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1 rules during the first five million years of planetary accretion to explain their observed abundance.
4 pogenic aerosols are hypothesized to enhance planetary albedo and offset some of the warming due to t
5 ysis reveals a striking relationship between planetary albedo and sea ice cover, quantities inferred
7 igible, we find direct evidence of increased planetary albedo primarily through increased drop concen
9 Wind tunnel data collected under ambient and planetary-analogue conditions inform our models of aeoli
13 electron spectrometers that can be used for planetary and space science missions to environments of
17 ly 250 parts per million) indicates that the planetary atmosphere is predominantly clear down to an a
20 ronments such as the interstellar medium and planetary atmospheres (CN, SiN and C2H), and combustion
23 to's atmosphere is unique among Solar System planetary atmospheres, as its radiative energy equilibri
27 re essential for scientific investigation of planetary bodies and are therefore ubiquitous on mission
29 substantial process during crustal growth on planetary bodies and well documented to have occurred in
30 n whether the notable volatile depletions of planetary bodies are a consequence of accretion or inher
31 cognized that Earth and other differentiated planetary bodies are chemically fractionated compared to
34 tem, the molten metallic cores of many small planetary bodies convected vigorously and were capable o
35 u evidence of impacts on boulders on airless planetary bodies has come from Apollo lunar samples(6) a
38 gnetic data(9), and especially in studies of planetary bodies that no longer have a dynamo(10), such
39 a major contributor of volatile elements to planetary bodies, and could have played a key role in th
40 ces of the major elements of Earth and other planetary bodies, are a natural consequence of substanti
41 one of the most fundamental constituents in planetary bodies, being an essential building block of m
42 is critical for modeling collisions between planetary bodies, interpreting the significance of shock
51 and isotopic signatures compared with other planetary bodies; any successful model for the origin of
52 differentiation of a carbonaceous chondritic planetary body, bridging a previously persistent gap in
53 their source, for the first time across any planetary body, creating a novel way to probe planetary
54 ation at static pressures >20 GPa in a large planetary body, like diamonds formed deep within Earth's
56 , five food-related per capita environmental planetary boundaries (carbon emissions, water, land, nit
57 n B12, vitamin E, and saturated fats and the planetary boundaries for carbon emissions and nitrogen a
61 ve climate policies that comply with the two planetary boundaries related to climate change: (1) stay
64 l pollution has been mentioned as one of the planetary boundaries within which humanity can safely op
66 cosystem services, environmental footprints, planetary boundaries, human-nature nexuses, and telecoup
67 eatening to push the Earth system beyond its planetary boundaries, risking catastrophic and irreversi
71 cal ecosystems--beyond its recently proposed planetary boundary across 58.1% of the world's land surf
82 bution of the HDO/H(2)O ratio (D/H) from the planetary boundary layer up to an altitude of 80 kilomet
86 ays after contact of the air masses with the planetary boundary layer; this is related to the time ne
87 cycling rate of local moisture, regulated by planetary circulation patterns associated with the El Ni
88 Modeling studies of terrestrial extrasolar planetary climates are now including the effects of ocea
89 ne that formed Imbrium, should have survived planetary collisions and contributed to the heavy impact
90 voking Kozai-Lidov oscillations, an external planetary companion drives a planet onto an orbit having
91 e mass distribution, chemical abundances and planetary configuration of the Solar System today, but t
93 ng metal-silicate partitioning (analogous to planetary core formation) over a large range of oxygen f
95 ty and length scale-are poorly quantified in planetary cores owing to the strong dependence of these
96 Although modelling the conditions of larger planetary cores remains out of reach, the fact that the
98 is commonly found in astrophysics (e.g., in planetary cores) as well as in high energy density physi
100 gm involves the growth of a relatively mafic planetary crust over the first 1 to 2 billion years of E
103 here with heat recirculation confined to the planetary dayside, or a planet devoid of atmosphere with
104 ition of this disk is unlike all other known planetary debris around white dwarfs(7), but resembles p
107 Accurate (182)Hf-(182)W chronology of early planetary differentiation relies on highly precise and a
114 -on collision (giant impact) between a large planetary embryo and the proto-Jupiter could have shatte
115 The acquisition of nebular gases requires planetary embryos to grow to sufficiently large mass bef
116 impact of the three greenhouse gases on the planetary energy budget, with a best estimate (in petagr
119 year between 1991 and 2016, equivalent to a planetary energy imbalance of 0.80 +/- 0.49 W watts per
124 e exploration missions (i.e., Venus &Jupiter planetary exploration, and heliophysics missions) and ea
127 tudy of a wide range of phenomena, including planetary formation and asteroid impact sites, the forma
128 ry disk, would constrain a critical phase of planetary formation by unveiling the unknown planetesima
132 in ureilite meteorites is a timely topic in planetary geology as recent studies have proposed their
133 rent diets are detrimental to both human and planetary health and shifting towards more balanced, pre
134 several overarching themes that emerge from planetary health and suggest advances in the way we trai
135 iverse natural environments are dependent on planetary health, which should be a priority also among
138 Earth's mantle convection, which facilitates planetary heat loss, is manifested at the surface as pre
140 ns during haze episodes would have expedited planetary hydrogen loss, with a single episode of haze d
148 ctive generation of magnetic fields in fluid planetary interiors is known as the dynamo process.
