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Journal articles on the topic 'Moon-Plasma Interactions'

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1

Kivelson, Margaret G., Xianzhe Jia, and Krishan K. Khurana. "Medicean Moons Sailing Through Plasma Seas: Challenges in Establishing Magnetic Properties." Proceedings of the International Astronomical Union 6, S269 (2010): 58–70. http://dx.doi.org/10.1017/s1743921310007271.

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AbstractJupiter's moons, embedded in the magnetized, flowing plasma of Jupiter's magnetosphere, the plasma seas of the title, are fluids whose highly non-linear interactions imply complex behavior. In a plasma, magnetic fields couple widely separated regions; consequently plasma interactions are exceptionally sensitive to boundary conditions (often ill-specified). Perturbation fields arising from plasma currents greatly limit our ability to establish more than the dominant internal magnetic field of a moon. With a focus on Ganymede and a nod to Io, this paper discusses the complexity of plasma
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2

Szabo, Paul S., Andrew R. Poppe, Andreas Mutzke, Lucas Liuzzo, and Shane R. Carberry Mogan. "Backscattering of Ions Impacting Ganymede’s Surface as a Source for Energetic Neutral Atoms." Astrophysical Journal Letters 963, no. 1 (2024): L32. http://dx.doi.org/10.3847/2041-8213/ad2701.

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Abstract Jupiter’s largest moon Ganymede has its own intrinsic magnetic field, which forms a magnetosphere that is embedded within Jupiter’s corotating magnetospheric plasma. This scenario has been shown to lead to complex ion precipitation patterns that have been connected to heterogeneous space weathering across Ganymede’s surface. We present the first simulations of energetic neutral atoms (ENAs) from backscattered H, O, and S ions, accounting for magnetospheric plasma precipitation and Ganymede’s heterogeneous surface composition. Our model shows that backscattering introduces significant
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3

Popel, Sergey I., and Lev M. Zelenyi. "Dusty plasma interactions near the Moon and in the system of Mars." Proceedings of the International Astronomical Union 14, A30 (2018): 389–90. http://dx.doi.org/10.1017/s1743921319004861.

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4

Xia, Qing, Ming-Hui Cai, Liang-Liang Xu, Rui-Long Han, Tao Yang, and Jian-Wei Han. "Distribution of charged lunar dust in the south polar region of the moon." Chinese Physics B 31, no. 4 (2022): 045201. http://dx.doi.org/10.1088/1674-1056/ac2e61.

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Lunar dust is one of the most threatening problems confronting the return of human beings to the moon. In this work we studied the spatial distribution behavior of charged lunar dust in the solar wind plasma environment in the south polar region of the moon and considered the influence of a mini-crater using Spacecraft Plasma Interactions Software. The distribution of dust and plasma at low solar altitude angles of 20° and 0° was studied, and the spatial density of lunar dust was ∼ 1010.4 m−3 and ∼ 1011.5 m−3, respectively. This is because a higher surface potential will result in transportati
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5

Roussos, E., J. Müller, S. Simon, et al. "Plasma and fields in the wake of Rhea: 3-D hybrid simulation and comparison with Cassini data." Annales Geophysicae 26, no. 3 (2008): 619–37. http://dx.doi.org/10.5194/angeo-26-619-2008.

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Abstract. Rhea's magnetospheric interaction is simulated using a three-dimensional, hybrid plasma simulation code, where ions are treated as particles and electrons as a massless, charge-neutralizing fluid. In consistency with Cassini observations, Rhea is modeled as a plasma absorbing obstacle. This leads to the formation of a plasma wake (cavity) behind the moon. We find that this cavity expands with the ion sound speed along the magnetic field lines, resulting in an extended depletion region north and south of the moon, just a few Rhea radii (RRh) downstream. This is a direct consequence of
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6

Simon, Sven. "An analytical model of sub‐Alfvénic moon‐plasma interactions with application to the hemisphere coupling effect." Journal of Geophysical Research: Space Physics 120, no. 9 (2015): 7209–27. http://dx.doi.org/10.1002/2015ja021529.

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7

Omerbashich, M. "Global coupling mechanism of Sun resonant forcing of Mars, Moon, and Earth seismicity." Journal of Geophysics 65, no. 1 (2023): 1–46. https://doi.org/10.5281/zenodo.8327412.

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Global seismicity on all three solar system bodies with <em>in situ</em> measurements (Earth, Moon, and Mars) is mainly due to the mechanical Rieger resonance (RR) of macroscopic flapping of the solar wind, driven by the well-known P<sub>Rg</sub>=~154-day Rieger period and commonly detected in most heliophysical data types and the interplanetary magnetic field (IMF). Thus, InSight mission marsquakes rates are periodic with P<sub>Rg</sub> as characterized by a very high (≫12) fidelity &Phi;=2.8&middot;10<sup>6</sup> and by being the only &ge;99%-significant spectral peak in the 385.8&ndash;64.3
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8

Carballo, David M., Jennifer Carballo, and Hector Neff. "Formative and Classic Period Obsidian Procurement in Central Mexico: A Compositional Study Using Laser Ablation-Inductively Coupled Plasma-Mass Spectrometry." Latin American Antiquity 18, no. 1 (2007): 27–43. http://dx.doi.org/10.2307/25063084.

