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1 time dilation is due to the increase in the atmospheric (14)C/(12)C ratio caused by the (14)C produc
4 uitous in the atmosphere and a source of new atmospheric aerosol particles of potentially global sign
5 tion (HESI) and nano-ESI for the analysis of atmospheric aerosol samples in the negative ionization m
6 dentities, properties, and concentrations of atmospheric aerosol surfactants in multiple environments
7 in the concentration and the composition of atmospheric aerosol, uncertainty exists as to whether th
8 hotosensitizer chemistry of HULIS in ambient atmospheric aerosols is unlikely to be a significant sou
9 ite (HMSi), which has not been identified in atmospheric aerosols, can emerge as the product of aqueo
10 umic-like substances (HULIS), extracted from atmospheric aerosols, retain the compositional complexit
11 cid, as a proxy for humic-like substances in atmospheric aerosols, to contribute to secondary organic
14 ations in many areas of chemistry, including atmospheric and environmental chemistry, biology, electr
18 munity is advanced in investigating sources, atmospheric and oceanic transport, and forecasting clima
19 ine heatwave (2014-2016) associated with two atmospheric and oceanographic anomalies, the "Blob" and
21 MSA can significantly alter the pH values of atmospheric aqueous aerosols and HMHSi is the most abund
22 These efforts are critical constraints to atmospheric assessment of anthropogenic fluxes in additi
23 nformer transition-state theory study of the atmospheric autoxidation in amines exemplified by the at
24 station measurements in Samoa combined with atmospheric back-trajectories provide novel information
25 the air temperature, significantly shallower atmospheric boundary layer, and weaker winds lead to sta
28 years, driven by increasing concentration of atmospheric carbon dioxide (CO(2)) and rising earth-surf
31 stent with the expected net effect of rising atmospheric carbon dioxide and air temperature(7-9).
33 bliquity (axial tilt)-can explain the lag of atmospheric carbon dioxide behind climate during glacial
36 wing the Stack process, the (14)C isotope of atmospheric carbon dioxide is fixed in the carbonate, an
40 and vegetated marine systems contributes to atmospheric carbon drawdown, but little empirical eviden
41 of Forest Transitions to the sequestering of atmospheric carbon will enable its potential to aid in c
42 Tropical forest responses to climate and atmospheric change are critical to the future of the glo
43 uence to test plant responses to climate and atmospheric change over the past 200 yr (including Pinus
44 We performed high-resolution (12 km x 12 km) atmospheric chemical transport modeling (WRF-Chem) for t
45 coupled Earth system model, with interactive atmospheric chemistry and a microphysical treatment of s
47 ed herein has considerable potential both in atmospheric chemistry and numerous others fields (e.g.,
48 que for gas-phase analysis in analytical and atmospheric chemistry mainly due to its very high mass r
49 should also be studied in relation to other atmospheric chemistry processes, such as facilitating mu
51 tion results from the EMAC (ECHAM5/MESSy for Atmospheric Chemistry) model were analyzed to assess the
52 utions is important in the context of, e.g., atmospheric chemistry, biophysics, and electrochemistry.
53 f these examples are taken from the field of atmospheric chemistry, they were selected because of the
54 nmental data on air monitoring and simulated atmospheric chemistry, we used a spatiotemporal model to
57 While CH(3)Cl is the largest contributor of atmospheric chlorine, recent studies have shown that gro
60 y depends on distinct shifts in the regional atmospheric circulation associated with the existence of
61 This intensified energy flux reorganizes the atmospheric circulation leading to a northward shift of
63 response by a shift in the dominant mode of atmospheric circulation, likely connected with a time-tr
66 Possible explanations include mild wave or atmospheric climates and minimal anthropogenic impacts.
71 implicated as the drivers behind the rise in atmospheric CO(2) across the last deglaciation; however,
76 he combined effects of elevated salinity and atmospheric CO(2) concentration (c(a) ) on leaf gas exch
77 associated with periods of decreased global atmospheric CO(2) concentration during the LGM, confirmi
78 effects of nitrogen (N) addition and rising atmospheric CO(2) concentration on plant communities.