149 Evidence for the capture of nebular gases by planetary interiors would place important constraints on
150 ties and compressibility of, e.g., fluids in planetary interiors, and is a prerequisite for the prepa
151 mixture at the high-pressure environment of planetary interiors, in particular, for non-crystalline
152 anding Warm Dense Matter (WDM), the state of planetary interiors, is a new frontier in scientific res
158 ge terrestrial planets with implications for planetary magnetic-field generation in silicate magma la
161 osition of atmospheres while factors such as planetary mass, thermal state, and age mainly affect the
163 d as evidence of planet formation(1-3), with planetary-mass bodies carving rings and gaps in the disk
166 ied by the observed transit times permit the planetary masses to be measured, which is key to determi
168 identifying multi-stage events from complex planetary materials is highly challenging at the length
169 n carbonaceous chondrites and differentiated planetary materials, suggesting the existence, perhaps e
174 rrectly infers the phase space structure for planetary motion, avoids overfitting in a biological sig
175 giant branch (AGB) star into a nonspherical planetary nebula (PN) could be due to binary interaction
179 e and cost-effective measures to avoid these planetary nitrogen burdens and the necessity to remediat
186 discrete field theory from a set of data of planetary orbits similar to what Kepler inherited from T
187 e serving algorithm correctly predicts other planetary orbits, including parabolic and hyperbolic esc
188 rometer (FIPS), which detected heavy ions of planetary origin that were recently ionized, and "picked
191 re haze development played a pivotal role in planetary oxidation, hastening the contingent biological
192 gest that most fluid compounds, e.g., strong planetary oxides, reach a common state on the universal
193 led C-P-O-Fe cycles that can lead to runaway planetary oxygenation as rising atmospheric pO(2) sweeps
195 bservational constraint is available for the planetary population surrounding ultracool dwarfs, of wh
201 sition of Earth's mantle control fundamental planetary properties, including the vigor of mantle conv
203 r Mars exploration in terms of rover safety, planetary protection during rover operations, and the cu
208 We find that the difference between the planetary radius measured at optical and infrared wavele
212 e dominated by the controlling influences of planetary rotation and magnetic fields through the Corio
214 the strong dependence of these properties on planetary rotation, buoyancy driving and magnetic fields
216 re and 100 km in the ocean, smaller than the planetary scale and the typical extent of ocean basins,
222 tion is dominated by beat patterns caused by planetary-scale wave pairs and by a small number of brig
223 the positive STWCPSST anomaly and subsequent planetary-scale wave propagation act to increase the Arc
226 occur in several astrophysical scenarios and planetary science [Drake R (2005) Plasma Phys Controlled
227 ities across scientific disciplines, such as planetary science and astronomy, each of which are grapp
230 s, and a prominent goal in geomorphology and planetary science is to determine formation processes fr
237 rent interest for warm dense matter physics, planetary sciences, and inertial fusion energy research.
238 f technical disciplines, including earth and planetary sciences, environmental monitoring, bioremedia
239 roblems across many disciplines in earth and planetary sciences, including paleoclimatology, sediment
240 rity, we integrate the physical insight from planetary sciences, the liquid marble model from fluid m
247 y consistent with gradual oxygenation of the planetary surface after the evolution of oxygenic photos
250 ns terrestrial life and consists of the thin planetary surface layer between unaltered rock and the a
252 returned samples underpins age estimates for planetary surfaces throughout the inner Solar System and
253 nderstanding the ways in which floods modify planetary surfaces, the hydrology of early Mars and abru
254 formation in heterogeneous thin films or on planetary surfaces-have been characterized experimentall
256 llenging to quantify how the architecture of planetary sysems is affected by these environmental proc
258 simulations to demonstrate that the GJ 3512 planetary system challenges generally accepted formation
259 solar system are merely possible outcomes of planetary system formation and evolution, and conceivabl
261 ences (with p values of 10(-5) to 10(-2)) in planetary system properties between phase space overdens
262 show that the solar nebula that spawned our planetary system was rich in water and organic molecules
268 sent yet another new and unexpected class of planetary systems and provide an opportunity to test the
271 12) and demonstrate that the architecture of planetary systems exhibits a strong dependence on local
272 ause these are the environments in which new planetary systems form, some of the chemical species mad
275 Accounting for detection efficiency, such planetary systems occur with a frequency similar to the
276 ilar events should be very rare in quiescent planetary systems of the age of Fomalhaut, suggesting th
277 dwarfs, suggests that rocky debris from the planetary systems of white-dwarf progenitors occasionall
278 tside it, despite models of the formation of planetary systems suggesting that orbital migration of g
279 dd an important constraint on simulations of planetary systems, since they must be able to reproduce
289 global topography is more subdued, allowing planetary temperatures to vary depending on the global d
292 s regarding the longevity of such sources on planetary timescales-and whether any survive today-remai
293 and vapor loss of lighter Si isotopes during planetary volatilization were also influential in establ
295 , we suggest that airborne dust can postpone planetary water loss at the inner edge of the habitable
296 spheric polar vortex by enhancing the upward planetary wave propagation, and thereby affecting both s
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.