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1 y element content ([Formula: see text] times solar).
2 ent trials of oral direct-acting antivirals (SOLAR 1 and 2), the United Network for Organ Sharing (UN
3  disease (MELD) scores were derived from the SOLAR-1 and 2 trials.
4 ce is on par with those of notable selective solar absorbers (SSAs) in the literature, while the wide
5 ormamidinium lead iodide (FAPbI3) perovskite solar absorbers.
6 to current methods for fabricating selective solar absorbers.
7  is demonstrated for fabricating selectively solar-absorbing plasmonic-nanoparticle-coated foils (PNF
8 lds PNFs which exhibit excellent, wide-angle solar absorptance (0.96 at 15 degrees , to 0.97 at 35 de
9 SAs) in the literature, while the wide-angle solar absorptance surpasses those of previously reported
10 ich in combination with their typically high solar absorption and low moisture availability generates
11 With straightforward optimization to improve solar absorption, our work shows the potential for uncon
12 ay have been induced independently by direct solar activity (and then possible feedback) and ocean-ic
13    Understanding the influence of changes in solar activity on Earth's climate and distinguishing it
14 sition is highly correlated with a proxy for solar activity, the F10.7 cm radio flux, and therefore w
15  investigate the causal relationship between solar activity, volcanic forcing, and climate as reflect
16 ntennial cycles that are possibly related to solar activity.
17 ely a combination of external forcing, i.e., solar and volcanic, and internal feedbacks, that drives
18 ermittent sustainable energy sources such as solar and wind power by storing the energy in liquid ele
19       Intermittent energy sources, including solar and wind, require scalable, low-cost, multi-hour e
20 tems that relies almost exclusively on wind, solar, and hydroelectric power.
21  for solar concentrators for mid-temperature solar applications such as supplying process heat.
22 on continues to be an outstanding problem in solar-astrophysics.
23 al reflectance, to better understand polymer solar cell (PSC) optimization approaches.
24  mesoporous standard architecture perovskite solar cell (PSC).
25 of attention CH3NH3PbI3 has received for its solar cell application, intrinsic properties of this mat
26  C-H/C-H green catalysis with dye-sensitized solar cell applications.
27 ed as possible lower toxicity alternates for solar cell applications.
28 s finding provides a novel concept to design solar cell by sacrificing part of sunlight to provide "e
29 opic TiO2 layer in a metal halide perovskite solar cell can influence the overall power conversion ef
30                                  In a tandem solar cell comprising a NIR BODIPY subcell and a matchin
31 d perovskite-based single bandgap and tandem solar cell designs have yielded impressive performances.
32 on (TTA-UC) and increase maximum theoretical solar cell efficiencies from 33% to >43%.
33              The Shockley-Queisser limit for solar cell efficiency can be overcome if hot carriers ca
34             The fabrication of a new type of solar cell encapsulation architecture comprising a perio
35          Inverted PffBT4T-2OD:EH-IDTBR blend solar cell fabricated without any processing additive ac
36   Selenium was used in the first solid state solar cell in 1883 and gave early insights into the phot
37  of the absorber and it clearly improved the solar cell performance.
38 ted approximately 50% enhancement in maximum solar cell performance.
39 tant monolithic perovskite-perovskite tandem solar cell shows a high V oc of 1.98 V (approaching 80%
40                      Herein, dye-synthesized solar cell technology is combined with lithium-ion mater
41 ens asymmetry in organic-c-Si heterojunction solar cell through molecule alignment process.
42                                          The solar cell's photovoltic performance in terms of efficie
43 ve this including crystalline silicon (c-Si) solar cell.
44 8.1% is achieved for the flexible perovskite solar-cell devices made on an indium tin oxide/poly(ethy
45                                  All-polymer solar cells (all-PSCs) offer unique morphology stability
46 units is designed and applied in all-polymer solar cells (all-PSCs).
47 eveloped so far for high-performance organic solar cells (OSCs) are designed in planar molecular geom
48                         Mixed ion perovskite solar cells (PSC) are manufactured with a metal-free hol
49 ular acceptor (SMA) for nonfullerene polymer solar cells (PSCs).
