{"id":30,"date":"2024-06-17T19:08:10","date_gmt":"2024-06-17T19:08:10","guid":{"rendered":"https:\/\/dev.esp.epss.ucla.edu\/?page_id=30"},"modified":"2024-06-17T19:22:27","modified_gmt":"2024-06-17T19:22:27","slug":"30-2","status":"publish","type":"page","link":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/30-2\/","title":{"rendered":"Research Areas"},"content":{"rendered":"<h4><strong>Solar Wind-Magnetosphere Interactions<\/strong><\/h4>\n<p>The solar wind serves as the ultimate driver of dynamics in Earth&#8217;s magnetosphere, but the exact mechanisms responsible for the interactions are many and complex. Examples include: chaotic solar wind plasma and IMF conditions, reconnection, flux transfer events, dynamics in the magnetosheath, and the highly variable nature of Earth&#8217;s ion foreshock. These disturbances all impact the magnetopause, where they can then generate plasma waves, drive convection, and alter the background magnetic field throughout the rest of the magnetosphere.<\/p>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetopause_t.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-73 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetopause_t.jpg\" alt=\"The magnetotail in the night-side of Earth's magnetosphere is formed from the stretching of the planet's magnetic field by the solar wind. It consists of two lobes with the magnetic field directed mainly sunward (the northern lobe) and anti-sunward (the southern lobe), with the plasma sheet separating the two lobes. Whereas the lobes are populated by cold particles with low concentration, the plasma sheet is populated by hot plasma, mainly of solar origin. Variations in the solar wind and interplanetary magnetic field often trigger burst-like re-configuration in the plasma sheet magnetic field, which results in rapid plasma energization and acceleration. A portion of the charged particle population, energized in the dynamic plasma sheet, can propagate along magnetic field lines and bombard the planet's ionosphere and upper atmosphere to produce a spectacular phenomenon known as the aurora. Other energized particles intrude into the dipole-dominant inner magnetosphere and become trapped in the dipole magnetic field, forming the ring current and radiation belts in the Earth's magnetosphere. &lt;\/p&gt; &lt;a href=&quot;images\/themis.jpg&quot; target=&quot;_blank&quot;&gt;&lt;img src=&quot;images\/themis_t.jpg&quot; width=&quot;175&quot; title=&quot;From October to December 2003, the radiation belts swelled and shrank in response to geomagnetic storms as particles entered and escaped the belts. Credit: NASA\/Goddard Scientific Visualization Studio\" width=\"348\" height=\"293\" \/><\/a><\/p>\n<p>&#8211; Topics: Magnetopause surface waves (THEMIS+, FTEs); Upstream phenomena (Foreshock bubbles, Hot flow anomalies, upstream waves, upstream jets); Coupling (to ULF pulsations and ground signatures).<\/p>\n<p>&#8211; People: Drew Turner, Jiang Liu, Zixu Liu, Vassilis Angelopoulos<\/p>\n<div class=\"divresearch\" style=\"background-image: url('images\/divradbelts.jpg'); border-bottom: white 6px solid;\">\n<h4><strong>Radiation Belt Dynamics<\/strong><\/h4>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-80 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability-300x295.jpg\" alt=\"\" width=\"300\" height=\"295\" srcset=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability-300x295.jpg 300w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability-1024x1008.jpg 1024w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability-768x756.jpg 768w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/radbeltsvariability.jpg 1250w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><br \/>\nEarth&#8217;s radiation belts consist of populations of relativistic protons and electrons that are stably trapped in torus-shaped regions of the inner magnetosphere. Various source, loss, and transport processes are responsible for the often drastic variations in the intensity of the radiation belts. The inner electron and proton belts, located within around 2.5 Earth radii near the equator, change on slower time scales over a solar cycle, though they can also be enhanced in relation to sudden solar events such as coronal mass ejections and solar energetic particle events. Earth&#8217;s outer electron radiation belt is much more dynamic, exhibiting orders of magnitude changes in intensity over timescales ranging from minutes to decades. Some of the most important physical mechanisms in the belts include diffusive processes, which randomly scatter particles with respect to the background magnetic field, Fermi and betatron acceleration (and deceleration), and wave-particle interactions.<\/p>\n<p>&#8211; Topics: Energetic particle telescopes and missions (ELFIN, Lomonosov, THEMIS); comparing observations and theory to better understand various source, loss, and transport mechanisms (shadowing, scattering, heating); particle injections (THEMIS); wave-particle interactions with whistler-mode chorus, magnetosonic waves, plasmaspheric hiss, EMIC waves, and ULF waves; shock injections; diffusive processes; magnetopause shadowing; multi-spacecraft data intercalibration and analysis.