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        <title>Space Science &amp; Space Physics &#8211; Eos</title>
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        <description>Science News by AGU</description>
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	<title>Space Science &amp; Space Physics &#8211; Eos</title>
	<link>https://eos.org</link>
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<site xmlns="com-wordpress:feed-additions:1">195464399</site>                            <item>
                    <title>Hidden Atmospheric Particles Sculpt Near-Earth Space Environment</title>
                    <link>https://eos.org/editors-vox/hidden-atmospheric-particles-sculpt-near-earth-space-environment</link>
                                            <comments>https://eos.org/editors-vox/hidden-atmospheric-particles-sculpt-near-earth-space-environment#respond</comments>
                                        <pubDate>Wed, 22 Sep 2021 12:26:26 +0000</pubDate>
                    <dc:creator><![CDATA[Sergio Toledo, Mats André, Nicolas Aunai, Charles R. Chappell, Jérémy Dargent, Stephen A. Fuselier, Alex Glocer, Daniel B. Graham, Stein Haaland, Michal Hesse, Lynn M. Kistler, Benoit Lavraud, Wenya Li, Thomas E. Moore, Paul Tenfjord, and Sarah K. Vines]]></dc:creator>
                                        <guid isPermaLink="false">https://eos.org/?post_type=editors-vox&#038;p=163314</guid>
                                            <description><![CDATA[Charged particles escape our atmosphere following Earth’s magnetic field and constitute a main source of matter that modulates Sun-Earth interactions.]]></description>
                                                                            <content:encoded><![CDATA[<img src="https://eos.org/wp-content/uploads/2021/09/IonFeature820x615-800x600.jpg"><p>The near-Earth space is filled with charged particles that come from two sources, the solar wind and the Earth&#8217;s upper atmosphere. A new article published in <em>Reviews of Geophysics</em> investigates the relative importance of the two sources of charged particles and their effects on plasma dynamics, especially the process of magnetic reconnection, which is responsible of coupling the Sun magnetic field to the Earth’s magnetic field. Here the authors explain what ionospheric ions are, what we understand about them, and what there is still to discover.</p>
<p><strong>What are ionospheric ions and where do they come from?</strong></p>
<p>Up in the higher altitudes of the atmosphere is the ionosphere where there are increasing number of charged particles ionized by the Sun’s radiation. These “ionospheric ions” reflect the make-up of Earth’s atmosphere: ionized hydrogen, oxygen, nitrogen, and helium can all be found in this region of space.</p>
<p>Electromagnetic processes can give some of these ions enough energy to escape the Earth’s gravity potential, and magnetic field lines guide these particles in their journey to outer space, where they are further energized.</p>
<p>If that escaping rate remained constant, it would take around 1,000 billion years to deplete the atmosphere.Most of these particles do not go back to the atmosphere, and the net average escaping rate is roughly 5,250 tons per year.</p>
<p>This sounds like a large number, but it is actually a very small fraction of the Earth’s atmosphere. If that escaping rate remained constant, it would take around 1,000 billion years to deplete the atmosphere.</p>
<p><strong>Although the loss of ionospheric ions is small, what impact do they have on near-Earth space?</strong></p>
<p>The near-Earth space environment is known as the magnetosphere, i.e., the region where the Earth’s magnetic field dominates over the Sun’s magnetic field. The magnetosphere is like a magnetic bubble immersed in the heliosphere, the region where the Sun’s magnetic field dominates within the solar system. When certain conditions are met, the coupling between these two regions becomes very efficient, allowing large amounts of energy and particles from the Sun to enter the magnetosphere, generating geomagnetic storms and a variety of space weather phenomena.</p>
<p>The magnetosphere is constantly filled by particles from the solar wind and the Earth’s ionosphere.The magnetosphere is constantly filled by particles from two sources: the solar wind and the Earth’s ionosphere.</p>
<p>The relative contribution of the two sources is variable and roughly of the same order of magnitude, but their properties are quite different.</p>
<p>Solar wind ions entering the magnetosphere are composed mainly of H+ ions and a few percent of He++ ions. Ionospheric ions are initially cold, i.e., have lower thermal energy than the solar wind, and often contain large amounts of O+ ions in addition to the much lighter H+ ions.</p>
