Effects of the Interplanetary Magnetic Field Y Component on the Dayside

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Effects of the Interplanetary Magnetic Field Y Component on the Dayside Liou and Mitchell Geosci. Lett. (2019) 6:11 https://doi.org/10.1186/s40562-019-0141-3 RESEARCH LETTER Open Access Efects of the interplanetary magnetic feld y component on the dayside aurora K. Liou* and E. Mitchell Abstract A dawn–dusk asymmetry in many high-latitude ionospheric and magnetospheric phenomena, including the aurora, can be linked to the east–west (y) component of the interplanetary magnetic feld (IMF). Owing to the scarcity of observations in the Southern Hemisphere, most of the previous fndings are associated with the Northern Hemi- sphere. It has long been suspected that if the IMF By component also produces a dawn–dusk asymmetry and/or a mirror image in the Southern Hemisphere as predicted by some theories. The present study explores the efect of the IMF By component on the dayside aurora from both hemispheres by analyzing the auroral emission data from the Global UltraViolet scanning spectrograph Imager on board the Thermosphere Ionosphere Mesosphere Energetics and Dynamics mission spacecraft from 2002 to 2007. The data set comprises 28,774 partial images of the northern hemispheric oval and 29,742 partial images of the southern hemispheric oval, allowing for a statistical analysis. It is found that even though auroras in diferent regions of the dayside oval respond diferently to the orientation of the IMF By component, their responses are opposite between the two hemispheres. For example, at ~ 1400–1600 MLT in the Northern Hemisphere, where the so-called 1500 MLT auroral hot spots occur, peak auroral energy fux is larger for negative IMF By comparing to positive IMF By. The response is reversed in the Southern Hemisphere. The present study also suggests that the total energy fux does not change with the IMF By orientation change. This result is consist- ent with a larger (smaller) convection vortex in the postnoon sector for IMF By < 0 (By > 0) resulting from anti-parallel merging. Keywords: Dayside aurora, Hemispheric asymmetry, TIMED, GUVI, FUV Introduction region near the midday is typically the weakest in auro- Te auroral oval, when viewed from space, is a continu- ral intensity and was named “the midday gap” (Dandekar ous ring of luminosity circling the magnetic pole and and Pike 1978). Observations with multispectral imaging covering both nightside and dayside. Auroras that occur from the International Satellites for Ionospheric Studies on dayside are considered distinct from their nightside 2 (ISIS-2) satellite suggest that the midday gap is a region counterpart (e.g., Akasofu and Kan 1980; Meng and of intensity minimum (Murphree et al. 1980). It features Lundin 1986). Te statistical precipitation energy fux magnetosheath-like soft electron precipitation and thus into the auroral oval was frst derived by Newell et al. is associated with the cusp (Meng 1981). A few hours east (1996) using particle precipitation data from the Defense of the midday between ~ 1400 and 1600 MLT (magnetic Meteorological Satellite Program (DMSP) satellites and local time) is a region where most intense auroral activity later by Liou et al. (1997) using satellite imaging data in occurs on dayside (e.g., Cogger et al. 1977) and is often far ultraviolet (FUV) from the polar spacecraft. Tese called the 1500 MLT auroral hot spot. Sometimes peri- studies demonstrated two local intensity maxima and odic forms of auroras appear in the afternoon sector (e.g., one intensity minimum in the dayside auroral oval. Te Lui et al. 1989). Te boundary plasma sheet is found to be the major source of the brightest auroral hot spots (Liou et al. 1999). Te morning warm spot, which is less intense *Correspondence: [email protected] The Johns Hopkins University Applied Physics Laboratory, 11100 Johns than the 1500 MLT hot spot, is located between 0600 and Hopkins Road, Laurel, MD 20723, USA © The Author(s) 2019. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creat iveco mmons .org/licen ses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. Liou and Mitchell Geosci. Lett. (2019) 6:11 Page 2 of 10 1000 MLT and is associated with sub-keV electron pre- occurrence of the postnoon dayside auroras. Tis is sup- cipitation (e.g., Newell et al. 1996). ported by multi-spectral observations of the dayside Te morphology of dayside auroras is believed to be aurora from the ground (Hu et al. 2012). Tey found controlled by the IMF orientation because solar wind that statistically auroral intensity at 630.0 nm increases energy enters the magnetosphere mainly through mag- monotonically with the north–south component of the netic merging between the interplanetary magnetic feld solar wind electric feld, with a larger (smaller) increas- (IMF) and