<\/p>\n<p>&#8211; People: Drew Turner, Andrei Runov, Christine Gabrielse, Vassilis Angelopoulos<\/p>\n<\/div>\n<div class=\"divresearch\" style=\"background-image: url('images\/divmagtail.jpg'); border-bottom: white 6px solid;\">\n<h4><strong>Magnetotail Physics<\/strong><\/h4>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetotail.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-75 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetotail-300x230.jpg\" alt=\"\" width=\"300\" height=\"230\" srcset=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetotail-300x230.jpg 300w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/magnetotail.jpg 350w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><br \/>\nThe magnetotail in the night-side of Earth&#8217;s magnetosphere is formed from the stretching of the planet&#8217;s magnetic field by the solar wind. It consists of two lobes with the magnetic field directed mainly sunward (the northern lobe) and anti-sunward (the southern lobe), with the plasma sheet separating the two lobes. Whereas the lobes are populated by cold particles with low concentration, the plasma sheet is populated by hot plasma, mainly of solar origin. Variations in the solar wind and interplanetary magnetic field often trigger burst-like re-configuration in the plasma sheet magnetic field, which results in rapid plasma energization and acceleration. A portion of the charged particle population, energized in the dynamic plasma sheet, can propagate along magnetic field lines and bombard the planet&#8217;s ionosphere and upper atmosphere to produce a spectacular phenomenon known as the aurora. Other energized particles intrude into the dipole-dominant inner magnetosphere and become trapped in the dipole magnetic field, forming the ring current and radiation belts in the Earth&#8217;s magnetosphere.<\/p>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis_t.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-91 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis_t.jpg\" alt=\"\" width=\"250\" height=\"193\" \/><\/a><br \/>\n&#8211; Topics: Storms and substorms (energy and flux budget, onset timing, current systems); Plasma sheet dynamics (Low frequency waves, thin current sheets, reconnection, current sheet structure, plasmoid growth and release); Particle acceleration (injections, bursty bulk flows, current generation); Wave particle interactions (ECH).<\/p>\n<p>&#8211; People: Christine Gabrielse, Xiaojia Zhang, Jiang Liu, Andrei Runov, Stefan Kiehas, Vassilis Angelopoulos<\/p>\n<\/div>\n<div class=\"divresearch\" style=\"background-image: url('images\/divionocouple.jpg'); border-bottom: white 6px solid;\">\n<h4><strong>Magnetosphere-ionosphere coupling<\/strong><\/h4>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/eic_sec-1.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-93 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/eic_sec-1-256x300.jpg\" alt=\"\" width=\"256\" height=\"300\" srcset=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/eic_sec-1-256x300.jpg 256w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/eic_sec-1.jpg 700w\" sizes=\"auto, (max-width: 256px) 100vw, 256px\" \/><\/a><\/p>\n<p>Magnetosphere-Ionosphere Coupling refers to the processes which interconnect the lower-altitude ionospheric plasma with the energized plasmas and mechanisms of the high-altitude magnetosphere. These processes include field aligned currents, waves, electric fields, particle precipitation, and ionospheric plasma outflow.<\/p>\n<p>&#8211; Topics: Pulsations, field aligned currents (modeling, convection, closure), vertical currents that do not account for the ionospheric conductivity (similar to field aligned currents), equivalent ionospheric currents (horizontal to the earth surface), and particle precipitation.<\/p>\n<p>&#8211; People: Drew Turner, James Weygand, Vassilis Angelopoulos<\/p>\n<\/div>\n<div class=\"divresearch\" style=\"background-image: url('images\/divlunar.jpg'); border-bottom: white 6px solid;\">\n<h4><strong>Lunar science and space environment<\/strong><\/h4>\n<p><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-89 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis-300x225.jpg\" alt=\"\" width=\"300\" height=\"225\" srcset=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis-300x225.jpg 300w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis-768x576.jpg 768w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/themis.jpg 1024w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><br \/>\nThe &#8220;Acceleration, Reconnection, Turbulence and Electrodynamics of Moon&#8217;s Interaction with the Sun&#8221; mission repurposed two of the THEMIS probes, sending them to the moon to study particle acceleration in the magnetotail, the solar wind, and the lunar wake. From their unique vantage point around the moon as it moves in and out of Earth&#8217;s magnetotail, the two probes measure varying solar wind conditions in three dimensions, including electric\/magnetic fields and charged particles. ARTEMIS characterization of the lunar environment contributes greatly to our knowledge of both heliophysics and planetary physics, and is also critical for future exploration of the moon and other airless bodies, especially for manned missions.<\/p>\n<p>&#8211; Topics: Lunar interior modeling, Plasmoid generation and dynamics.