<p>Ionospheric ions circulate in the magnetosphere following magnetic field convection and are the origin of various magnetospheric populations, including for instance plasmaspheric plumes or the warm plasma cloak. These populations eventually reach the interface between the magnetosphere and the solar wind, i.e., the magnetopause, and change its properties. Therefore, depending on the time-history (hours to days) of the solar wind and the magnetosphere, the magnetopause changes its location and properties, potentially affecting the efficiency of the coupling between the two regions.</p>
<img loading="lazy" class="wp-image-163352 size-full" title="Artist rendition of the MMS mission orbiting in formation the Earth’s magnetosphere" src="https://eos.org/wp-content/uploads/2021/09/SolarWind800w.jpg" alt="Artist rendition of the MMS mission orbiting in formation the Earth’s magnetosphere" width="800" height="615" srcset="https://eos.org/wp-content/uploads/2021/09/SolarWind800w.jpg 800w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-480x369.jpg 480w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-768x590.jpg 768w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-130x100.jpg 130w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-42x32.jpg 42w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-290x223.jpg 290w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-263x202.jpg 263w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-150x115.jpg 150w, https://eos.org/wp-content/uploads/2021/09/SolarWind800w-395x304.jpg 395w" sizes="(max-width: 800px) 100vw, 800px" />Artist rendition of the MMS mission orbiting in formation the Earth’s magnetosphere, to study its interaction with the solar wind. Credit: NASA/Goddard Space Flight Center (Public domain)
<p><strong>How have recent observations and models advanced our understanding of the behavior of ionospheric ions?</strong></p>
<p>The NASA Magnetospheric Multiscale (MMS) mission has revolutionized our understanding of magnetic reconnection, the main process at work for coupling the Earth’s magnetosphere to the solar wind. Its spatial and time resolution has enabled us to understand how different charged particle populations are energized by the reconnecting magnetic fields.</p>
<p>Thanks to that mission, combined with high-performance numerical modeling, we now understand much better how ionospheric ions modify the reconnection process at a microphysical level. Ionospheric ions circulating in the magnetosphere are accelerated at reconnection sites and constitute a significant sink of energy for the reconnection process. In addition, depending on the ion mass, initial energy, and where the ions are entrained in a reconnection site, different energization mechanisms, some of them more efficient than others, come into play.</p>
<p><img loading="lazy" class="wp-image-163353" title="Image of main regions of the Earth’s magnetosphere. Ionospheric ions (light blue) escape and fill the outer magnetosphere until they exit the Earth space environment. " src="https://eos.org/wp-content/uploads/2021/09/IonFig1.jpg" alt="Image of main regions of the Earth’s magnetosphere. Ionospheric ions (light blue) escape and fill the outer magnetosphere until they exit the Earth space environment. " width="800" height="505" srcset="https://eos.org/wp-content/uploads/2021/09/IonFig1.jpg 2128w, https://eos.org/wp-content/uploads/2021/09/IonFig1-480x303.jpg 480w, https://eos.org/wp-content/uploads/2021/09/IonFig1-1024x646.jpg 1024w, https://eos.org/wp-content/uploads/2021/09/IonFig1-768x484.jpg 768w, https://eos.org/wp-content/uploads/2021/09/IonFig1-1536x969.jpg 1536w, https://eos.org/wp-content/uploads/2021/09/IonFig1-2048x1292.jpg 2048w, https://eos.org/wp-content/uploads/2021/09/IonFig1-130x82.jpg 130w, https://eos.org/wp-content/uploads/2021/09/IonFig1-51x32.jpg 51w, https://eos.org/wp-content/uploads/2021/09/IonFig1-159x100.jpg 159w, https://eos.org/wp-content/uploads/2021/09/IonFig1-290x183.jpg 290w, https://eos.org/wp-content/uploads/2021/09/IonFig1-150x95.jpg 150w, https://eos.org/wp-content/uploads/2021/09/IonFig1-395x249.jpg 395w" sizes="(max-width: 800px) 100vw, 800px" />Main regions of the Earth’s magnetosphere. Ionospheric ions (light blue) escape and fill the outer magnetosphere until they exit the Earth space environment. Credit: Toledo-Redondo et al. [2021], Figure 1<strong>What are some of the unresolved questions where further research, data gathering, or modeling is needed?</strong></p>
<p>We still understand relatively little about how magnetic reconnection microphysics shapes the magnetosphere system as a whole.We still understand relatively little about how these recent discoveries about magnetic reconnection microphysics shape the magnetosphere system as a whole.</p>