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This report presents the results of a compositional study using laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) to examine central Mexican obsidian procurement at four sites dating to the Formative and Classic periods. The study demonstrates LA-ICP-MS to be a highly accurate obsidian sourcing technique, with results that are directly comparable to instrumental neutron activation analysis. It documents a shift circa 600 B.C. in which Middle Formative villages in Tlaxcala began to obtain obsidian almost exclusively from sources located in the Mesa Central, when they had p
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9

Hanley, K. G., Q. McKown, E. M. Cangi, et al. "The Vulcan Mission to Io: Lessons Learned during the 2022 JPL Planetary Science Summer School." Planetary Science Journal 5, no. 7 (2024): 164. http://dx.doi.org/10.3847/psj/ad5841.

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Abstract A mission to Jupiter's moon Io, the most volcanically active body in the solar system, was suggested as a priority for the New Frontiers program in the 2013 Planetary Science Decadal Survey. We present a New Frontiers–class mission concept, Vulcan, that was designed as an educational exercise through the Jet Propulsion Laboratory’s 2022 Planetary Science Summer School. Vulcan would leverage an instrument suite consisting of wide- and narrow-angle cameras, a thermal infrared spectrometer, two fluxgate magnetometers, and ion and electron electrostatic analyzers to conduct the most thoro
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10

Simon, S. "Real-time 3-D hybrid simulation of Titan's plasma interaction during a solar wind excursion." Annales Geophysicae 27, no. 9 (2009): 3349–65. http://dx.doi.org/10.5194/angeo-27-3349-2009.

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Abstract. The plasma environment of Saturn's largest satellite Titan is known to be highly variable. Since Titan's orbit is located within the outer magnetosphere of Saturn, the moon can leave the region dominated by the magnetic field of its parent body in times of high solar wind dynamic pressure and interact with the thermalized magnetosheath plasma or even with the unshocked solar wind. By applying a three-dimensional hybrid simulation code (kinetic description of ions, fluid electrons), we study in real-time the transition that Titan's plasma environment undergoes when the moon leaves Sat
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11

Yan, Tao, Binzheng Zhang, Junjie Chen, et al. "Three-dimensional Magnetohydrodynamic Simulations of Periodic Variations of Ganymede’s Footprint." Astrophysical Journal 965, no. 1 (2024): 82. http://dx.doi.org/10.3847/1538-4357/ad2c8a.

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Abstract Alfvénic power is generated through the interaction between the mini-magnetosphere of Ganymede and the corotating flow of the Jovian plasma, contributing to the formation of the Ganymede auroral footprint at Jupiter’s ionosphere. Using a three-dimensional, high-resolution global magnetohydrodynamic model of the Ganymede magnetosphere, we investigate the temporal variations of the Alfvénic power generated in the mini-magnetosphere of the moon under steady-state upstream conditions. Results show that (1) the Alfvénic power caused by the intermittent magnetic reconnections and the Kelvin
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12

Ambili, K. M., and R. K. Choudhary. "Three-dimensional distribution of ions and electrons in the lunar ionosphere originated from the photochemical reactions." Monthly Notices of the Royal Astronomical Society 510, no. 3 (2021): 3291–300. http://dx.doi.org/10.1093/mnras/stab3734.

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ABSTRACT Using a fluid-based time-dependent numerical photochemical model, the three-dimensional distribution of ions and electrons in the lunar ionosphere, originated purely from photochemical reactions, is investigated. The photochemical model includes the production and recombination of 16 ions, namely CO$_2^+$, H2O+, H3O+, OH+, O$_2^+$, O+, Ar+, Ne+, He+, H+, H$_2^+$, CH$_3^+$, CH$_4^+$, and CH$_5^+$. The model also includes the interaction of solar wind with lunar plasma and calculates electron density profiles from the surface to 200 km altitude for the entire latitudes and longitudes. M
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13

Allegrini, F., F. Bagenal, R. W. Ebert, et al. "Plasma Observations During the 7 June 2021 Ganymede Flyby From the Jovian Auroral Distributions Experiment (JADE) on Juno." Geophysical Research Letters 49 (July 5, 2022): e2022GL098682. https://doi.org/10.1029/2022GL098682.

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On June 7, 2021 the Juno mission came as close as 1046 km from the surface of Ganymede, the largest moon in the solar system. Similar close encounters were previously made by the Galileo mission, from which we learned much of the interaction of the moon, with its own intrinsic magnetic field, and Jupiter&rsquo;s magnetosphere. In this paper, we present an overview of the plasma observations, i.e. ions and electrons in the lower part of the energy spectrum, made by the Jovian Auroral Distributions Experiment (JADE). We find that the ion composition near Ganymede is very different than that from
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14

Izvekova, Yu N., S. I. Popel, and A. P. Golub’. "Nonlinear Dust Acoustic Waves in Exosphere of Mercury." Физика плазмы 49, no. 10 (2023): 1010–15. http://dx.doi.org/10.31857/s0367292123600814.

