses, the PI currents in events 1 and 2 are quite different, even though the magnitude of the IMF B y behind the shocks is only different by a factor of ~2. The MI currents in event 1 became asymmetric (Fig. 3h), but the MI currents in event 2 were more symmetric (Fig. 5f). From these comparisons, we do not see an indication that the IMF B y contributes to the asymmetric response mentioned above.
Event 3 (northward IMF with post-noon PI)
The 557.7-nm diffuse aurora started to brighten during the PI phase equatorward of the preexisting 630.0-nm auroral arc and reached almost the maximum intensity level before the MI (Fig. 6i–l). The 630.0-nm auroral arc brightening occurred during the MI (Fig. 6g, h, k, m). In contrast to events 1 and 2, the arc did not substantially move equatorward but remained essentially at the same latitude. These wavelength-dependent intensifications again indicate that high-energy (seen for 557.7 nm) and low-energy (for 630.0 nm) precipitations have different roles in carrying currents. The diffuse aurora is likely an indicator of the PI currents, which occurred ~8° equatorward of the preexisting currents in this case. The MI currents appear to be an intensification of preexisting currents.
Event 4 (northward IMF without post-noon PI)
Unlike the previous events, the discrete aurora at ~75° MLAT for both 557.7 and 630.0 nm started to brighten during the PI and then intensified further during the MI with a small equatorward expansion. This may be related to the early initiation of the post-noon MI. The 557.7-nm diffuse aurora was negligibly weak during the PI but abruptly intensified during the MI. The lack of diffuse auroral brightening during the PI suggests that the PI current in the post-noon sector was very weak and that the MI current dominated the post-noon current system throughout the SC, even though the pre-noon sector had both a PI and an MI.
Although the SCs in events 3 and 4 are both driven by solar wind dynamic pressure jumps of ~2 nPa under a northward IMF, the PI aurora and currents have striking differences. We discuss a possible cause of this in “Shock orientation” section. The IMF B y is negative in events 3 and 4. Although |B y| is larger in event 3 (~10 nT) than in event 4 (<5 nT), the PI currents are more symmetric in event 3. The MI currents are symmetric in both cases. In these comparisons, we do not see a consistent pattern of IMF B y effects.
In “Event 1 (southward IMF with post-noon PI)”, “Event 2 (southward IMF without post-noon PI)”, “Event 3 (northward IMF with post-noon PI)”, and “Event 4 (northward IMF without post-noon PI)” sections, we showed that PI currents can be highly asymmetric and sometimes undetectably small within the dayside magnetometer coverage, even though these events are all associated with sharp solar wind dynamic pressure jumps. Sastri et al. (2001) also reported an asymmetric PI current pattern and speculated that shock impacts away from the Sun–Earth line could induce asymmetric PI currents. To test this hypothesis, we calculated the shock normal using the ACE and WIND measurements shown in the figures in Additional file 1: Figure S1, Additional file 2: Figure S2 and Additional file 4: Figure S4, Additional file 5: Figure S5. Takeuchi et al. (2002) compared different methods for calculating a shock normal and showed that a time lag method gives the most reasonable solution. In this method, assuming that the shock normal is located on the ecliptic plane and the shock propagates with a constant solar wind speed behind the shock, the time lag of the shock measurements at two different locations in the solar wind gives the orientation. Although the shock normal could also have a component out of the ecliptic plane, it does not explain the asymmetry with respect to the noon–midnight meridian and thus is not considered in this study.
Normal angle of the interplanetary shocks analyzed in this study
Shock arrival UT at ACE
Shock arrival UT at WIND
Solar wind speed (km/s)
SYM-H rise time (min)
Shock normal angle (X–Y) (deg)
Shock normal angle (X-Y) (deg)
Shock normal angle (XY-Z) (deg)
Med/min eigenvalue ratio
Shock normal angle (X-Y) (deg)
Shock normal angle (XY-Z) (deg)
1 (June 14, 2005)
2 (July 07, 2012)
3 (April 26, 2004)
4 (May 30, 2003)
For a comparison, we also estimated the normal angles using the minimum variance analysis (MVA) and coplanarity methods (Takeuchi et al. 2002; Keika et al. 2009). Data within a 5-min window around each shock were used for the MVA, and 1-min median-filtered data before and after each shock were used for the coplanarity method. The azimuthal normal angles estimated by the MVA are close those from the time lag method. The longitudinal angles are not zero but are confined within 30°. However, note that unlike the discontinuities studied by Keika et al. the med/min eigenvalue ratio is <3. As shown in Additional file 1: Figure S1, Additional file 2: Figure S2 and Additional file 4: Figure S4, Additional file 5: Figure S5, the magnetic field jumps across the shocks are often linearly polarized in the GSM Y or Z directions; thus, the median and minimum variance directions are not determined precisely. This may explain ~10° differences between the time lag and MVA methods. The azimuthal angles estimated using the coplanarity method are quite different from the other two methods. Such a difference was also seen in the analysis of Takeuchi et al., and the quasi-linear polarization nature of the changes in the magnetic field at the shocks may again introduce large uncertainties in the coplanarity method.