50                      Conventional perovskite solar cells (PSCs); however, suffer the issue that lead
51 er improve PCE of single junction perovskite solar cells (PVSCs) because of a better balance between
52 rated in organic-inorganic hybrid perovskite solar cells (PVSCs), critical concerns pertaining to the
53 e efficient, low-cost, and stable perovskite solar cells (PVSCs).
54 ymer acceptors" in bulk-heterojunction (BHJ) solar cells achieve >7 % efficiency when used in conjunc
55  lend them to application in high-efficiency solar cells and light-emission devices.
56  stability problem for their applications in solar cells and other optoelectronics.
57 es over laborious layer-by-layer methods for solar cells and photodetectors, while opening the door t
58      Efficient wide-bandgap (WBG) perovskite solar cells are needed to boost the efficiency of silico
59   While the basic principles of conventional solar cells are well understood, little attention has go
60  cost-effective manufacturing process for Si solar cells based on electrodeposition.
61 g the further commercialization of thin-film solar cells based on hybrid organohalide lead perovskite
62                                              Solar cells based on hybrid perovskites have shown high
63  a solid standing point, on which perovskite solar cells can be understood more accurately and their
64 s quite limited because very few such hybrid solar cells can simultaneously show high short-circuit c
65 n be efficiently harvested by the perovskite solar cells for electric power generation.
66 e that the choice of redox mediator in these solar cells has a profound influence on both the light h
67  interfacial electron transfer in sensitized solar cells has mostly been probed by visible-to-teraher
68                 The efficiency of perovskite solar cells has surged in the past few years, while the
69                 Organic-inorganic perovskite solar cells have attracted tremendous attention because
70                   Amorphous silicon (a-Si:H) solar cells have been constructed on nanoholes array tex
71                                      Silicon solar cells have captured a large portion of the total m
72 ic-inorganic hybrid perovskite multijunction solar cells have immense potential to realize power conv
73 ersion efficiency (PCE) of the 3-dimensional solar cells improved by up to 60% compared to using AZO
74 conversion efficiency of ITIC2-based organic solar cells is 11.0%, much higher than that of ITIC1-bas
75 methylammonium lead triiodide single crystal solar cells is extended to 820 nm, 20 nm broader than th
76 e layer of bulk heterojunction (BHJ) organic solar cells is paramount to achieve high-efficiency devi
77 ever, the efficiency of tin-based perovskite solar cells is still low and they exhibit poor air stabi
78 ), organic field-effect transistors (OFETs), solar cells or other light harvesting devices.
79 evolution of the dye adsorption capacity and solar cells parameters are explored as a function of the
80            TOA-perovskite-based n-i-p planar solar cells show minimal discrepancies between stabilize
81                       Fullerene-free organic solar cells show over 11% power conversion efficiency, p
82 highest efficiencies reported for perovskite solar cells so far have been obtained mainly with methyl
83          Highly efficient colored perovskite solar cells that exploit localized surface plasmon reson
84 re needed to boost the efficiency of silicon solar cells to beyond Schottky-Queisser limit, but they
85 ng the charge transport layers in perovskite solar cells when the perovskites have a different compos
86 PCE10), the two mixed acceptors also lead to solar cells with 11.0 +/- 0.4% efficiency and a high ope
87 mance is also achieved for cesium tin iodide solar cells with en loading, demonstrating the broad sco
88                               WBG perovskite solar cells with ICBA-tran3 show enhanced VOC by 60 mV,
89 trategy to improve the efficiency of Silicon solar cells with mass-compatible techniques that could s
90 dy, we demonstrate graded bandgap perovskite solar cells with steady-state conversion efficiencies av
91             During the 140 h experiment, the solar cells with the Au electrode experience a dramatic,
92 ons in the movie provide insight into future solar cells, 2D materials and other semiconductor device
93 eneration environmentally friendly germanium solar cells, and near-to-mid infrared (1.8-2.0 mum) lase
94  create stratified bulk heterojunction (BHJ) solar cells, in which the two BHJ layers are spin cast s
95 o enhance the efficiency of perovskite-based solar cells, instead of using tandem devices or near inf
96      GaAs based optoelectronic devices (e.g. solar cells, modulators, detectors, and diodes) used in
97 on process, known to provide high efficiency solar cells, on semitransparent indium tin oxide (ITO) a
98 applications in white light emitting diodes, solar cells, optical codes, biomedicine and so on.