<p>The impact of cold ions is still an open field of research, as cold ions introduce a new length-scale and many plasma processes depend on the coupling between different scales.</p>
<p>The MMS dataset is continuously growing and only a portion has been extensively analyzed. Combining it with other mission datasets, such as for instance Cluster or THEMIS, to perform large statistical studies in the solar wind parameter space, will shed light about how the system reacts to ionospheric ions on a global scale.</p>
<p>Moreover, global 3D magnetospheric numerical models coupled to the ionosphere are very advanced nowadays and will also deepen our understanding of the global picture of ion circulation and energization in the magnetosphere in response to different kinds of solar activity.</p>
<p>There is yet another ionospheric population, which is even less understood: cold electrons. They also outflow from the ionosphere, and these are even harder to characterize than cold ions. Electrons play crucial roles on magnetic reconnection and wave generation in the magnetosphere. So far, because of the immense difficulty of observing these low-energy electrons, the effects of cold electrons remain largely unexplored.</p>
<p><img loading="lazy" class="wp-image-163354" title="Particle-in-cell simulation of magnetic reconnection, the main coupling process between the solar wind and the Earth’s magnetosphere. " src="https://eos.org/wp-content/uploads/2021/09/IonFig13.jpg" alt="Particle-in-cell simulation of magnetic reconnection, the main coupling process between the solar wind and the Earth’s magnetosphere. " width="800" height="402" srcset="https://eos.org/wp-content/uploads/2021/09/IonFig13.jpg 2128w, https://eos.org/wp-content/uploads/2021/09/IonFig13-480x241.jpg 480w, https://eos.org/wp-content/uploads/2021/09/IonFig13-1024x515.jpg 1024w, https://eos.org/wp-content/uploads/2021/09/IonFig13-768x386.jpg 768w, https://eos.org/wp-content/uploads/2021/09/IonFig13-1536x772.jpg 1536w, https://eos.org/wp-content/uploads/2021/09/IonFig13-2048x1030.jpg 2048w, https://eos.org/wp-content/uploads/2021/09/IonFig13-130x65.jpg 130w, https://eos.org/wp-content/uploads/2021/09/IonFig13-64x32.jpg 64w, https://eos.org/wp-content/uploads/2021/09/IonFig13-200x100.jpg 200w, https://eos.org/wp-content/uploads/2021/09/IonFig13-290x146.jpg 290w, https://eos.org/wp-content/uploads/2021/09/IonFig13-150x75.jpg 150w, https://eos.org/wp-content/uploads/2021/09/IonFig13-395x199.jpg 395w" sizes="(max-width: 800px) 100vw, 800px" />Particle-in-cell simulation of magnetic reconnection, the main coupling process between the solar wind and the Earth’s magnetosphere. The color coding represents plasma number density. The magnetic field lines (solid black lines) break and reconnect at the Electron Diffusion Region, generating reconnection outflow jets. Credit: Toledo-Redondo et al. [2021], Figure 13—Sergio Toledo (Sergio.Toledo@um.es; <img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-4459-8783), University of Murcia, Spain and University of Toulouse, France; Mats André (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0003-3725-4920), Swedish Institute of Space Physics, Sweden; Nicolas Aunai (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-9862-4318), Laboratoire de Physique des Plasmas, France; Charles R. Chappell (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-1703-6769) Vanderbilt University, USA; Jérémy Dargent (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-7131-3587), University of Pisa, Italy; Stephen A. Fuselier (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0003-4101-7901), Southwest Research Institute and University of Texas at San Antonio, USA; Alex Glocer (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0001-9843-9094), NASA Goddard Space Flight Center, USA; Daniel B. Graham (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-1046-746X), Swedish Institute of Space Physics, Sweden; Stein Haaland (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-1241-7570), Max-Planck Institute for Solar Systems Research, Germany, University of Bergen and The University Centre in Svalbard, Norway; Michal Hesse (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0003-0377-9673), NASA Ames Research Center, USA; Lynn, M. Kistler (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-8240-5559), University of New Hampshire, USA; Benoit Lavraud (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0001-6807-8494), University of Bordeaux, France; Wenya Li (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0003-1920-2406), National Space Science Center, China; Thomas E. Moore (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-3150-1137), NASA Goddard Space Flight Center, USA; Paul Tenfjord (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0001-7512-6407), University of Bergen, Norway; and Sarah K. Vines (<img loading="lazy" class="alignnone size-full wp-image-131733" src="https://eos.org/wp-content/uploads/2019/08/ORCID-iD-icon16x16-for-Eos.png" alt="ORCID logo" width="16" height="16" />0000-0002-7515-3285), Johns Hopkins University Applied Physics Laboratory, USA</p>