According to Araki et al. (2004) and Wang et al. (2006), a larger shock normal angle from the Sun–Earth line leads to a more gradual SC because the shock sweeping time across a geoeffective length [30 R E by Araki et al. (2004)] becomes longer. However, the SYM-H rise time in our events does not show a clear dependence on the shock normal angle (Table 1). According to Fig. 3 of Wang et al. (2006), a substantial increase in the rise time seems to occur for events with a normal angle of less than ~150°. Thus, the lack of a rise-time normal-angle dependence in our events could be because of the small normal angles from the Sun–Earth line. Our results indicate that even small shock normal angles from the Sun–Earth line can drive asymmetric responses in the PI and MI currents.
By combining aurora and magnetometer data, we observationally identified evolution of the currents during four isolated SC events. The large amount of magnetometer data allowed us to trace evolution of the PI and MI equivalent currents. The PI current pair formed equatorward and sunward of the preexisting DP-2 currents, and in event 1 with a southward IMF, it propagated antisunward over a 3-h MLT distance across the dawn–dusk meridian. An MI current pair also formed at about the same location at which the PI currents initiated, propagated antisunward, and then became the post-SC DP-2 currents. The overall current pattern is consistent with the model by Araki (1994), and the coexisting current patterns of the PI and MI as well as their antisunward propagation are quite analogous to results from MHD simulations (e.g., Fujita et al. 2003; Samsonov et al. 2010). However, the onsets of the PI and MI were not always simultaneous or symmetric in the pre- and post-noon sectors. The duration and antisunward propagation distance of the PI equivalent currents were also asymmetric in the pre- and post-noon sectors.
By comparing the equivalent currents with the aurora, we identified auroral features that correspond to FACs of the PI and MI current systems, and the high spatial resolution and multiwavelength measurements by imaging can provide more details of the SC-related current evolution. The PI currents can be identified as diffuse auroral brightening that occurs several degrees equatorward of the preexisting discrete aurora (preexisting DP-2 currents). The MI currents can be characterized by the subsequent discrete auroral brightening poleward of the diffuse aurora. Although the overall auroral evolution is consistent with Motoba et al. (2009), we found an interesting dependence on the IMF and PI. When the IMF B z is negative, discrete auroral brightening occurs equatorward of the preexisting discrete aurora, indicating that the MI currents are located equatorward of the preexisting DP-2. For a positive IMF B z, the discrete auroral latitude is essentially unchanged with less antisunward propagation; hence, the MI currents appear as a rebrightening of the preexisting DP-2. Although the limited spatial resolution of the magnetometers does not always show the relative locations of these currents, the ground-based auroral imaging clearly separates the evolution of these currents. The difference in the dynamic pressure may also play a role. In addition, the PI current cells propagated antisunward by ~3-h MLT for the negative IMF B z (event 1), whereas the propagation during the PI cells for a positive IMF B z was smaller (event 3), indicating that the IMF polarity is important for determining the evolution of the equivalent current pattern.