<\/p>\n<p>&#8211; People: Xuzhi Zhou, Stefan Kiehas, Vassilis Angelopoulos<\/p>\n<\/div>\n<p><!--\n\n\n<div class=\"divresearch\" style=\"background-image:url(images\/diviono2.jpg); border-bottom: white 6px solid;\">\n\n\n<h4>Ionospheric dynamics<\/h4>\n\n\n<a href=\"images\/ionosphereprocesses.jpg\" target=\"_blank\" rel=\"noopener\"><img decoding=\"async\" src=\"images\/ionosphereprocesses_t.jpg\" width=\"300\" border=\"0\" title=\"The prominent features in the ionosphere-thermosphere system and their coupling to the different energy inputs, showing the complex temporal and spatial phenomena that are generated.\" style=\"float:right;\"\/><\/a>\nEarth's ionospheric layer develops between 80km to ~1000km due to photo-ionization at the dayside and due to charged particle precipitation from the magnetosphere at the nightside. Our group is involved in studies of the ionosphere from the ground at all latitudes using ground based magnetometers which measure the ionospheric currents, and ground based cameras that measure the auroral activity due to the field aligned currents at high latitudes. Additionally, rockets are flown through the ionosphere to determine both the currents as well as the current generation and dissipation. At the nightside high-latitude auroral regions, we are studying substorm energy flow and the substorm current wedge using the THEMIS Ground Based Observatories, a distributed network of UCLA built magnetometers (as well as Canadian and Alaskan chain magnetometers) plus UCB built All Sky Imagers, most deployed and monitored by Canadian colleagues. A subset of 10 magnetometers are in the continental US at various school locations and double-up as vehicles for education and public outreach. At the dayside equatorial ionosphere, we are studying the large scale current systems that are driven by solar heating. Those current systems are also quite dynamic at times. Through our participation in the DYNAMO rocket campaign with a UCLA-JPL magnetometer, we are participating in the analysis of the data that will determine the validity of Ohm's law for the ionospheric medium at 110km altitude.\n\n-\tTopics: Dayside dynamo (modeling, dynamics)\n\n-\tPeople: Ivan Bernal, Ferdinand Plaschke\n\n<\/div>\n\n\n--><\/p>\n<div class=\"divresearch\" style=\"background-image: url('images\/divaurora.jpg');\">\n<h2>NASA Missions<\/h2>\n<h3><a href=\"http:\/\/themis.igpp.ucla.edu\"><strong>THEMIS<\/strong><\/a>: Time History of Events and Macroscale Interactions During Substorms<br \/>\n<a href=\"http:\/\/artemis.igpp.ucla.edu\"><strong>ARTEMIS<\/strong><\/a>: Acceleration, Reconnection, Turbulence, and Electrodynamics of Moon&#8217;s Interaction with the Sun<br \/>\n<a href=\"http:\/\/elfin.igpp.ucla.edu\"><strong>ELFIN<\/strong><\/a>: Electron Loss and Fields Investigation<\/h3>\n<h4><!--<span style=\"float:right;\">--><a href=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-87 aligncenter\" src=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015.jpg\" alt=\"\" width=\"1588\" height=\"985\" srcset=\"https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015.jpg 1588w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015-300x186.jpg 300w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015-1024x635.jpg 1024w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015-768x476.jpg 768w, https:\/\/dev.esp.epss.ucla.edu\/wp-content\/uploads\/2024\/06\/Teamphoto_Believe_Spring2015-1536x953.jpg 1536w\" sizes=\"auto, (max-width: 1588px) 100vw, 1588px\" \/><\/a><br \/>\nELFIN Team June 2015&#8230; Believe!<!--<\/span>--><\/h4>\n<h2><strong>Experiments<\/strong><\/h2>\n<p><a href=\"http:\/\/elfin-lomo.igpp.ucla.edu\" target=\"_blank\" rel=\"noopener\">ELFIN-Lomo<\/a><br \/>\n<a href=\"http:\/\/elfin-lomo.igpp.ucla.edu\/?epd.shtml\" target=\"_blank\" rel=\"noopener\">EPD Development<\/a><br \/>\n<a href=\"http:\/\/www.igpp.ucla.edu\/public\/DYNAMO-MAG\/\" target=\"_blank\" rel=\"noopener\">DYNAMO\/VHM Development Project<\/a><\/p>\n<h2><strong>Analysis Tools<\/strong><\/h2>\n<h4><a href=\"http:\/\/themis.igpp.ucla.edu\/software.shtml\" target=\"_blank\" rel=\"noopener\">THEMIS Data Analysis Software (TDAS)<\/a><br \/>\nGEANT modeling<\/h4>\n<p>&nbsp;<\/p>\n<hr \/>\n<p>&nbsp;<\/p>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Solar Wind-Magnetosphere Interactions The solar wind serves as the ultimate driver of dynamics in Earth&#8217;s magnetosphere, but the exact mechanisms responsible for the interactions are many and complex. Examples include: chaotic solar wind plasma and IMF conditions, reconnection, flux transfer events, dynamics in the magnetosheath, and the highly variable nature of Earth&#8217;s ion foreshock. These [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-30","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/pages\/30","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/comments?post=30"}],"version-history":[{"count":9,"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/pages\/30\/revisions"}],"predecessor-version":[{"id":33,"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/pages\/30\/revisions\/33"}],"wp:attachment":[{"href":"https:\/\/dev.esp.epss.ucla.edu\/index.php\/wp-json\/wp\/v2\/media?parent=30"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}