81 The influence of terrestrial carbon flux on atmospheric CO(2) concentrations (DeltaCO(2) ) is estima
82 nt with Oi-1 was, thus, a response to coeval atmospheric CO(2) decline and continental-scale Antarcti
85 strial carbon sinks by increasing amounts of atmospheric CO(2) implies a weakening negative feedback
86 cean is thought to play an important role in atmospheric CO(2) increases associated with Pleistocene
90 ) is mainly shifted to the night period when atmospheric CO(2) is fixed by phosphoenolpyruvate carbox
92 e South Indian Ocean's capacity to influence atmospheric CO(2) levels and amplify the impacts of inte
95 over the past ~285,000 years across varying atmospheric CO(2) levels, global ice volume and sea leve
96 ediated carbonate-silicate weathering cycle, atmospheric CO(2) partial pressure (pCO(2)) responds to
98 e we present a new high-resolution record of atmospheric CO(2) using the delta(11)B-pH proxy from 3.3
99 ise (SLR) and its interactions with elevated atmospheric CO(2), eutrophication, and plant community c
100 lytic reduction of carbon dioxide, including atmospheric CO(2), into methanol, under ambient conditio
102 We found limited evidence of cultivar or atmospheric [CO(2) ] effects on plant-fixed carbon trans
103 e of terrestrial carbon uptake to increasing atmospheric [CO(2) ], that is the CO(2) fertilization ef
106 maize (a) benefited less from an increase in atmospheric [CO(2) ]; (b) was less affected by higher te
108 pase and lipoxygenase after the same time of atmospheric cold plasma (ACP) treatment were 77.50% and
110 hod does not allow the quantification of the atmospheric components accurately because the difference
111 thanogenic metabolisms strongly modifies the atmospheric composition, leading to a warmer but less re
113 ncubated for 21 h-showed about 15-fold lower atmospheric concentrations (3-4 pg.L(air)(-1)), while im
116 partitioning of VOC oxidation products under atmospheric conditions and thus greatly affect their atm
117 non-noble metal catalysts under solvent-free atmospheric conditions hinders their industrial applicat
118 ol particles and explore gel formation under atmospheric conditions in a contactless environment with
119 producibility, for instance, due to changing atmospheric conditions or sensitive positioning of the i
120 hurricane-force winds created sediment-laden atmospheric conditions, and that muddy rains rapidly set
129 n acceleration in ice motion coincident with atmospheric cooling and a ~15% reduction in mean surface
134 deposition to the watershed, or 184% of the atmospheric deposition to the embayments that discharge
135 urces, 51% of the septic sources, 98% of the atmospheric deposition to the watershed, or 184% of the
138 We present a method for compensating the atmospheric dispersion of terahertz pulses using a cohor
139 oral variance in the Aleutian Low (a leading atmospheric driver of the PDO), and increasing correlati
140 hese results show that the photochemistry of atmospheric dust is both richer and more complex than pr
144 o optimize the magnitude and distribution of atmospheric ethane and higher-alkane VOC emissions in th
148 ong the sites suggests that OPEs with longer atmospheric half-lives and relatively high octanol-air p
150 nce of these photodissociation mechanisms on atmospheric Hg chemistry, lifetime, and surface depositi
152 s broadly considered as a possible source of atmospheric HONO in dark conditions, but the associated
154 tial pathways for anoxygenic phototrophy and atmospheric hydrogen oxidation as supplemental energy so
155 how this system of interacting units in the atmospheric, hydrologic and geomorphological realm funct
157 , hydrocarbon seepage is expected to have no atmospheric impact because the gas is typically consumed
159 tribution of shale gas emissions to observed atmospheric increases in the global methane burden.
160 utes originates from various sources such as atmospheric inputs, rock dissolution and fertilizer resi
161 ropopause heightening, position and speed of atmospheric interface zones, as well as the poleward mov
163 ndamentally different approaches: "top-down" atmospheric inversions and "bottom-up" biosphere models.
166 y, controlled experiments involving isolated atmospheric ions and neat saturated hydrocarbons in vacu
167 mpilation of global records of anthropogenic atmospheric lead (Pb) spanning the last 4000 years, an e
168 se ash particles are assumed to have a short atmospheric lifetime, and to not participate in sulfur c
170 timates for 1,2-IHN Henry's law constant and atmospheric liquid water volume, we show that condensed-
172 cing emission sources and transformations of atmospheric mercury with Hg stable isotopes depends on t
175 n sources responsible for the sudden rise of atmospheric methane concentration (XCH(4)) since 2007, b
176 sidered to be the dominant natural source of atmospheric methane in terrestrial and shallow-water are
178 orth Atlantic Oscillation (NAO) is the major atmospheric mode that controls winter European climate v
184 In this regard, extraction of the ubiquitous atmospheric moisture is a powerful strategy allowing for
186 re we present recently available data on the atmospheric mole fraction of CO(2), measured from six si
192 ts for emissions that might be sensed by the atmospheric network, but which are not included in inven
195 led the potential future impact of change in atmospheric nitrogen deposition on hypoxia in Chinese co
196 oxygen isotope compositions (Delta'(17)O) of atmospheric O(2) and [Formula: see text] are primarily r
197 Archean volcanic gases could have prevented atmospheric O(2) from accumulating until ~2.5 Ga with >=
199 including humans, thrive because of abundant atmospheric O(2), but for much of Earth history O(2) lev