In events 2 and 4, the PI currents were highly asymmetric with respect to the noon–midnight meridian, and no indication of a post-noon PI was detected within the available magnetometer network. The 557.7-nm diffuse aurora during the PI was much weaker than in the other events, and the lack of a post-noon PI is not because the PI signal was masked by other currents but was indeed substantially weaker than those in the other events with a post-noon PI. The PI in the equatorial magnetometer data of these events was also small or not detected, indicating that the penetration of the electric fields to lower latitudes was also weak. In these events, we found that the interplanetary shock normals were more tilted from the Sun–Earth line than those in the other events. Because PI currents are considered to arise from compressional waves in the equatorial magnetosphere that are convert into Alfven waves propagating into the ionosphere (Fujita et al. 2003), a gradual compression of the magnetosphere would lead to a much weaker PI signal. Since the magnetosphere was compressed from the post-noon side, the post-noon MI started earlier than the pre-noon MI; thus, the PI currents were only seen in the pre-noon sector. The post-noon PI would have arrived substantially later than the MI initiation or far from noon where the ionospheric conductance is much lower. The asymmetric nature of the magnetic field disturbance is analogous to that of the TCVs associated with IMF discontinuities (Zesta and Sibeck 2004), and our interpretation of the shock angle effects is consistent with their idea of the discontinuity angle. Although the IMF B y generally contributes to the dawn–dusk asymmetry and may be the reason for the asymmetric MI of event 1, it is not likely the cause of the asymmetric PI responses because the IMF |B y| is large in events 1–3 but the PI asymmetry is seen in events 2 and 4. The Alfvén Mach number is known to alter the SC responses (Yu and Ridley 2011), but the numbers in events 1–3 are in the same range (7–8) and thus do not explain the PI asymmetry.
Liu et al. (2011) inferred that fading of a discrete aurora in the post-noon sector corresponds to the PI phase. None of our events showed such a fading during the PI, but intensification of a diffuse aurora was identified without involving discrete auroral changes. Because their auroral keogram shows a similar fading even before the SC, we think that the fading is due to other dynamic processes of DP-2 currents unrelated to the SC and that PI currents occur equatorward of preexisting DP-2 (discrete aurora) well within closed magnetic field lines. Boudouridis et al. (2003) showed that the polar cap shrinks after shocks. Although we did not see such poleward expansions within our imager FOV, this could be because we focused on several minutes around the SC onset times, whereas they were concerned with changes over longer time scales.
The present study compared an aurora in the dark hemisphere and the magnetic fields in the sunlit hemisphere by taking advantage of the measurements in each hemisphere. The consistency of the initiation times of the PI and MI signals around the conjugate points suggests that the interhemispheric comparison is reasonable. It should be noted, however, that ground magnetic field responses to SCs in the two hemispheres are not the same. The PI magnitude is larger in the sunlit hemisphere (Sastri et al. 2008), and the current pattern may be different (Kim et al. 2013). Although the present study does not compare the current distribution or intensity in the two hemispheres, the auroral brightening locations and intensity in the sunlit hemisphere could be different from the measurements in the dark hemisphere.
Through an analysis of these events, we demonstrated that the combination of magnetometers and an aurora can reveal the detailed evolution of the currents associated with solar wind dynamic pressure pulses and their dependence on the IMF polarity and shock orientation. This approach could be used for other types of solar wind disturbances for understanding the responses of current systems in the magnetosphere–ionosphere coupling system. However, since our results are limited to a case study basis, further examination is needed to evaluate how common the measured signatures are.
YN carried out the work and consulted with the other coauthors. All authors read and approved the final manuscript.
This work was supported by NASA Grants NNX13AI61G, NNX15AI62G, and NAS5-02099 and NSF Grants PLR-1341359, AGS-1451911, and AFOSR FA9550-15-1-0179. The South Pole imager has been supported by a cooperative agreement between NSF and the National Institute of Polar Research, Japan. THEMIS, SuperMAG, and MAGDAS/CPMN data were obtained from http://themis.ssl.berkeley.edu as daily CDF files, from http://supermag.jhuapl.edu/ as daily ASCII files, and by A. Yoshikawa (http://magdas.serc.kyushu-u.ac.jp/) as daily ASCII files, respectively, and we thank the individual magnetometer projects for making these data available for this study, including the National Space Institute at the Technical University of Denmark for Greenland magnetometer data. SYM-H, ACE, and WIND data were downloaded as CDF files through http://cdaweb.gsfc.nasa.gov. Contact the authors for the South Pole imager and satellite data used in this study.
The authors declare that they have no competing interests.