magnetospheric feld on the dayside magne- ing rate in the postnoon than in the prenoon oval for IMF topause. For example, the expansion and contraction of By < 0 (By > 0). However, contradictive reports exist. For the auroral oval/polar cap are associated with the north– example, Liou et al. (1998) analyzed the 4-month worth south (Bz in Geocentric Solar Magnetospheric (GSM) of global auroral images from polar and concluded that coordinate) component of the IMF (e.g., Holzworth and the auroral power deposited into the afternoon (1300– Meng 1975) and the dawn–dusk shift of the polar cap 1800 MLT) sector of the northern oval is linearly propor- center for diferent signs of IMF (Holzworth and Meng tional to the magnitude of IMF By component, meaning 1984). Tis has been interpreted by the open magneto- that the magnitude of IMF By is the controlling param- sphere model (e.g., Cowley 1981). eter. More recently, Yang et al. (2013) analyzed the same In addition, the y-component of IMF may result in a data from polar for one full year but found no signifcant hemispheric dawn-dusk asymmetry in the auroral parti- IMF By efect on the dayside auroral intensity. cle precipitation. Te anti-parallel merging theory (Reif If a negative IMF By component favors the occur- and Burch 1985) predicts the merging site in regions of rence of postnoon auroras in the Northern Hemisphere, highest magnetic shear at the magnetopause. As shown what would be expected for the response of the post- in Figure 1, for a southward and large positive (negative) noon aurora to IMF By in the Southern Hemisphere? y-component of IMF, the merging site moves to dawn Tis question has not been fully addressed because most (dusk) in the Northern Hemisphere and dusk (dawn) in of the auroral measurements come from the Northern the Southern Hemisphere. Tis hemispheric dawn-dusk Hemisphere. Hu et al. (2012) addressed this question by asymmetry in the merging site can lead to a hemispheric analyzing ground-based all-sky image data from both dawn-dusk asymmetry of the magnetospheric convection hemispheres. Tey found an asymmetric response of and feld-aligned currents that produce a hemispheric postnoon auroras at 557.7 nm to the IMF By orientation dawn-dusk asymmetry in the dayside aurora." between the two hemispheres. What is interesting in their Te Viking FUV imaging system provided the frst fnding is that there are signifcant diferences between snapshot auroral images on global scales and led to a the intensity and location of the auroral enhancements number of studies of dayside auroral activity in associa- from the two hemispheres in response to the sign of IMF tion with IMF By. For example, Murphree et al. (1981) By (see Figure 2 of Hu et al.). It is not clear if their fnding reported that during non-substorm periods, discrete is physical and implies asymmetries in the hemispheric auroras near 1400 MLT are observed when the IMF By response to the IMF or is associated with instrumental component is often negative. Vo and Murphree (1995) problems, such as lack of inter-calibration of the imagers. found that dayside auroral hot spots observed in the Current understanding of the dayside merging associated Viking UV images usually in the afternoon sector occur with a fnite IMF By component predicts a dawn–dusk mostly during negative IMF By and have a less pro- asymmetry, not a hemispheric asymmetry of the dayside nounced dependence on IMF Bz. Trondsen et al. (1999) aurora. In this study, we will look into this issue difer- examined auroral images from Viking UV imager obser- ently from space with much more data and in a more vations acquired between March 1986 and November quantitative way than previous studies to clarify this puz- 1986 and concluded that increased dayside auroral inten- zle (Fig. 1). sity and the generation of narrow continuous auroral oval around noon are often associated with negative IMF Methodology By rather than positive IMF By. Based on ground-based In this study, observations of the Northern and South- meridian scanning photometer data, Karlson et al. (1996) ern auroras from the Global Ultraviolet Imager (GUVI) reported an asymmetry in the prenoon–postnoon auro- (Paxton et al. 1999) on board NASA’s Termosphere, ral occurrence distribution caused by the IMF By polarity Ionosphere, Mesosphere, Energetics and Dynamics under southward IMF conditions—auroral events pre- (TIMED) satellite during the period of 2002–2007 will dominantly occurring in the postnoon (prenoon) sector be analyzed. Te TIMED spacecraft was launched in the for IMF By < 0 (By > 0). December of 2001 into in a near circular, Sun-synchro- In summary, these previous studies have commonly nous orbit with an averaged altitude of ~ 612 km and a suggested that a negative IMF By component favors the 74.07° inclination angle.
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