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1 rules during the first five million years of planetary accretion to explain their observed abundance.
4 data to document the Arctic-wide decrease in planetary albedo and its amplifying effect on the warmin
5 ysis reveals a striking relationship between planetary albedo and sea ice cover, quantities inferred
7 Wind tunnel data collected under ambient and planetary-analogue conditions inform our models of aeoli
13 ly 250 parts per million) indicates that the planetary atmosphere is predominantly clear down to an a
15 ronments such as the interstellar medium and planetary atmospheres (CN, SiN and C2H), and combustion
20 to's atmosphere is unique among Solar System planetary atmospheres, as its radiative energy equilibri
21 conditions consistent with extraterrestrial planetary atmospheres, that ammonia forms clathrate hydr
25 tion the imaging of motion patterns inside a planetary ball mill from simulations and video recording
29 during the last few years the application of planetary ball mills has extended to mechanochemical app
30 delines to follow for modelling processes in planetary ball mills in terms of refinement, synthesis'
34 ned a major role as antifreeze in giving icy planetary bodies (e.g., Titan) a liquid subsurface ocean
35 re essential for scientific investigation of planetary bodies and are therefore ubiquitous on mission
37 substantial process during crustal growth on planetary bodies and well documented to have occurred in
38 achyandesites on Earth, also formed on small planetary bodies approximately 4.56 billion years ago.
39 n whether the notable volatile depletions of planetary bodies are a consequence of accretion or inher
40 cognized that Earth and other differentiated planetary bodies are chemically fractionated compared to
43 tem, the molten metallic cores of many small planetary bodies convected vigorously and were capable o
44 e nature and extent of volatile-depletion of planetary bodies during the earliest stages of Solar Sys
47 ng of reduced carbon from Fe-rich basalts on planetary bodies would produce methane-bearing, CO-rich
48 a major contributor of volatile elements to planetary bodies, and could have played a key role in th
49 ces of the major elements of Earth and other planetary bodies, are a natural consequence of substanti
50 is critical for modeling collisions between planetary bodies, interpreting the significance of shock
53 istory has implications for the formation of planetary bodies, the delivery of water to the inner Sol
63 and isotopic signatures compared with other planetary bodies; any successful model for the origin of
65 their source, for the first time across any planetary body, creating a novel way to probe planetary
70 ve climate policies that comply with the two planetary boundaries related to climate change: (1) stay
75 cosystem services, environmental footprints, planetary boundaries, human-nature nexuses, and telecoup
78 cal ecosystems--beyond its recently proposed planetary boundary across 58.1% of the world's land surf
81 ion planetary boundary, but rather that many planetary boundary issues governed by chemical pollution
93 ays after contact of the air masses with the planetary boundary layer; this is related to the time ne
96 tly available to identify chemicals that are planetary boundary threats is prioritization against pro
97 e that there is no single chemical pollution planetary boundary, but rather that many planetary bound
100 cycling rate of local moisture, regulated by planetary circulation patterns associated with the El Ni
102 Modeling studies of terrestrial extrasolar planetary climates are now including the effects of ocea
103 ne that formed Imbrium, should have survived planetary collisions and contributed to the heavy impact
104 voking Kozai-Lidov oscillations, an external planetary companion drives a planet onto an orbit having
108 e mass distribution, chemical abundances and planetary configuration of the Solar System today, but t
113 is commonly found in astrophysics (e.g., in planetary cores) as well as in high energy density physi
117 here with heat recirculation confined to the planetary dayside, or a planet devoid of atmosphere with
118 span a wide range of terrestrial, marine and planetary depositional systems, we show that the advecti
121 Accurate (182)Hf-(182)W chronology of early planetary differentiation relies on highly precise and a
123 of gas can naturally be produced by a proto-planetary disc surrounding a low-mass star, which was sc
124 tic centre, and that tidal debris from proto-planetary discs can flag low-mass stars, which are other
125 m the dynamical evolution of idealized proto-planetary disks under perturbations from massive distant
130 impact of the three greenhouse gases on the planetary energy budget, with a best estimate (in petagr
132 lability of meteoritic organic materials for planetary environments than previously assumed and that
135 e exploration missions (i.e., Venus &Jupiter planetary exploration, and heliophysics missions) and ea
136 tudy of a wide range of phenomena, including planetary formation and asteroid impact sites, the forma
137 e in some of the most enigmatic processes of planetary formation by mediating the rapid accretion of
138 ry disk, would constrain a critical phase of planetary formation by unveiling the unknown planetesima
141 nd characteristic spectral features from the planetary geological surface and subsurface which are de
142 are powerful indicators of a wide variety of planetary geophysical processes, and for Mars they revea
143 several overarching themes that emerge from planetary health and suggest advances in the way we trai
145 s the contribution of continental growth and planetary hydrogen loss to the secular evolution of hydr
146 ns during haze episodes would have expedited planetary hydrogen loss, with a single episode of haze d
150 e study of the evolution and dynamics of the planetary interiors as well as to the fundamental unders
151 d determining its origin and distribution in planetary interiors has important implications for under
152 ctive generation of magnetic fields in fluid planetary interiors is known as the dynamo process.