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- Araki T (1977) Global structure of geomagnetic sudden commencements. Planet Space Sci 25:373–384. doi:10.1016/0032-0633(77)90053-8 View ArticleGoogle Scholar
- Araki T (1994) A physical model of geomagnetic sudden commencement. In: Engebretson MJ, Takahashi K, Scholer M (eds) Solar wind sources of magnetospheric ultra-low-frequency waves. Geophysical monograph series, vol 81. AGU, Washington, DC, pp 183–200. doi:10.1029/GM081p0183
- Araki T, Allen JH, Araki Y (1985) Extension of a polar ionospheric current to the nightside equator. Planet Space Sci 33:11–16View ArticleGoogle Scholar
- Araki T, Takeuchi T, Araki Y (2004) Rise time of geomagnetic sudden commencements—statistical analysis of ground geomagnetic data—. Earth Planets Space 56:289–293View ArticleGoogle Scholar
- Boudouridis A, Zesta E, Lyons R, Anderson PC, Lummerzheim D (2003) Effect of solar wind pressure pulses on the size and strength of the auroral oval. J Geophys Res 108:8012. doi:10.1029/2002JA009373 View ArticleGoogle Scholar
- Boudouridis A, Lyons LR, Zesta E, Weygand JM, Ribeiro AJ, Ruohoniemi JM (2011) Statistical study of the effect of solar wind dynamic pressure fronts on the dayside and nightside ionospheric convection. J Geophys Res 116:A10233. doi:10.1029/2011JA016582 View ArticleGoogle Scholar
- Chi PJ et al (2001) Propagation of the preliminary reverse impulse of sudden commencements to low latitudes. J Geophys Res 106(A9):18857–18864. doi:10.1029/2001JA900071 View ArticleGoogle Scholar
- Ebihara Y, Tanaka Y-M, Takasaki S, Weatherwax AT, Taguchi M (2007) Quasi-stationary auroral patches observed at the South Pole Station. J Geophys Res 112:A01201. doi:10.1029/2006JA012087 View ArticleGoogle Scholar
- Egeland A, Burke WJ, Maynard NC, Basinska EM, Winningham JD, Deehr CS (1994) Ground and satellite observations of postdawn aurorae near the time of a sudden storm commencement. J Geophys Res 99(A2):2095–2108. doi:10.1029/92JA03027 View ArticleGoogle Scholar
- Engebretson MJ et al (1999) A multipoint determination of the propagation velocity of a sudden commencement across the polar ionosphere. J Geophys Res 104(A10):22433–22451. doi:10.1029/1999JA900237 View ArticleGoogle Scholar
- Fujita S, Tanaka T, Kikuchi T, Fujimoto K, Hosokawa K, Itonaga M (2003) A numerical simulation of the geomagnetic sudden commencement: 1. Generation of the field-aligned current associated with the preliminary impulse. J Geophys Res 108:1416. doi:10.1029/2002JA009407 View ArticleGoogle Scholar
- Gjerloev JW (2012) The SuperMAG data processing technique. J Geophys Res 117:A09213. doi:10.1029/2012JA017683 View ArticleGoogle Scholar
- Han D-S, Yang H-G, Liang J, Iyemori T, Cowley SWH, Araki T (2010) High-latitude reconnection effect observed at the dayside dip equator as a precursor of a sudden impulse. J Geophys Res 115:A08214. doi:10.1029/2009JA014787 Google Scholar
- Hardy DA, Schmitt LK, Gussenhoven MS, Marshall FJ, Yeh HC, Schumaker TL, Huber A, Pantazis J (1984) Precipitating electron and ion detectors (SSJ/4) for the block 5D/Flights 6–10 DMSP satellites: calibration and data presentation. Rep. AFGL-TR-84-0317 Air Force Geophysics Laboratory, Hanscom AFB, Mass. http://www.dtic.mil/dtic/tr/fulltext/u2/a157080.pdf
- Holmes JM, Johnsen MG, Deehr CS, Zhou X-Y, Lorentzen DA (2014) Circumpolar ground-based optical measurements of proton and electron shock aurora. J Geophys Res Space Phys 119:3895–3914. doi:10.1002/2013JA019574 View ArticleGoogle Scholar
- Keika K et al (2009) Deformation and evolution of solar wind discontinuities through their interactions with the Earth’s bow shock. J Geophys Res 114:A00C26. doi:10.1029/2008JA013481 Google Scholar
- Kikuchi T (1986) Evidence of transmission of polar electric fields to the low latitude at times of geomagnetic sudden commencements. J Geophys Res 91:3101–3105. doi:10.1029/JA091iA03p03101 View ArticleGoogle Scholar