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The exosphere of Mercury, which has much in common with the exosphere of the Moon, can also contain suspended dust particles, which, under the action of intense solar radiation, acquire positive charges and form one of the components of the dusty plasma system. In addition to dust particles, there are photoelectrons above the planet surface, formed as a result of interaction of solar radiation with the planet surface, as well as with suspended dust particles. Mercury, unlike the Moon, has its own magnetosphere, which affects the parameters of dusty plasma system. The dusty plasma parameters ne
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15

Pohjola, V., and E. Kallio. "On the modeling of planetary plasma environments by a fully kinetic electromagnetic global model HYB-em." Annales Geophysicae 28, no. 3 (2010): 743–51. http://dx.doi.org/10.5194/angeo-28-743-2010.

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Abstract. We have developed a fully kinetic electromagnetic model to study instabilities and waves in planetary plasma environments. In the particle-in-a-cell (PIC) model both ions and electrons are modeled as particles. An important feature of the developed global kinetic model, called HYB-em, compared to other electromagnetic codes is that it is built up on an earlier quasi-neutral hybrid simulation platform called HYB and that it can be used in conjunction with earlier hybrid models. The HYB models have been used during the past ten years to study globally the flowing plasma interaction wit
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16

Lou, Yuequn, Xudong Gu, Xing Cao, et al. "Statistical Analysis of Lunar 1 Hz Waves Using ARTEMIS Observations." Astrophysical Journal 943, no. 1 (2023): 17. http://dx.doi.org/10.3847/1538-4357/aca767.

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Abstract Like 1 Hz waves occurring in the upstream of various celestial bodies in the solar system, 1 Hz narrowband whistler-mode waves are often observed around the Moon. However, wave properties have not been thoroughly investigated, which makes it difficult to proclaim the generation mechanism of the waves. Using 5.5 yr wave data from ARTEMIS, we perform a detailed investigation of 1 Hz waves in the near-lunar space. The amplitude of lunar 1 Hz waves is generally 0.05–0.1 nT. In the geocentric solar ecliptic coordinates, the waves show no significant regional differentiation pattern but sho
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17

Poppe, A. R., and S. Fatemi. "The Solar Wind Interaction with (1) Ceres: The Role of Interior Conductivity." Planetary Science Journal 4, no. 1 (2023): 14. http://dx.doi.org/10.3847/psj/acaf6a.

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Abstract As a potential “ocean world,” (1) Ceres’ interior may possess relatively high electrical conductivities on the order of 10−4–100 S m−1, suggesting that the solar wind interaction with Ceres may differ from other highly resistive objects such as the Moon. Here, we use a hybrid plasma model to quantify the solar wind interaction with Ceres over a range of scenarios for Ceres’ internal conductivity structure and the upstream solar wind and interplanetary magnetic field (IMF) conditions. Internal models for Ceres include one-, two-, and three-layer conductivity structures that variously i
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18

Lorenzini, E. C., D. Curreli, and D. Zanutto. "Exploration of the Galilean Moons using Electrodynamic Tethers for Propellantless Maneuvers and Self-Powering." Proceedings of the International Astronomical Union 6, S269 (2010): 229–33. http://dx.doi.org/10.1017/s1743921310007465.

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AbstractRecent studies have demonstrated the benefits of using electrodynamic tethers (EDT) for the exploration of the inner region of the Jovian system. Intense planetary magnetic field and reasonable environmental plasma density make the electrodynamic interaction of the conductive tether with the plasmasphere strong. The interaction is responsible for a Lorentz force that can be conveniently used for propellantless maneuvers and extraction of electrical power for on board use. Jupiter and the four Galilean Moons represent an exceptional gravitational environment for the study of the orbital
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19

Kleiman, J., S. Horodetsky, V. Issoupov, V. Verba, and D. Artymowicz. "Interaction of Lunar Dust Simulants with Materials: Importance of Charging." IOP Conference Series: Materials Science and Engineering 1328, no. 1 (2025): 012003. https://doi.org/10.1088/1757-899x/1328/1/012003.

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Abstract Materials exposed to lunar regolith dust and other environmental factors on the Moon may suffer permanent damage, risking catastrophic failures. Lunar dust poses the greatest threat. Preventive measures are crucial, with principles emerging to deter dust accumulation in vacuum conditions. Charging of dust and surfaces significantly affects adhesion. Charging sources include photoemission, solar wind, and secondary electron emission from Earth’s magnetosphere, resulting in positive charge on the dayside and negative charge on the nightside. In framework of NASA’s “Regolith Adherence Ch
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20

Rovige, Lucas, Filipe D. Cruz, Robert S. Dorst, et al. "Laboratory Study of Magnetic Reconnection in Lunar-relevant Mini-magnetospheres." Astrophysical Journal 969, no. 2 (2024): 124. http://dx.doi.org/10.3847/1538-4357/ad4fff.