]]></content:encoded>
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                        <slash:comments>0</slash:comments>
                                                            <post-id xmlns="com-wordpress:feed-additions:1">163314</post-id><enclosure url="https://eos.org/wp-content/uploads/2021/09/IonFeature820x615-150x103.jpg" length="11781" type="image/jpeg" /><media:group><media:content url="https://eos.org/wp-content/uploads/2021/09/IonFeature820x615.jpg" type="image/jpeg" width="615" height="820" fileSize="135778" medium="image" /><media:content url="https://eos.org/wp-content/uploads/2021/09/SolarWind800w.jpg" type="image/jpeg" width="615" height="800" fileSize="224588" medium="image" /><media:content url="https://eos.org/wp-content/uploads/2021/09/IonFig1.jpg" type="image/jpeg" width="1342" height="2128" fileSize="288729" medium="image" /><media:content url="https://eos.org/wp-content/uploads/2021/09/IonFig13.jpg" type="image/jpeg" width="1070" height="2128" fileSize="258374" medium="image" /></media:group>                </item>
                                                <item>
                    <title>Filling the Gaps in the SuperDARN Archive</title>
                    <link>https://eos.org/research-spotlights/filling-the-gaps-in-the-superdarn-archive</link>
                                            <comments>https://eos.org/research-spotlights/filling-the-gaps-in-the-superdarn-archive#respond</comments>
                                        <pubDate>Mon, 13 Sep 2021 12:02:01 +0000</pubDate>
                    <dc:creator><![CDATA[Kate Wheeling]]></dc:creator>
                                        <guid isPermaLink="false">https://eos.org/?post_type=research-spotlights&#038;p=163086</guid>
                                            <description><![CDATA[Researchers present a new pattern-finding technique to better estimate missing data on ionospheric plasma velocities.]]></description>
                                                                            <content:encoded><![CDATA[<img src="https://eos.org/wp-content/uploads/2021/09/magnetosphere-ionosphere-interactions-800x600.jpg"><p>When solar wind slams into Earth’s magnetic field, the impacts ripple down through the planet’s ionosphere, the outer shell of the atmosphere full of charged particles. A global array of high-frequency radars known as the Super Dual Auroral Radar Network (SuperDARN) tracks ionospheric plasma circulation from the ground, giving researchers insights into the interactions between solar wind, the magnetosphere, and the ionosphere. Though widely used in space physics research, the network is not comprehensive—each ground-based radar can measure plasma velocity only in its line-of-sight direction, for example. As a result, there are major spatial and temporal gaps in the SuperDARN archive.</p>
<p>Historically, researchers have filled in these gaps with models that make assumptions based either on climatological averages of the SuperDARN data or on solar wind measurements. In a new study, <em>Shore et al</em><em>.</em> present a new method using a data-interpolating empirical orthogonal function technique, which allows researchers to detect patterns within existing SuperDARN plasma velocity data and then use this information to fill in gaps. The team used observations collected by the network’s Northern Hemisphere stations in February 2001 and filled in missing information at any given time using the velocity patterns deduced from data collected at a given location throughout the month and from other network locations at the same time.</p>
<p>The SuperDARN data set is critical for understanding space weather and its potential impacts on the technologies underlying things like radio communications and satellite services, and this new technique can provide researchers with the most accurate estimates yet of ionospheric electrodynamic variability. (<em>Journal of Geophysical Research: Space Physics</em>, https://doi.org/10.1029/2021JA029272, 2021)</p>
<p>—Kate Wheeling, Science Writer</p>
]]></content:encoded>
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                        <slash:comments>0</slash:comments>
