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2 y calculations involving over half a million atmospheric absorption lines, providing a highly accurat
5 lobal biogeochemical cycling, and ameliorate atmospheric accumulation of carbon dioxide by 'pumping'
6 on Climate Change, the National Oceanic and Atmospheric Administration, the National Renewable Energ
7 or the elemental carbon (EC) contents in the atmospheric aerosol may have a stronger effect than the
10 O) may incur effects on the SO2 chemistry in atmospheric aerosols because the solvation of SO2 at the
11 (BrC) consists of those organic compounds in atmospheric aerosols that absorb solar radiation and may
12 g can be relatively long-lived components in atmospheric aerosols, thus more likely to have larger im
17 le the standard Sellmeier equation (SSE) for atmospheric air is not intended for the description of a
20 ultrashort mid-infrared laser pulses through atmospheric air, probing air dispersion in the 3.6-4.2-m
21 trol has precluded precise alignment of ice, atmospheric and marine records, making it difficult to a
28 ts in this region include randomly occurring atmospheric blocking patterns, ocean impacts on atmosphe
32 the tropics, consistently underestimate the atmospheric burden of CH4 determined via remote sensing
33 cal for simulating stomatal control of plant-atmospheric carbon and water exchange under current, pas
34 nds play an important role in regulating the atmospheric carbon dioxide (CO2 ) concentrations and thu
36 al variations in the measured growth rate of atmospheric carbon dioxide (CO2) originate primarily fro
37 n over the tropics, while the growth rate of atmospheric carbon dioxide (CO2) was the largest on reco
38 onses to past, present and future changes in atmospheric carbon dioxide concentration ([CO2 ]) is cri
39 anges-especially climate change and elevated atmospheric carbon dioxide concentrations-are increasing
40 ely played an important role in the observed atmospheric carbon dioxide swings by affecting the parti
45 twentieth century that is based on long-term atmospheric carbonyl sulfide (COS) records, derived from
48 e mid-Palaeozoic c. 0.45-0.4 Ga shows global atmospheric changes consistent with increased terrestria
50 nd RBS, respectively) are known for altering atmospheric chemistry and causing sharp tropospheric ozo
52 lculations were performed to investigate the atmospheric chemistry of (CF3)2CFCN, a proposed replacem
56 due to a common forcing, such as large-scale atmospheric circulation (North Atlantic Oscillation, NAO
58 ospheric blocking patterns, ocean impacts on atmospheric circulation, and climate's response to anthr
59 idence that a specific pattern of summertime atmospheric circulation--the summer East Atlantic (SEA)
60 rved changes in U.S. frost timing to various atmospheric circulations yielded only modest correlation
62 productivity by the low partial pressure of atmospheric CO2 (Ca ) experienced during the last glacia
65 ferred from double deconvolution analyses of atmospheric CO2 and [Formula: see text]C at different te
66 vironments are warmer, have higher levels of atmospheric CO2 and have altered patterns of disturbance
71 reveals large orbitally driven variations in atmospheric CO2 concentration between [Formula: see text
72 d to underpin much of the ice age decline in atmospheric CO2 concentration, but the specific changes
77 ough correlations between the growth rate of atmospheric CO2 concentrations and the El Nino-Southern
78 important role in modulating the changes in atmospheric CO2 concentrations during El Nino events-a p
79 stock grazing, fire-suppression and elevated atmospheric CO2 concentrations facilitating shrub recrui
80 enic carbon dioxide emissions have increased atmospheric CO2 concentrations from 270 to 400 mol mol(-
81 ibution of deforestation emissions to rising atmospheric CO2 concentrations is poorly quantified.