99 ignificant interest for applications such as solar cells, photodectors, light-emitting diodes, and la
100 monstrated only in the application of a-Si:H solar cells, the ideas are able to extend to application
101 ropelled by modern applications in thin-film solar cells, transistors and optical sensors.
102 nificantly affects the efficiency of organic solar cells.
103 w-cost high-performance tin-based perovskite solar cells.
104 graphene nanoribbons and their properties in solar cells.
105 iency of 17.8% for single crystal perovskite solar cells.
106 ith aspect-ratios up to 8, on the surface of solar cells.
107 tor devices, such as transistors, diodes and solar cells.
108 is an electron transport material in organic solar cells.
109 -free HTL for lead-free tin-based perovskite solar cells.
110 ise for boosting the PCE of third generation solar cells.
111 d backward scattering in plasmonic thin film solar cells.
112 ove the power conversion efficiency (PCE) of solar cells.
113 ganic, photovoltaics (OPV)/perovskite hybrid solar cells.
114 potential for applications in tandem organic solar cells.
115 and diffusion lengths observed in perovskite solar cells.
116 ing materials for vacuum processable organic solar cells.
117  the corresponding polycrystalline thin-film solar cells.
118 e for a new generation of easily processable solar cells.
119 e time for carrier extraction in hot carrier solar cells.Carrier-carrier scattering rates determine t
120 e Shockley-Queisser limit of single-junction solar cells; however, they are limited by large nonideal
121  avenue in low cost fabrication of thin-film solar-cells.
122 me shift around 1000-1300 CE after which the solar-climate coupling weakened considerably.
123  degrees C, thereby eliminating the need for solar concentrators for mid-temperature solar applicatio
124 -conversion applications such as luminescent solar concentrators.
125 ts that will find uses in efficiency-limited solar conversion technologies, heat sinks, and biofuel p
126 nergetic particles akin to those seen in the solar corona.
127  F10.7 cm radio flux, and therefore with the solar cycle phase.
128 iming and compromises synchronisation to the solar day when wake-times are not enforced.
129                                              Solar driven photoelectrochemical water splitting (PEC-W
130 mpts us to explore its use in fabrication of solar-driven electrolysis.
131                                              Solar-driven heterogeneous photocatalysis has been widel
132 uidic devices with customizable wettability, solar-driven oil-water clean-up and demulsification tech
133   Here we use full-Sun observations from the Solar Dynamics Observatory, to show that when the Sun is
134 in 171 A by the Atmospheric Imaging Assembly/Solar Dynamics Observatory.
135 arlight around the Sun during the 1919 total solar eclipse provided measurements that confirmed Einst
136                             About 50% of the solar energy absorbed at the Earth's surface drives evap
137 etwork of pigment-protein complexes captures solar energy and transports it to the reaction center, w
138 sis is the mimicry of the natural process of solar energy conversion into chemical energy carriers.
139 titanium dioxide is important for its use in solar energy conversion, photocatalysis, and other appli
140 y wasting reaction is of direct relevance to solar energy conversion.
141 s, spanning areas from biological imaging to solar energy conversion.
142 reasing biomass yields and developing robust solar energy devices.
143 n because of its ability to directly utilize solar energy for production of solar fuels, such as hydr
144 omising solutions for renewable and portable solar energy generation and other related phase-change a
145 to artificial photosynthesis for large-scale solar energy harvesting and storage.
146 forts are dedicated to convert and store the solar energy in a single device.
147 house gas emissions and simultaneously store solar energy in chemical form.
148                            Greater levels of solar energy storage provide an effective solution to th
149 provides an attractive route for large-scale solar energy storage, but issues surrounding the efficie
150 er change from energy development, including solar energy, presents trade-offs for land used for the
151 hieve efficient and high-capacity storage of solar energy, through improving both photocurrent and ph
152 nter (PSII RC) indicates that photosynthetic solar-energy conversion might be optimized through the i
153 avorable excited-state properties for use in solar-energy conversion.