- Kikuchi T (2014) Transmission line model for the near-instantaneous transmission of the ionospheric electric field and currents to the equator. J Geophys Res Space Phys 119:1131–1156. doi:10.1002/2013JA019515 View ArticleGoogle Scholar
- Kikuchi T, Tsunomura S, Hashimoto K, Nozaki K (2001) Field-aligned current effects on midlatitude geomagnetic sudden commencements. J Geophys Res 106(A8):15555–15565. doi:10.1029/2001JA900030 View ArticleGoogle Scholar
- Kim K-H, Park KS, Ogino T, Lee D-H, Sung S-K, Kwak Y-S (2009) Global MHD simulation of the geomagnetic sudden commencement on 21 October 1999. J Geophys Res 114:A08212. doi:10.1029/2009JA014109 Google Scholar
- Kim H, Cai X, Clauer CR, Kunduri BSR, Matzka J, Stolle C, Weimer DR (2013) Geomagnetic response to solar wind dynamic pressure impulse events at high-latitude conjugate points. J Geophys Res Space Phys 118:6055–6071. doi:10.1002/jgra.50555 View ArticleGoogle Scholar
- Liou K, Newell PT, Shue J-H, Meng C-I, Miyashita Y, Kojima H, Matsumoto H (2007) “Compression aurora”: particle precipitation driven by long-duration high solar wind ram pressure. J Geophys Res 112:A11216. doi:10.1029/2007JA012443 View ArticleGoogle Scholar
- Liu JJ, Hu HQ, Han DS, Araki T, Hu ZJ, Zhang QH, Yang HG, Sato N, Yukimatu AS, Ebihara Y (2011) Decrease of auroral intensity associated with reversal of plasma convection in response to an interplanetary shock as observed over Zhongshan station in Antarctica. J Geophys Res 116:A03210. doi:10.1029/2010JA016156 Google Scholar
- Meurant M, Gérard J-C, Blockx C, Hubert B, Coumans V (2004) Propagation of electron and proton shock-induced aurora and the role of the interplanetary magnetic field and solar wind. J Geophys Res 109:A10210. doi:10.1029/2004JA010453 View ArticleGoogle Scholar
- Motoba T, Kadokura A, Ebihara Y, Frey HU, Weatherwax AT, Sato N (2009) Simultaneous ground-satellite optical observations of postnoon shock aurora in the Southern Hemisphere. J Geophys Res 114:A07209. doi:10.1029/2008JA014007 View ArticleGoogle Scholar
- Nishida A (1964) Ionospheric screening effect and storm sudden commencement. J Geophys Res 69(9):1861–1874. doi:10.1029/JZ069i009p01861 View ArticleGoogle Scholar
- Nishimura Y et al (2013) Structures of dayside whistler-mode waves deduced from conjugate diffuse aurora. J Geophys Res Space Phys 118:664–673. doi:10.1029/2012JA018242 View ArticleGoogle Scholar
- Peng Z, Wang C, Hu YQ, Kan JR, Yang YF (2011) Simulations of observed auroral brightening caused by solar wind dynamic pressure enhancements under different interplanetary magnetic field conditions. J Geophys Res 116:A06217. doi:10.1029/2010JA016318 Google Scholar
- Rich FJ (1984) Fluxgate magnetometer (SSM) for the Defense Meteorological Satellite Program (DMSP) Block 5D-2, flight 7. Tech. Rep. AFGL-TR-84-0225, Air Force Geophysics Laboratory, Hanscom Air Force Base, Mass. http://www.dtic.mil/dtic/tr/fulltext/u2/a155229.pdf
- Richmond AD, Kamide Y (1988) Mapping electrodynamic features of the high-latitude ionosphere from localized observations: technique. J Geophys Res 93(A6):5741–5759. doi:10.1029/JA093iA06p05741 View ArticleGoogle Scholar
- Russell CT, Chi PJ, Dearborn DJ, Ge YS, Kuo-Tiong B, Means JD, Pierce DR, Rowe KM, Snare RC (2008) THEMIS ground-based magnetometers. Space Sci Rev 141:389–412. doi:10.1007/s11214-008-9337-0 View ArticleGoogle Scholar
- Samsonov AA, Sibeck DG, Yu Y (2010) Transient changes in magnetospheric-ionospheric currents caused by the passage of an interplanetary shock: Northward interplanetary magnetic field case. J Geophys Res 115:A05207. doi:10.1029/2009JA014751 Google Scholar
- Sastri JH, Takeuchi T, Araki T, Yumoto K, Tsunomura S, Tachihara H, Luehr H, Watermann J (2001) Preliminary impulse of the geomagnetic storm sudden commencement of November 18, 1993. J Geophys Res 106(A3):3905–3918. doi:10.1029/2000JA000226 View ArticleGoogle Scholar