82 acity of land ecosystems to slow the rise in atmospheric CO2 concentrations may be smaller than previ
83 l soils could undergo N-dependent changes as atmospheric CO2 concentrations rise, having global-scale
84 sed to characterize the response of tropical atmospheric CO2 concentrations to the strong El Nino eve
85 vity is most strongly associated with rising atmospheric CO2 concentrations using yearly aggregated d
86 siological responses of plants to changes in atmospheric CO2 concentrations, and fire, as well as wha
87 osystem-scale responses to future changes in atmospheric CO2 concentrations, and thus feedbacks to cl
89 iment records suggest that episodes of major atmospheric CO2 drawdown during the last glacial period
91 the synthesis of renewable bioproducts from atmospheric CO2 Growth and metabolism of cyanobacteria a
93 impose restrictions on the potential role of atmospheric CO2 in inferred warmer conditions and valley
94 The abundance variations of near surface atmospheric CO2 isotopologues (primarily (16)O(12)C(16)O
95 owing consensus that the ongoing increase in atmospheric CO2 level will lead to a variety of effects
100 ven the low levels and large fluctuations of atmospheric CO2 These findings highlight the importance
101 ane seep field on the Svalbard margin reveal atmospheric CO2 uptake rates (-33,300 +/- 7,900 mumol m(
103 Statistical models indicated that increasing atmospheric CO2 was the most important factor driving th
105 hanistically predict gS and A in response to atmospheric CO2, water availability, and time is critica
106 al sea level changes, volcanic degassing and atmospheric CO2, which may have modulated the climate sy
113 ntreal Protocol has led to reductions in the atmospheric concentration of many ozone-depleting gases,
114 tal complexity associated with assessing OPE atmospheric concentrations across a large urban landscap
116 f the surface of black phosphorus (BP) under atmospheric conditions is a significant constraint on th
125 vel at 60min (slower glycemic response) than atmospheric counterparts ( approximately 98.3% degree of
128 improving plant performance through reduced atmospheric demand and conservation of available soil wa
129 The data set was compiled by the Delaware Atmospheric Deposition Network (DADN) from samples taken
134 concentrations and isotopic compositions of atmospheric dust and dissolved depositions were monitore
135 habitable in such environments and how their atmospheric dynamics is influenced by the rapidly changi
138 igration of GJ 436b could have triggered the atmospheric escape that now sustains its giant exosphere
143 environments, but their contribution to the atmospheric formation of secondary organic aerosol (SOA)
146 istent with a Rayleigh-like evolution of the atmospheric gaseous boron reservoir with possible but li
148 ng peat-derived GEM dry deposition to modern atmospheric GEM levels we are able to reconstruct the fi
150 ay become more frequent in coming decades as atmospheric greenhouse gas concentrations rise, but the
152 5) can affect the surface energy balance and atmospheric heating rates and thus may impact the intens
153 oxy for metallicity, we measured HAT-P-26b's atmospheric heavy element content ([Formula: see text] t
154 s appear to be driven by decreasing regional atmospheric Hg emissions although they may be partly cou
155 ear, consistent with the decline in regional atmospheric Hg emissions and water Hg concentrations.
156 al mercury (Hg) have substantially increased atmospheric Hg levels during the 20th century compared t
157 owever, the impact of concomitant changes in atmospheric humidity and CO2 concentration through their
159 d 29 s after the event onset in 171 A by the Atmospheric Imaging Assembly/Solar Dynamics Observatory.
161 ioaccumulation modeling forced by changes in atmospheric inputs reasonably capture magnitudes and tem
163 series allows the determination of the boron atmospheric inputs to this forest ecosystem and contribu
164 e-receptor relationships and by the means of atmospheric inversion we were able to quantify spatially
166 erize the stellar wind of TRAPPIST-1 and the atmospheric ion escape rates for all of the seven planet
168 ielding effects can substantially extend the atmospheric lifetime of reactive pesticides from a few d
172 methane emissions have been quantified using atmospheric measurements to provide an independent compa
174 alt-induced chemical cycling of Hg (through 'atmospheric mercury depletion events', or AMDEs) and wet
175 blished data showing latitudinal declines in atmospheric mercury deposition in Canada, we observed lo
176 o quantify mercury emissions on the basis of atmospheric mercury measurements conducted at the remote
178 hyl chloroform, and the C(13)/C(12) ratio in atmospheric methane (delta(13)CH4) from 1983 through 201
180 day, water column photosynthesis based on an atmospheric model of spectral radiation, satellite-deriv
182 in the transmission spectrum, together with atmospheric modelling, then gives clues to the propertie
185 missions) and top-down approaches (measuring atmospheric mole fractions and isotopes) for constrainin
187 ting evidence indicates that future rates of atmospheric N deposition have the potential to increase
188 of N availability were independent of recent atmospheric N deposition rates, implying a minor role fo
189 change suggests that, by 2010, anthropogenic atmospheric N deposition represented 20 +/- 5% of the an
190 ignals increased deposition of anthropogenic atmospheric N on the open ocean and its incorporation in
196 ett and Strawn gas have distinct crustal and atmospheric noble gas signatures, allowing clear identif
197 iable underestimation of the traffic related atmospheric NOx input in Europe, comparable to the weeke
199 endent on lithology and the concentration of atmospheric O2 Future work on glaciation-weathering-carb
200 eninsula has been widely debated in light of atmospheric/oceanic warming and increases in glacial mel
202 established by depth-dependent variations in atmospheric oxidant and dissolved-solute concentrations.