154 erged as a new and highly promising class of solar-energy materials.
155                  However, the development of solar-energy technologies is severely hindered by poor e
156 her because it is impossible to forecast the solar eruptions that can cause these terrestrial events
157 t magnetic breakout is a universal model for solar eruptions.
158                          The observations of solar flare onsets show rapid increase of hard and soft
159 ue to assemble efficient photoelectrodes for solar fuel generation.
160 ogen fuel generated in this way is named as "solar fuel".
161                   Photoelectrochemical (PEC) solar-fuel conversion is a promising approach to provide
162 ectly utilize solar energy for production of solar fuels, such as hydrogen and hydrocarbon fuels and
163  in the (photo)electrochemical generation of solar fuels.
164 CO2 to CO is a sustainable route to storable solar fuels.
165 iable and nondispatchable nature of wind and solar generation has been driving interest in energy sto
166                        The most widely known solar geoengineering proposal is stratospheric aerosol i
167                                              Solar geoengineering refers to a range of proposed metho
168 distinguish these alternatives, we pursued a solar geolocator study [23, 24] to do so.
169 g Titan's 2009 northern spring equinox, peak solar heating moved to the northern hemisphere, initiati
170 ly localized photothermal heating induced by solar illumination alone drives the distillation process
171 zed dyes (less than 1 in 100,000) under full solar illumination.
172 uorescence from space using passive methods (solar-induced Chl fluorescence, SIF) promise improved ma
173 in the ten megacities track well that of the solar-induced chlorophyll fluorescence (SIF) data from G
174 leaf-level ChlF was linked with canopy-scale solar-induced chlorophyll fluorescence (SIF) in a temper
175 limate anomalies by assimilating column CO2, solar-induced chlorophyll fluorescence, and carbon monox
176 of sensitivity experiments in which not only solar insolation changes are varied but also vegetation
177 ossby waves and differential rotation of the solar interior shear-layer (called tachocline).
178 iven by variations in the magnitude of total solar irradiance (TSI) and changes in the greenhouse gas
179               By experimentally manipulating solar irradiance and nighttime air humidity, we estimate
180 ogenic radionuclide data and resulting total solar irradiance estimates during grand minima.
181 orewater and oceanic DOS molecular formulas, solar irradiation increased the similarity due to the re
182 cture and scalable methods which can convert solar irradiation into exploitable thermal energy with h
183  a simple and inexpensive system that, under solar irradiation, forms highly reductive radicals in th
184 predictor more often than relative humidity, solar irradiation, or temperature.
185 ge 7 dye in aqueous solution under simulated solar irradiation.
186 >90% selectivity under UV-filtered simulated solar light irradiation (AM 1.5G, 100 mW cm(-2), lambda
187 l composition in the coronae of low-activity solar-like stars appears to be related to fundamental st
188 r understanding the elemental composition of solar-like stellar coronae.The Sun's elemental compositi
189 e consistent with a shell of several tens of solar masses ejected by the progenitor star at supernova
190      This merging companion hosts 35 billion solar masses of stars and has a star-formation rate of 5
191 with initial masses of more than about 10(4) solar masses or episodic hyper-Eddington accretion.
192 xies with star-formation rates exceeding 100 solar masses per year at z > 6 (corresponding to an age
193 f stars and has a star-formation rate of 540 solar masses per year, but has an order of magnitude les
194 on rates of these galaxies, which exceed 100 solar masses per year, require large reservoirs of cold
195 ion rates in the companions of more than 100 solar masses per year.
196             The existence of massive (10(11) solar masses) elliptical galaxies by redshift z approxim
197 n indicates a high mass ( approximately 0.03 solar masses) wind-driven outflow with moderate electron
198 er halo with a mass of more than 100 billion solar masses, making it among the rarest dark-matter hal
199 lained with an ejected mass of 0.04 +/- 0.01 solar masses, with an opacity of less than 0.5 square ce
200 = 3.717, with a stellar mass of 1.7 x 10(11) solar masses.