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Abstract Mini-magnetospheres are small ion-scale structures that are well suited to studying kinetic-scale physics of collisionless space plasmas. Such ion-scale magnetospheres can be found on local regions of the Moon, associated with the lunar crustal magnetic field. In this paper, we report on the laboratory experimental study of magnetic reconnection in laser-driven, lunar-like ion-scale magnetospheres on the Large Plasma Device at the University of California, Los Angeles. In the experiment, a high-repetition rate (1 Hz), nanosecond laser is used to drive a fast-moving, collisionless plas
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21

Arridge, C. S., N. Achilleos, and P. Guio. "Electric field variability and classifications of Titan's magnetoplasma environment." Annales Geophysicae 29, no. 7 (2011): 1253–58. http://dx.doi.org/10.5194/angeo-29-1253-2011.

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Abstract. The atmosphere of Saturn's largest moon Titan is driven by photochemistry, charged particle precipitation from Saturn's upstream magnetosphere, and presumably by the diffusion of the magnetospheric field into the outer ionosphere, amongst other processes. Ion pickup, controlled by the upstream convection electric field, plays a role in the loss of this atmosphere. The interaction of Titan with Saturn's magnetosphere results in the formation of a flow-induced magnetosphere. The upstream magnetoplasma environment of Titan is a complex and highly variable system and significant quasi-pe
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22

Tiwari, Sanjiv Kumar. "Are the photospheric sunspots magnetically force-free in nature?" Proceedings of the International Astronomical Union 6, S273 (2010): 333–37. http://dx.doi.org/10.1017/s1743921311015481.

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AbstractIn a force-free magnetic field, there is no interaction of field and the plasma in the surrounding atmosphere i.e., electric currents are aligned with the magnetic field, giving rise to zero Lorentz force. The computation of many magnetic parameters like magnetic energy, gradient of twist of sunspot magnetic fields (computed from the force-free parameter α), including any kind of extrapolations heavily hinge on the force-free approximation of the photospheric magnetic fields. The force-free magnetic behaviour of the photospheric sunspot fields has been examined by Metcalf et al. (1995)
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23

Burne, Sofía, César Bertucci, Nick Sergis, et al. "Space Weather in the Saturn–Titan System." Astrophysical Journal 948, no. 1 (2023): 37. http://dx.doi.org/10.3847/1538-4357/acc738.

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Abstract New evidence based on Cassini magnetic field and plasma data has revealed that the discovery of Titan outside Saturn’s magnetosphere during the T96 flyby on 2013 December 1 was the result of the impact of two consecutive interplanetary coronal mass ejections (ICMEs) that left the Sun in 2013 early November and interacted with the moon and the planet. We study the dynamic evolution of Saturn's magnetopause and bow shock, which evidences a magnetospheric compression from late November 28 to December 4 (at least), under prevailing solar wind dynamic pressures of 0.16–0.3 nPa. During this
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24

V.G, Sapogin, and Sapogin К.V. "Invisible Bubbles with Liquid Wall from Dark Plasma of the Sun§." Advances in Theoretical & Computational Physics 7, no. 4 (2024): 01–18. https://doi.org/10.33140/atcp.07.04.04.

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The article presents fragments of canonical physics of mass particles’ collective interaction. Equations of selfconsistent statics of mass particles and their solutions are given. The integral of "living forces" in plane symmetry is found. It allows to validate the field confinement of matter by a self-consistent field. A pair of forces of field origin, holding the layer in a static equilibrium state, is found - the compression force and the expansion force. The distribution of physical parameters in a flat layer is investigated. The thickness of layer is determined. It coincides with doubled
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25

Ki, Soyoung, Jinhee Kim, Jungtae Na, et al. "Abstract 3227: Developing brain-penetrating MAT2A inhibitors for MTAP-deleted brain metastatic cancer and GBM." Cancer Research 84, no. 6_Supplement (2024): 3227. http://dx.doi.org/10.1158/1538-7445.am2024-3227.

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Abstract Background: Homozygous deletion of MTAP is one of the most frequent genetic alterations in various solid tumors including glioblastoma (GBM), mesothelioma, pancreatic cancer and lung cancer. While MTAP-deleted cancers are associated with a poor prognosis, there are no approved drugs for the treatment of patients with MTAP deficiency. MAT2A has emerged as a potential target for selective anticancer effects in MTAP-deleted cancers. However, development of brain-penetrating MAT2A inhibitors are yet to be reported in preclinical or clinical stages despite of high MTAP deletion fraction in
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26

Choi, Jaeyul, Wongi Park, Soye Jeon, et al. "Abstract LB429: Discovery of a novel SOS1-KRASmulti inhibitor, HM101207, demonstrates a broad-spectrum antitumor activity across KRAS-MAPK mutant cancers." Cancer Research 85, no. 8_Supplement_2 (2025): LB429. https://doi.org/10.1158/1538-7445.am2025-lb429.