200 standing carbon cycle dynamics observed from atmospheric observations and in using these observations
203 ld have been partly attributed to a range of atmospheric or landscape drivers, one often-forgotten dr
204 as used in this work to examine the roles of atmospheric organics in affecting ROS formation and anti
207 ement in urban areas, further increasing the atmospheric oxidizing capacity and facilitating secondar
208 uilibrium stromal oxygen concentration under atmospheric oxygen at 3 mW/cm(2) was 2.3% in 100 mum dec
209 t fracturing and erosion are as important as atmospheric oxygen in limiting pyrite reactivity over Ea
213 transformation products were measured in 20 atmospheric particle samples collected in Chicago, in 21
214 ss burning is a significant global source of atmospheric particles and a highly variable and poorly u
215 exposed to elevated number concentrations of atmospheric particles are also exposed to more externall
218 lar mechanism from ocean iodine emissions to atmospheric particles that is currently missing in model
219 l acidity largely regulates the chemistry of atmospheric particles, and resolving the drivers of aero
221 miological studies address health effects of atmospheric particulate matter (PM) using mass-based mea
224 ith a special clamping device of non-thermal atmospheric plasma (NTAP) treatment using mixed gas for
225 n 300 daily PM(10) and further size-resolved atmospheric PM samples in the size range from 15 nm to 1
227 clic aromatic hydrocarbons (PAHs) are common atmospheric pollutants and known to cause adverse health
229 transcriptional response induced by outdoor atmospheric pollution mixtures using field-based exposur
231 verall, a reducing scenario leads to a lower atmospheric pressure at the surface and to a larger atmo
235 ost identical mass spectra as APCI involving atmospheric pressure conditions, the presence of many di
236 mass spectrometry data files generated by an atmospheric pressure gas chromatography-quadrupole time-
238 ablation (LA) system to the liquid sampling-atmospheric pressure glow discharge (LS-APGD) microplasm
239 turated hydrocarbons at room temperature and atmospheric pressure has been performed in this system t
242 lectrospray ionization (ESI)(+), ESI(-), and atmospheric pressure photoionization (APPI)(+)) to chara
243 i)Pr(3))(2), Cp* = C(5)Me(5)) with ethene at atmospheric pressure produces the ethene-bridged diurani
244 tected at the surface during a period of low atmospheric pressure resulted from fractures of extremel
249 additional methods that ionize molecules at atmospheric pressure, (ii) ambient pressure ion mobility
250 tube ion mobility spectrometer, operated at atmospheric pressure, to a linear ion trap mass spectrom
251 lene but not propane at room temperature and atmospheric pressure, whereas the isostructural SIFSIX-3
252 temperature, and negatively correlated with atmospheric pressure, while the correlation pattern was
255 tably, facile switching of the ion source to atmospheric-pressure chemical ionization with the exact
256 terization techniques to nanoparticles using atmospheric-pressure ion mobility-mass spectrometry (IM-
257 of LTP treatments against bacteria using an atmospheric-pressure plasma jet and show that LTP treatm
258 per, we present a new method to study global atmospheric processes and their changes during the last
260 severe consequences for ecosystem function, atmospheric processes, sustainable resources and global
263 able if use can be made of past increases in atmospheric radiocarbon concentration or so-called Miyak
264 gs, which would affect the seasonal cycle of atmospheric radiocarbon concentrations recorded in diffe
266 erature and precipitation extremes onto each atmospheric regime, we gain insight into the types of di
267 hese uncertainties, we use a global model of atmospheric Se cycling and a database of more than 600 s
269 lts highlight the role of the ocean as a net atmospheric Se sink, with around 7 Gg yr(-1) of Se trans
270 OCs) in the bulk particle phase of a viscous atmospheric secondary organic aerosol (SOA) can have a p
271 nt implications for nucleation and growth of atmospheric secondary organic aerosols and atmospheric O
273 olysis exerts a substantial control over the atmospheric SOA lifetime, with a likely dependence upon
274 ms are applicable to a broader extent across atmospheric species having carbonyl and hydroxyl functio
276 ions of the plume width based on terrestrial atmospheric stability classes; a modified Gaussian dispe
278 region of New York, a historical hotspot for atmospheric sulfur and nitrogen deposition, features abu
280 ndicates the influence of temperature-driven atmospheric teleconnections on wave-generation cycles.
282 eric pressure at the surface and to a larger atmospheric thickness compared to an oxidised system.
285 ing, dissipating an object's heat through an atmospheric transparency window (8-13 mum) to outer spac
286 ization-selective thermal emission at the IR atmospheric transparency window for radiative cooling, i
287 e cooling lies in the high emissivity in the atmospheric transparency window through which heat can b
289 se state-of-the-art numerical simulations of atmospheric transport and meteorological data to follow
293 ganophosphate esters (OPEs) were measured in atmospheric vapor and particle samples collected at six
294 om airborne remote sensing imagery indicates atmospheric venting from refinery hydrogen plants, landf
295 ssociated with similar amplifications in the atmospheric vertical and horizontal moisture advections.
299 e/(4)He lavas from Iceland (up to 42.9 times atmospheric) with anomalous (182)W and examine how Sr-Nd
300 -based detection and attribution analysis of atmospheric zonal wind, we show that the pause in circul