154 ties and compressibility of, e.g., fluids in planetary interiors, and is a prerequisite for the prepa
155 anding Warm Dense Matter (WDM), the state of planetary interiors, is a new frontier in scientific res
161 nstrumental suites on robotic spacecraft and planetary landers; this necessitates robust and reliable
162 ge terrestrial planets with implications for planetary magnetic-field generation in silicate magma la
165 h a millisecond pulsar, a white dwarf, and a planetary-mass object in an orbit of several decades), s
168 ied by the observed transit times permit the planetary masses to be measured, which is key to determi
169 provide precise, but complex, constraints on planetary masses, densities, and orbits, even for planet
170 havior of carbon dioxide (CO2), an important planetary material found in Venus, Earth, and Mars, is v
171 identifying multi-stage events from complex planetary materials is highly challenging at the length
173 substantial mixing through processes such as planetary migration and the subsequent dynamical process
174 t Jupiters') can largely be accounted for by planetary migration associated with viscous evolution of
176 rrectly infers the phase space structure for planetary motion, avoids overfitting in a biological sig
178 e and cost-effective measures to avoid these planetary nitrogen burdens and the necessity to remediat
181 at the stellar spin axis and the axis of the planetary orbit coincide, the minimum spectroscopic mass
184 e degree of coplanarity and proximity of the planetary orbits imply energy dissipation near the end o
185 for misalignment-driven mechanisms to modify planetary orbits, and that these conditions are present
186 guaranteed: dynamical interactions may tilt planetary orbits, or stars may be misaligned with the pr
187 cts to realign the stellar spin axis and the planetary orbits, the fraction of planetary systems (inc
189 re haze development played a pivotal role in planetary oxidation, hastening the contingent biological
190 gest that most fluid compounds, e.g., strong planetary oxides, reach a common state on the universal
191 iety of non-trivial structures attributed to planetary perturbations and used to constrain the proper
195 bservational constraint is available for the planetary population surrounding ultracool dwarfs, of wh
198 sition of Earth's mantle control fundamental planetary properties, including the vigor of mantle conv
202 We find that the difference between the planetary radius measured at optical and infrared wavele
205 heir dust streams are regular occurrences in planetary rings, altering them in ways that remain detec
206 topic fractionation during volatilization in planetary rocks, but is hardly fractionated during terre
207 e dominated by the controlling influences of planetary rotation and magnetic fields through the Corio
209 the Earth's system are intricately linked to planetary scale processes, and precise characterization
211 China but highlight the fundamental role of planetary-scale atmospheric dynamics in the sensitivity
212 n react in the same way and is approaching a planetary-scale critical transition as a result of human
215 or the generation of persistent longitudinal planetary-scale high-amplitude patterns of the atmospher
217 tion is dominated by beat patterns caused by planetary-scale wave pairs and by a small number of brig
218 ara seas, enhances the upward propagation of planetary-scale waves with wavenumbers of 1 and 2, subse
224 s, and a prominent goal in geomorphology and planetary science is to determine formation processes fr
230 rent interest for warm dense matter physics, planetary sciences, and inertial fusion energy research.
231 on-hydrogen system is of great importance to planetary sciences, as hydrocarbons comprise a significa
232 roblems across many disciplines in earth and planetary sciences, including paleoclimatology, sediment
233 rity, we integrate the physical insight from planetary sciences, the liquid marble model from fluid m
238 The low-degree gravity field, combined with planetary spin parameters, yields the moment of inertia
243 ns terrestrial life and consists of the thin planetary surface layer between unaltered rock and the a
244 ives of environmental conditions and ancient planetary surface processes that led to their formation.
245 ersal palaeohydraulic reconstruction tool on planetary surfaces and allow for quantitative identifica
246 nderstanding the ways in which floods modify planetary surfaces, the hydrology of early Mars and abru
247 formation in heterogeneous thin films or on planetary surfaces-have been characterized experimentall
249 live in urban areas, a critical question for planetary sustainability is how the size of cities affec
252 solar system are merely possible outcomes of planetary system formation and evolution, and conceivabl
256 show that the solar nebula that spawned our planetary system was rich in water and organic molecules
257 moons with Kepler (HEK) project, we report a planetary system with two confirmed planets and one cand
261 is and the planetary orbits, the fraction of planetary systems (including systems of 'hot Neptunes' a
263 sent yet another new and unexpected class of planetary systems and provide an opportunity to test the
268 e differences between hot Jupiters and other planetary systems denote a distinctly different formatio
270 t the typical characteristics of planets and planetary systems for planets with sizes as small as, an
274 Accounting for detection efficiency, such planetary systems occur with a frequency similar to the
275 dwarfs, suggests that rocky debris from the planetary systems of white-dwarf progenitors occasionall
276 tside it, despite models of the formation of planetary systems suggesting that orbital migration of g
280 sently, we have limited knowledge about such planetary systems, mostly about their sizes and orbital
281 dd an important constraint on simulations of planetary systems, since they must be able to reproduce
293 global topography is more subdued, allowing planetary temperatures to vary depending on the global d
295 ons of the Rossiter-McLaughlin effect during planetary transits have revealed that a considerable fra
298 her show that resonance conditions for these planetary waves were, in many cases, present before the
299 highly magnified quasistationary midlatitude planetary waves with zonal wave numbers m = 6, 7, and 8.
300 tant role of the QRA mechanism in amplifying planetary waves, favoring recent NH weather extremes.
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