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Abstract The RAS subfamily is a well-known oncogene with the highest mutation rate and poor prognosis among various cancers. Among the RAS subfamily, KRAS is the most frequent mutation isoform, especially with a prevalence of approximately 35%∼90% in NSCLC, CRC, and PDAC. KRAS protein cycles between "off" (inactive) and "on" (active) states induce downstream signal transduction to promote cell proliferation and survival. Son of sevenless homolog 1 (SOS1) is one of guanine nucleotide exchange factor (GEF) responsible for a binary molecular switch to activate KRAS as well as a node in the negati
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27

Holmstrom, Mats, Mark Lester, and Beatriz Sanchez-Cano. "Future opportunities in solar system plasma science through ESA’s exploration programme." npj Microgravity 10, no. 1 (2024). http://dx.doi.org/10.1038/s41526-024-00373-9.

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AbstractThe solar wind interacts with all solar system bodies, inducing different types of dynamics depending on their atmospheric and magnetic environments. We here outline some key open scientific questions related to this interaction, with a focus on the Moon and Mars, that may be addressed by future Mars and Moon missions by the European Space Agency’s Human and Robotic Exploration programme. We describe possible studies of plasma interactions with bodies with and without an atmosphere, using multi-point and remote measurements, and energetic particle observations, as well as recommend som
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28

Tolba, R. E., W. M. Moslem, and R. Sabry. "Modulated dust-ion-acoustic waves result from Earth's magnetosphere and lunar ionosphere interactions." Physics of Fluids 36, no. 3 (2024). http://dx.doi.org/10.1063/5.0198213.

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The Earth's magnetosphere's modulational amplitude dust-ion-acoustic waves are studied. When the moon passes through the Earth's magnetotail, its dust grains may interact, causing these waves. The theoretical plasma model for this study includes positive ionospheric ion fluids, isothermal electrons, and fluid-negative dust grains on the moon. A perturbation technique derived the nonlinear Schrödinger equation, which exhibited dispersion and nonlinear effects. The nonlinear and dispersion term coefficients' polarity may predict stable and unstable pulse domains. A numerical study was performed
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Yang, Fan, Xu‐Zhi Zhou, Ying Liu, et al. "Revisiting Discrete Energy Bands in Galilean Moon's Footprint Tails: Remote Signals of Particle Absorption." Geophysical Research Letters 52, no. 14 (2025). https://doi.org/10.1029/2024gl112240.

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AbstractObservations from the Juno spacecraft near the M‐shells of the Galilean moons have identified alternating enhancements and reductions of particle fluxes at discrete energies. These banded structures were previously attributed to bounce resonance between particles and standing Alfvén waves generated by moon‐magnetospheric interactions. Here, we show that this explanation is inconsistent with key observational features, and propose an alternative interpretation: the bands are remote signatures of particle absorption at the moons. In this scenario, whether a particle encounters the moon b
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30

Xiao, Chao, Fei He, Quanqi Shi, et al. "Evidence for lunar tide effects in Earth’s plasmasphere." Nature Physics, January 26, 2023. http://dx.doi.org/10.1038/s41567-022-01882-8.

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AbstractTides are universal and affect spatially distributed systems, ranging from planetary to galactic scales. In the Earth–Moon system, effects caused by lunar tides were reported in the Earth’s crust, oceans, neutral gas-dominated atmosphere (including the ionosphere) and near-ground geomagnetic field. However, whether a lunar tide effect exists in the plasma-dominated regions has not been explored yet. Here we show evidence of a lunar tide-induced signal in the plasmasphere, the inner region of the magnetosphere, which is filled with cold plasma. We obtain these results by analysing varia
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31

An, Xin, Vassilis Angelopoulos, Terry Z. Liu, Anton Artemyev, Andrew R. Poppe, and Donglai Ma. "Plasma Refilling of the Lunar Wake: Plasma‐Vacuum Interactions, Electrostatic Shocks, and Electromagnetic Instabilities." Journal of Geophysical Research: Space Physics 130, no. 7 (2025). https://doi.org/10.1029/2025ja034205.

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AbstractA plasma void forms downstream of the Moon when the solar wind impacts the lunar surface. This void gradually refills as the solar wind passes by, forming the lunar wake. We investigate this refilling process using a fully kinetic particle‐in‐cell (PIC) simulation. The early stage of refilling follows plasma‐vacuum interaction theory, characterized by exponential decay of plasma density into the wake, along with ion acceleration and cooling in the expansion direction. Our PIC simulation confirms these theoretical predictions. In the next stage of the refilling process, the counter‐stre
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32

Nerney, Edward G. "Diffusive Equilibrium: Modeling Anisotropic Maxwellian and Kappa Field Line Distributions in Io's Plasma Torus Using Multi‐Fluid and Kinetic Approaches." Journal of Geophysical Research: Space Physics 130, no. 7 (2025). https://doi.org/10.1029/2024ja033582.