203 eo-records with which to constrain levels of atmospheric oxidants during past climate transitions.
204 ary organic aerosol (SOA) is formed from the atmospheric oxidation of gas-phase organic compounds lea
207 during the early stages of the first rise in atmospheric oxygen on the Earth (the Great Oxidation Eve
212 e apparent lag of animal diversification and atmospheric oxygenation during this critical period of E
213 oth size and mass based metrics is common in atmospheric particle measurements, but now, the NTA can
219 ssil fuels, and it is a major contributor to atmospheric particulate matter known to have a deleterio
223 otential influence of silicate weathering on atmospheric pCO2 levels on geologically short timescales
224 gress in atmospheric plasmas has led to cold atmospheric plasma (CAP) devices with ion temperatures c
228 acerifolia is highly suitable to be used in atmospheric PM monitoring studies and that morphological
239 ded to increase with first-trimester average atmospheric pressure (odds ratio per 5-mbar increase = 1
240 and aperture from ICT analysis performed at atmospheric pressure are higher than those calculated fr
242 ainst both electrospray ionization (ESI) and atmospheric pressure chemical ionization (APCI) for the
243 urate mass (HRAM) mass spectrometry (MS) and atmospheric pressure chemical ionization (APCI) MS were
245 the sampled materials into the gas phase for atmospheric pressure chemical ionization and mass spectr
246 of a solution of polymer into the commercial atmospheric pressure chemical ionization source on this
247 applied was direct liquid injection into an atmospheric pressure chemical ionization source, followe
248 ently integrates sampling/sample cleanup and atmospheric pressure ionization, making it an advantageo
249 lective hydrocarboxylation of styrenes under atmospheric pressure of CO2 has been developed using pho
250 of solvent or dopant effects as observed in atmospheric pressure photoionization (APPI) and laser io
251 e used in parallel for (1)D detection, while atmospheric pressure photoionization (APPI) MS and ESI-M
253 ance of a new orthogonal geometry field-free atmospheric pressure photoionization (FF-APPI) source wa
256 iotic CO2 uptake in arid and semiarid soils: atmospheric pressure pumping, carbonate dissolution, and
260 cles at elevated temperature under oxygen at atmospheric pressure, by using advanced in situ electron
261 as to novel environmental challenges of low atmospheric pressure, high ultraviolet radiation, and un
262 grow only during periods of relatively high atmospheric pressure, suggesting a formation timescale o
263 n contrast, FAIMS devices operate at or near atmospheric pressure, which complicated integration with
265 Treatment of Ni(0) complexes 1a-e with sub-atmospheric pressures of trifluoroethylene (TrFE) afford
266 T-1-makes possible in-depth studies of their atmospheric properties with present-day and future astro
267 ow-cost approach based on the application of atmospheric radio frequency glow discharge (rf-GD) optic
268 isotopic ratios (up to 50 times the present atmospheric ratio, Ra) compared to the lower (3)He/(4)He
270 cal fluctuations, such as internal tides and atmospheric-related inertial currents, rather than day-n
271 , our measurements suggest that large future atmospheric releases of methane from old carbon sources
272 tude of the ENSO forcing, these sub-seasonal atmospheric responses cannot be detected for moderate El
273 presence of high-amplitude quasi-stationary atmospheric Rossby waves within a particular wavelength
275 y the CH4 flux from the SJB using continuous atmospheric sampling from aircraft collected during the
282 We report on a new method for analyzing atmospheric submicrometer particulate organic matter whi
285 , but most likely it is related to increased atmospheric temperature and precipitation, associated wi
287 dels find that ice nucleated and grown under atmospheric temperatures is at all sizes stacking-disord
289 late matter (PM2.5) pollution as a result of atmospheric transport and the production and consumption
290 wever, in contrast to the Arctic, long-range atmospheric transport is deemed less important than huma
292 tial-temporal variability and the long-range atmospheric transport potential of the studied POPs.
297 llite records, that increased cloudiness and atmospheric water vapor in winter and spring have caused
299 This invariant demonstrates that ocean and atmospheric waves share fundamental properties with topo
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