                                                            <post-id xmlns="com-wordpress:feed-additions:1">163086</post-id><enclosure url="https://eos.org/wp-content/uploads/2021/09/magnetosphere-ionosphere-interactions-150x103.jpg" length="3998" type="image/jpeg" /><media:content url="https://eos.org/wp-content/uploads/2021/09/magnetosphere-ionosphere-interactions-150x103.jpg" type="image/jpeg" width="103" height="150" fileSize="3998" medium="image" />                </item>
                                                <item>
                    <title>Looking Down to See Upwards</title>
                    <link>https://eos.org/editor-highlights/looking-down-to-see-upwards</link>
                                            <comments>https://eos.org/editor-highlights/looking-down-to-see-upwards#respond</comments>
                                        <pubDate>Tue, 24 Aug 2021 11:30:14 +0000</pubDate>
                    <dc:creator><![CDATA[Michael A. Hapgood]]></dc:creator>
                                        <guid isPermaLink="false">https://eos.org/?post_type=editor-highlights&#038;p=160997</guid>
                                            <description><![CDATA[Hydrological observations of cosmic ray neutrons scattered by water in soil can also provide information on space weather events such as Forbush decreases and ground level enhancements.]]></description>
                                                                            <content:encoded><![CDATA[<img src="https://eos.org/wp-content/uploads/2021/07/2021SW002800-Figure-17-sized-800x600.png"><p>Hands et al. [2021] provide a great example of how teams in the space weather community are seeking to exploit space-weather-generated signals in instrument sensors designed for other purposes. In this case, those sensors observe cosmic ray neutrons scattered by water in soil (so as to estimate the moisture content of soil). But, as studied here, those sensors can also observe changes in cosmic ray fluxes caused by space weather effects (for example, ground-level enhancements, Forbush decreases, and possibly also terrestrial gamma-ray flashes).</p>
<p>In this paper, a team of space weather and hydrological experts have worked together to explore how to adapt existing networks of cosmic-ray soil moisture monitors for dual use so that they also provide valuable data for space weather purposes. It shows how inter-disciplinary working can expand the range of data available for monitoring space weather and assessing the adverse impacts of future space weather events.</p>
<p><em>Citation: </em><em>Hands, A. D. P., Baird, F., Ryden, K. A., Dyer, C. S., Lei, F., Evans, J. G., et al. [2021]. Detecting ground level enhancements using soil moisture sensor networks. </em>Space Weather<em>, 19, e2021SW002800. https://doi.org/10.1029/2021SW002800</em></p>
<p>—Michael A. Hapgood, Editor, <em>Space Weather</em></p>
]]></content:encoded>
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                                                            <post-id xmlns="com-wordpress:feed-additions:1">160997</post-id><enclosure url="https://eos.org/wp-content/uploads/2021/07/2021SW002800-Figure-17-sized-150x103.png" length="17844" type="image/png" /><media:content url="https://eos.org/wp-content/uploads/2021/07/2021SW002800-Figure-17-sized-150x103.png" type="image/png" width="103" height="150" fileSize="17844" medium="image" />                </item>
                                                <item>
                    <title>The Auroral E-region is a Source for Ionospheric Scintillation</title>
                    <link>https://eos.org/editor-highlights/the-auroral-e-region-is-a-source-for-ionospheric-scintillation</link>
                                            <comments>https://eos.org/editor-highlights/the-auroral-e-region-is-a-source-for-ionospheric-scintillation#respond</comments>
                                        <pubDate>Mon, 09 Aug 2021 11:30:16 +0000</pubDate>
                    <dc:creator><![CDATA[Michael P. Hickey]]></dc:creator>
                                        <guid isPermaLink="false">https://eos.org/?post_type=editor-highlights&#038;p=161654</guid>
                                            <description><![CDATA[Observations reveal a connection between auroral particle precipitation and scintillation, indicating that the ionospheric <em>E</em>-region is a key source region for phase scintillation at auroral latitudes.]]></description>
                                                                            <content:encoded><![CDATA[<img src="https://eos.org/wp-content/uploads/2021/08/2021JA029212-Figure-2df-vertical-sized-800x600.png"><p>Scintillations are random fluctuations of radio signal amplitudes and/or phases caused by irregularities in the ionosphere, which impact global positioning system (GPS) signals. Makarevich et al. [2021] used data covering a period of 166 days from the incoherent scatter radar (ISR) at Poker Flat, Alaska (PFISR) and nearby global positioning system (GPS) receivers to examine the generation mechanisms and possible source regions of ionospheric scintillations.</p>