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AbstractModeling density distributions along Jupiter's magnetic field lines is essential for understanding the Io plasma torus, moon plasma interactions, and plasma throughout the magnetosphere. This study compares multi‐fluid and kinetic approaches to diffusive equilibrium and the effects of different plasma distribution functions and anisotropy. We establish a nominal equatorial centrifugal radial model of plasma densities and temperatures in the Io plasma torus (5–10 ) and define six cases representing combinations of distribution functions (Maxwellian, standard Kappa, product Kappa, and “F
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Rabia, J., V. Hue, N. André, et al. "Properties of Electrons Accelerated by the Ganymede‐Magnetosphere Interaction: Survey of Juno High‐Latitude Observations." Journal of Geophysical Research: Space Physics 129, no. 5 (2024). http://dx.doi.org/10.1029/2024ja032604.

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AbstractThe encounter between the Jovian co‐rotating plasma and Ganymede gives rise to electromagnetic waves that propagate along the magnetic field lines and accelerate particles by resonant or non‐resonant wave‐particle interaction. They ultimately precipitate into Jupiter's atmosphere and trigger auroral emissions. In this study, we use Juno/JADE, Juno/UVS data, and magnetic field line tracing to characterize the properties of electrons accelerated by the Ganymede‐magnetosphere interaction in the far‐field region. We show that the precipitating energy flux exhibits an exponential decay as a
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34

Haynes, C. Michael, Tyler Tippens, Peter Addison, Lucas Liuzzo, Andrew R. Poppe, and Sven Simon. "Emission of Energetic Neutral Atoms From the Magnetosphere‐Atmosphere Interactions at Callisto and Europa." Journal of Geophysical Research: Space Physics 128, no. 10 (2023). http://dx.doi.org/10.1029/2023ja031931.

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AbstractWe analyze the emission of energetic neutral atom (ENA) flux from charge exchange between Jovian magnetospheric ions and the atmospheres of Callisto and Europa. For this purpose, we combine the draped electromagnetic fields from a hybrid plasma model with a particle tracing tool for the energetic ions. We determine the ENA flux through a concentric sphere located just outside of each moon's atmosphere, thereby capturing the complete physics imprinted in these emission patterns. In order to constrain the modifications to the ENA emissions that arise from the periodic change of the ambie
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35

Li Meng-Yao, Xia Qing, Cai Ming-Hui, et al. "Characteristic research of dust and plasma environment in the lunar south pole." Acta Physica Sinica, 2024, 0. http://dx.doi.org/10.7498/aps.73.20240599.

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Unlike the Earth, the Moon lacks the protection of an atmosphere and a global magnetic field, and is directly exposed to complex radiation environments such as high-energy cosmic rays, solar wind, and the Earth's magnetotail plasma. The surface of the Moon is covered with a thick layer of lunar soil, of which particles with a size of 30nm-20&lt;i&gt;μ&lt;/i&gt;m are called lunar dust. In complex environments such as solar wind or magnetotail plasma, lunar dust carries an electric charge and becomes charged lunar dust. Charged lunar dust is prone to migration under the action of the electric fi
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36

Biswas, Ayan, Barnali Das, Poonam Chandra та ін. "Discovery of Magnetospheric Interactions in the Doubly-Magnetic Hot Binary ε Lupi". Monthly Notices of the Royal Astronomical Society, 13 червня 2023. http://dx.doi.org/10.1093/mnras/stad1756.

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Abstract Magnetic fields are extremely rare in close, hot binaries, with only 1.5% of such systems known to contain a magnetic star. The eccentric ε Lupi system stands out in this population as the only close binary in which both stars are known to be magnetic. We report the discovery of strong, variable radio emission from ε Lupi using the upgraded Giant Metrewave Radio Telescope (uGMRT) and the MeerKAT radio telescope. The light curve exhibits striking, unique characteristics including sharp, high-amplitude pulses that repeat with the orbital period, with the brightest enhancement occurring
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37

Paranicas, C., B. H. Mauk, G. Clark, et al. "Energetic Charged Particle Measurements During Juno's Two Close Io Flybys." Geophysical Research Letters 51, no. 13 (2024). http://dx.doi.org/10.1029/2024gl109495.

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AbstractOn days 2023‐364 and 2024‐034, the Juno spacecraft made close passages of Jupiter's moon Io, at altitudes of about 1,500 km. Data obtained from the first flyby, when the spacecraft was on magnetic field lines connected to both Jupiter and Io, revealed deep flux decreases. In addition, Juno's energetic particle detectors observed tens to hundreds of keV electron and proton beams. Such beams could be generated near Jupiter on field lines associated with Io. The second encounter occurred in the plasma wake and a more modest flux decrease was observed. Furthermore, data from both encounter
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38

Nishino, Masaki N., Yoshiya Kasahara, Yuki Harada, et al. "An event study on broadband electric field noises and electron distributions in the lunar wake boundary." Earth, Planets and Space 74, no. 1 (2022). http://dx.doi.org/10.1186/s40623-021-01566-2.