- Sastri JH, Yumoto K, Rao JVSV, Ikeda A (2008) Summer-winter hemisphere asymmetry of the preliminary reverse impulse of geomagnetic storm sudden commencements at midlatitudes. J Geophys Res 113:A05302. doi:10.1029/2007JA012968 View ArticleGoogle Scholar
- Shinbori A, Tsuji Y, Kikuchi T, Araki T, Watari S (2009) Magnetic latitude and local time dependence of the amplitude of geomagnetic sudden commencements. J Geophys Res 114:A04217. doi:10.1029/2008JA013871 View ArticleGoogle Scholar
- Slinker SP, Fedder JA, Hughes WJ, Lyon JG (1999) Response of the ionosphere to a density pulse in the solar wind: simulation of traveling convection vortices. Geophys Res Lett 26:3549–3552. doi:10.1029/1999GL010688 View ArticleGoogle Scholar
- Stauning P, Troshichev OA (2008) Polar cap convection and PC index during sudden changes in solar wind dynamic pressure. J Geophys Res 113:A08227. doi:10.1029/2007JA012783 View ArticleGoogle Scholar
- Sun W, Lee LC, Kamide Y, Akasofu S-I (1985) An improvement of the Kamide-Richmond-Matsushita Scheme for the estimation of the three-dimensional current system. J Geophys Res 90(A7):6469–6474. doi:10.1029/JA090iA07p06469 View ArticleGoogle Scholar
- Sun TR, Wang C, Zhang JJ, Pilipenko VA, Wang Y, Wang JY (2015) The chain response of the magnetospheric and ground magnetic field to interplanetary shocks. J Geophys Res Space Phys 120:157–165. doi:10.1002/2014JA020754 View ArticleGoogle Scholar
- Takeuchi T, Russell CT, Araki T (2002) Effect of the orientation of interplanetary shock on the geomagnetic sudden commencement. J Geophys Res 107(A12):1423. doi:10.1029/2002JA009597 View ArticleGoogle Scholar
- Tamao T (1964) A hydromagnetic interpretation of geomagnetic SSC*. Rep Ionos Space Res Jpn 18:16–31Google Scholar
- Wang C, Li CX, Huang ZH, Richardson JD (2006) Effect of interplanetary shock strengths and orientations on storm sudden commencement rise times. Geophys Res Lett 33:L14104. doi:10.1029/2006GL025966 View ArticleGoogle Scholar
- Yamada Y, Takeda M, Araki T (1997) Occurrence characteristics of the preliminary impulse of geomagnetic sudden commencement detected at middle and low latitudes. J Geomag Geoelectr 49:1001–1012View ArticleGoogle Scholar
- Yu Y-Q, Ridley AJ (2011) Understanding the response of the ionosphere-magnetosphere system to sudden solar wind density increases. J Geophys Res 116:A04210. doi:10.1029/2010JA015871 Google Scholar
- Yumoto K, the MAGDAS Group (2006) MAGDAS project and its application for space weather. In: Gopalswamy N, Bhattacharyya A (eds) Solar influence on the heliosphere and earth’s environment: recent progress and prospects. ISBN-81-87099-40-2, pp 309–405Google Scholar
- Zesta E, Singer HJ, Lummerzheim D, Russell CT, Lyons LR, Brittnacher MJ (2000) The effect of the January 10, 1997 pressure pulse on the magnetosphere-ionosphere current system. In: S-I Ohtani, Fujii R, Hesse M, Lysak RL (eds) Magnetospheric current systems. American Geophysical Union, Washington, D.C. doi:10.1029/GM118p0217
- Zesta E, Sibeck DG (2004) A detailed description of the solar wind triggers of two dayside transients: events of 25 July 1997. J Geophys Res 109:A01201. doi:10.1029/2003JA009864 View ArticleGoogle Scholar
- Zhang Y, Paxton LJ, Zheng Y (2008) Interplanetary shock induced ring current auroras. J Geophys Res 113:A01212. doi:10.1029/2007JA012554 View ArticleGoogle Scholar
- Zhou X-Y, Tsurutani BT (1999) Rapid intensification and propagation of the dayside aurora: large scale interplanetary pressure pulses (fast shocks). Geophys Res Lett 26(8):1097–1100. doi:10.1029/1999GL900173 View ArticleGoogle Scholar
- Zhou X-Y, Strangeway RJ, Anderson PC, Sibeck DG, Tsurutani BT, Haerendel G, Frey HU, Arballo JK (2003) Shock aurora: FAST and DMSP observations. J Geophys Res 108:8019. doi:10.1029/2002JA009701 View ArticleGoogle Scholar