<p>Scintillations have been traditionally described using the <em>S</em>4 (amplitude) and <em>σϕ </em>(phase) indexes, but when these are unavailable a proxy rate of change of total electron content (ROTI) index is often used. The authors find that the ROTI index exhibits significant correlation and an approximately linear relationship with the phase scintillation metric <em>σϕ </em>in the auroral region while the amplitude scintillation <em>S</em>4 shows no relationship with ROTI or <em>σϕ</em>. The probability of high scintillation measured using ROTI or <em>σϕ </em>also increases with auroral activity. A strong connection between the auroral particle precipitation into the <em>E</em>-region and scintillation (ROTI and <em>σϕ</em>) was noted, indicating that the ionospheric <em>E</em>-region is a key source region for phase scintillation at auroral latitudes. The authors also showed that for one event, scintillations occurred on the trailing edge of a well-defined propagating density enhancement in the <em>E</em>-region, suggesting that the gradient-drift instability was the possible candidate for the plasma structuring and scintillations.</p>
<p>This paper adds to the growing body of evidence that ROTI can be used as a useful proxy for phase scintillation and that the ionospheric <em>E</em>-region is an important source region for ionospheric scintillations at auroral latitudes.</p>
<p><em>Citation: </em><em>Makarevich, R. A., Crowley, G., Azeem, I., Ngwira, C., &amp; Forsythe, V. V. [2021]. Auroral E-region as a source region for ionospheric scintillation. </em>Journal of Geophysical Research: Space Physics<em>, 126, e2021JA029212. https://doi.org/10.1029/2021JA029212</em></p>
<p>—Michael P. Hickey, Editor, <em>JGR: Space Physics</em></p>
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                    <title>Satellite Data Reveal Magnetospause K-H Waves Impact Auroras</title>
                    <link>https://eos.org/editor-highlights/satellite-data-reveal-magnetospause-k-h-waves-impact-auroras</link>
                                            <comments>https://eos.org/editor-highlights/satellite-data-reveal-magnetospause-k-h-waves-impact-auroras#respond</comments>
                                        <pubDate>Thu, 05 Aug 2021 11:30:03 +0000</pubDate>
                    <dc:creator><![CDATA[Michael P. Hickey]]></dc:creator>
                                        <guid isPermaLink="false">https://eos.org/?post_type=editor-highlights&#038;p=161634</guid>
                                            <description><![CDATA[Analysis of multiple satellite data has revealed a striking connection between K-H waves on the magnetopause, surface waves in the hot zone near the plasmapause, and auroral undulations.]]></description>
                                                                            <content:encoded><![CDATA[<img src="https://eos.org/wp-content/uploads/2021/08/2021JA029144-Figure-2h-sized-800x600.png"><p>Horvath and Lovell [2021] are the first to describe two separate geomagnetic storm events occurring in 2017 in which detected Kelvin-Helmholtz (K-H) waves on the magnetopause were observed to be correlated with surface waves in the hot zone of the outer plasmasphere. The Near-Earth Plasma Sheet (NEPS), activated by the K-H waves, acts as a resonator with eigenfrequencies in the Pc4-5 range, and leads to surface waves in the low-density hot zone of the outer plasmasphere.</p>
<p>Observations confirm the coupling along magnetic field lines through field-aligned currents that link these high-altitude undulations to the auroral region. For one event a complex flow channel structure in the auroral regions was observed that appeared as sub-auroral ion drifts (SAIDs) early in the storm, and as sub-auroral polarization streams (SAPS) and abnormal SAIDs at later times. Observed wave structure embedded within the SAPS appeared to correlate well with the KH waves. The paper demonstrates the complex coupling that occurs over extremely large distances from the magnetopause to the auroral zones.</p>
<p><em>Citation: Horvath, I., &amp; Lovell, B. C. [2021]. Subauroral flow channel structures and auroral undulations triggered by Kelvin-Helmholtz waves. </em>Journal of Geophysical Research: Space Physics<em>, 126, e2021JA029144. https://doi.org/10.1029/2021JA029144</em></p>
<p>—Michael P. Hickey, Editor, <em>JGR: Space Physics</em></p>
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