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AbstractWave–particle interactions are fundamental processes in space plasma, and some plasma waves, including electrostatic solitary waves (ESWs), are recognised as broadband noises (BBNs) in the electric field spectral data. Spacecraft observations in recent decades have detected BBNs around the Moon, but the generation mechanism of the BBNs is not fully understood. Here, we study a wake boundary traversal with BBNs observed by Kaguya, which includes an ESW event previously reported by Hashimoto et al. Geophys Res Lett 37:L19204 10.1029/2010GL044529 (2010). Focusing on the relation between B
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39

Futaana, Yoshifumi, Esa Kallio, Olli Knuuttila, Leo Nyman, Manabu Shimoyama, and Stas Barabash. "The LimPa mission: a small mission proposal to characterize the enigmatic lunar dust exosphere." Earth, Planets and Space 76, no. 1 (2024). https://doi.org/10.1186/s40623-024-02106-4.

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AbstractThe lunar environment is known to be characterized by complex interactions between plasma, the exosphere, dust, and the surface. However, our understanding of the environment is limited due to the lack of experimental evidence. Here, we propose a small, low-cost mission to characterize the dust and exosphere environment of the Moon. Named the Limb Pathfinder (LimPa), this is a proof-of-concept mission aimed toward understanding the coupling between plasma, dust, and tenuous neutral atmosphere. The LimPa mission was proposed to a call for the Small Mission to the Moon issued by European
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40

C., Michael Haynes, Tippens Tyler, Addison Peter, Liuzzo Lucas, R. Poppe Andrew, and Simon Sven. "Emission of Energetic Neutral Atoms from the Magnetosphere-Atmosphere Interactions at Callisto and Europa." July 14, 2023. https://doi.org/10.5281/zenodo.8148611.

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Accompanying data products for publication entitled &quot;Emission of Energetic Neutral Atoms from the Magnetosphere-Atmosphere Interactions at Callisto and Europa&quot;. The article was submitted shortly after the date of upload. Data includes all simulation outputs for both the AIKEF hybrid model and the ENA production model. Information regarding the organization and file structure can be found in haynes_paper1_zenodo/info.txt , and any inquiries shall be addressed through the email associated with this data publication.
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41

Cohen, Ian J., Evan J. Smith, George B. Clark, et al. "Plasma Environment, Radiation, Structure, and Evolution of the Uranian System (PERSEUS): A Dedicated Orbiter Mission Concept to Study Space Physics at Uranus." Space Science Reviews 219, no. 8 (2023). http://dx.doi.org/10.1007/s11214-023-01013-6.

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AbstractThe Plasma Environment, Radiation, Structure, and Evolution of the Uranian System (PERSEUS) mission concept defines the feasibility and potential scope of a dedicated, standalone Heliophysics orbiter mission to study multiple space physics science objectives at Uranus. Uranus’s complex and dynamic magnetosphere presents a unique laboratory to study magnetospheric physics as well as its coupling to the solar wind and the planet’s atmosphere, satellites, and rings. From the planet’s tilted and offset, rapidly-rotating non-dipolar magnetic field to its seasonally-extreme interactions with
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42

Addison, Peter, Lucas Liuzzo, Hannes Arnold, and Sven Simon. "Influence of Europa's Time-Varying Electromagnetic Environment on Magnetospheric Ion Precipitation." December 9, 2020. https://doi.org/10.5281/zenodo.4313883.

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Data for the manuscript &quot;Influence of Europa&#39;s Time-Varying Electromagnetic Environment on Magnetospheric Ion Precipitation&quot; by Addison et al., (2021). See README.txt for a description of the data files included here.
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43

Aaron, Stahl, Addison Peter, Liuzzo Lucas, and Simon Sven. "Data for "Modeling of Ganymede's Magnetic and Plasma Environment During the Juno PJ34 Flyby" by Stahl et al. (2024)." September 13, 2023. https://doi.org/10.5281/zenodo.8326069.

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Data repository for the study entitled &quot;Modeling of Ganymede&#39;s Magnetic and Plasma Environment During the Juno PJ34 Flyby&quot; by Stahl et al. (2024). Information on file structure and contents can be found in the file: readme.txt. Please email corresponding author for questions regarding the manuscript or data: astahl3@gatech.edu (Aaron Stahl).
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44

Aaron, Stahl, Addison Peter, Simon Sven, and Liuzzo Lucas. "Data for "Modeling of Ganymede's Magnetic and Plasma Environment During the Juno PJ34 Flyby" by Stahl et al. (2023)." September 22, 2023. https://doi.org/10.5281/zenodo.8370898.

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Data repository for the study entitled &quot;Modeling of Ganymede&#39;s Magnetic and Plasma Environment During the Juno PJ34 Flyby&quot; by Stahl et al. (2024). Information on file structure and contents can be found in the file: readme.txt. Please email corresponding author for questions regarding the manuscript or data: astahl3@gatech.edu (Aaron Stahl).
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45

Crucian, Brian E., Heather Quiriarte, Chiu-wing Lam, et al. "Pulmonary and systemic immune alterations in rats exposed to airborne lunar dust." Frontiers in Immunology 16 (February 6, 2025). https://doi.org/10.3389/fimmu.2025.1538421.

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BackgroundDue to cosmic radiation bombardment and over 4 billion meteorite and micrometeoroid impacts on the airless Moon, the lunar surface is covered by a layer of fine, reactive dust. Very little is known regarding the toxicity of lunar dust on human physiology. This study assessed airborne lunar dust exposure in rats on localized pulmonary and systemic immune parameters.MethodsRats were exposed to 0 (air only), 20.8 (low), and 60.6 (high) mg/m3 of respirable-size lunar dust for 4 weeks (6 h/day, 5 days/week). Rats were then euthanized either 1 day, 7 days, 4 weeks, or 13 weeks after the la
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46

Sucerquia, Mario, Jaime A. Alvarado-Montes, Jorge I. Zuluaga, Nicolás Cuello, Jorge Cuadra, and Matías Montesinos. "The missing rings around Solar System moons." Astronomy & Astrophysics, October 4, 2024. http://dx.doi.org/10.1051/0004-6361/202449453.

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Rings are complex structures that surround various bodies within the Solar System, such as giant planets and certain minor bodies. While some formation mechanisms could also potentially promote their existence around (regular or irregular) satellites, none of these bodies currently bear these structures. We aim to understand the underlying mechanisms that govern the potential formation, stability, and/or decay of hypothetical circumsatellital rings (CSRs) orbiting the largest moons in the Solar System. This extends to the exploration of short-term morphological features within these rings, pro
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47

Bockelee-Morvan, Dominique, Olivier Poch, Francois Leblanc, et al. "A patchy CO_2 exosphere on Ganymede revealed by the James Webb Space Telescope." Astronomy & Astrophysics, September 30, 2024. http://dx.doi.org/10.1051/0004-6361/202451599.

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Jupiter's icy moon Ganymede has a tenuous exosphere produced by sputtering and possibly sublimation of water ice. To date, only atomic hydrogen and oxygen have been directly detected in this exosphere. Here, we present observations of Ganymede's CO$_2$ exosphere obtained with the James Webb Space Telescope. CO$_2$ gas is observed over different terrain types, mainly over those exposed to intense Jovian plasma irradiation, as well as over some bright or dark terrains. Despite warm surface temperatures, the CO$_2$ abundance over equatorial subsolar regions is low. CO$_2$ vapor has the highest ab
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48

Rush, Tomás A., Ann M. Wymore, Miguel Rodríguez, Jr, et al. "Fungal elemental profiling unleashed through rapid laser-induced breakdown spectroscopy (LIBS)." mSystems, August 27, 2024. http://dx.doi.org/10.1128/msystems.00919-24.

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ABSTRACT Elemental profiling of fungal species as a phenotyping tool is an understudied topic and is typically performed to examine plant tissue or non-biological materials. Traditional analytical techniques such as inductively coupled plasma–optical emission spectroscopy (ICP-OES) and inductively coupled plasma–mass spectrometry (ICP-MS) have been used to identify elemental profiles of fungi; however, these techniques can be cumbersome due to the difficulty of preparing samples. Additionally, the instruments used for these techniques can be expensive to procure and operate. Laser-induced brea
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49

Kato, Masahisa, Yuki Harada, Yoshifumi Saito, et al. "Inhomogeneous Electrostatic Potentials on the Dayside Lunar Surface in the Terrestrial Magnetotail Lobes: The Role of Lunar Crustal Magnetic Fields." Journal of Geophysical Research: Space Physics 130, no. 2 (2025). https://doi.org/10.1029/2024ja033545.

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AbstractThough the Moon does not possess a global magnetic field like the Earth, there are localized crustal magnetic fields on the lunar surface. Because of the plasma interaction with the crustal magnetic fields, electrostatic and electromagnetic environments near magnetized regions can differ from those near non‐magnetized regions on the Moon. Previous studies observationally revealed the difference in the electrostatic potential on the lunar surface between magnetized and non‐magnetized regions of the Moon in the solar wind, which was attributed to upward electric fields formed by electron
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50

Jia, Xianzhe, Margaret G. Kivelson, Krishan K. Khurana, and Raymond J. Walker. "Improved Models of Ganymede's Permanent and Induced Magnetic Fields Based on Galileo and Juno Data." Journal of Geophysical Research: Planets 130, no. 1 (2024). https://doi.org/10.1029/2024je008309.

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AbstractNear Ganymede, the magnetic field is a superposition of Jupiter's magnetospheric magnetic field, the field arising from sources within the moon, the field generated by plasma currents driven by the interaction of flowing magnetospheric plasma with the conducting moon, and the field arising from ionospheric currents. Previous fits to Ganymede's internal field have not identified the contributions of plasma and ionospheric currents, although their contributions can obscure the signature of sources internal to the moon. Fortunately, using magnetohydrodynamic simulations whose output agree
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