201 st white dwarf to the Sun-as 0.675 +/- 0.051 solar masses.
202   Here, we demonstrate nanophotonics-enabled solar membrane distillation (NESMD), where highly locali
203 asons, and that its timings are entrained to solar midnight.
204                      This indicates that the solar nebula field, and likely the nebular gas, had disp
205 s must have formed before dissipation of the solar nebula, which likely occurred within less than 10
206 is the evolution of a gaseous and magnetized solar nebula.
207  of the entire solar spectrum by redirecting solar photons to maximize FEW production from a given la
208                                              Solar photovoltaic (PV) electricity generation is expand
209                    We examine the utility of solar photovoltaic (PV) system deployment on urban rooft
210 uding semiconductor, flat panel display, and solar photovoltaic industries.
211 uct of copper refining, which is critical to solar photovoltaics, is chosen as a case study, and thre
212 ost abundant form of condensed matter in our solar planetary structure.
213     Our multicriteria assessment of wind and solar potential for large regions of Africa shows how ec
214 s natural resource is comparable to wind and solar power, yet it does not suffer as much from varying
215 se modified tetrapyrroles for the capture of solar radiation and its conversion to chemical energy.
216 flower activity were associated with greater solar radiation and lower rainfall during El Nino years.
217 ompounds in atmospheric aerosols that absorb solar radiation and may play an important role in planet
218 s, despite similar natural forcings, such as solar radiation and the North Atlantic Oscillation, duri
219                       Our findings emphasize solar radiation as a significant driver of mass balance
220 itivity of plants under the broad spectra of solar radiation in nature.
221 ops and increasing the efficiency with which solar radiation is converted into biomass has recently b
222  has amplified the effects on temperature of solar radiation on west-facing slopes.
223  exert a systematic modulating effect on the solar radiation penetrating into the subsurface layers,
224  severe aerosol pollution over China reduces solar radiation reaching the surface.
225 st electron transport in leaves under canopy solar radiation was shown to be a major contributor to t
226     In contrast, community-wide responses to solar radiation were predominantly positive.
227 y reference evapotranspiration, temperature, solar radiation, and precipitation together, but nonline
228  cover with a resulting increase in received solar radiation, and secondarily by a decrease in the st
229 , or fivefold stronger effect than rainfall, solar radiation, and the Multivariate ENSO Index, respec
230 , the changes are related to obliquity-paced solar radiation, manifest as variations in total summer
231   Black carbon (BC) aerosol strongly absorbs solar radiation, which warms climate.
232 fects the extent to which they interact with solar radiation.
233 s in response to soil water availability and solar radiation.
234 nderstanding for how such aerosols influence solar radiative forcing of the atmosphere.
235 ve spatial and frequency characterization of solar radio burst fine structures observed with the Low
236                            The choice of the solar reactor holds the key for the commercialization of
237                                              Solar rechargeable battery combines the advantages of ph
238 allation of roofing materials with increased solar reflectance (i.e., "cool roofs") can mitigate the
239       However, genes and pathways altered by solar-simulated UVR (ssUVR), a mixture of UVA and UVB, a
240 ngth measurements of absorption lines in the solar spectrum by Fraunhofer, the identification of tran
241 ge, we propose the utilization of the entire solar spectrum by redirecting solar photons to maximize
242  existing doped CQDs that are aimed for full solar spectrum LSCs suffer from moderately low quantum e
243                             We present novel solar spectrum unbundling FEW systems (SUFEWS), which ca
244              One approach to further enhance solar spectrum utilization is the graded bandgap, but th
245 etamaterial that is fully transparent to the solar spectrum while having an infrared emissivity great
246   Photosynthesis uses a limited range of the solar spectrum, so enhancing spectral coverage could imp
247                   Herein, a high-performance solar steam device composed entirely of natural wood is
248 result, the 3D-printed evaporator has a high solar steam efficiency of 85.6% under 1 sun illumination
249  generation device for low-cost and scalable solar steam generation applications.
250 lexible, portable, recyclable, and efficient solar steam generation device for low-cost and scalable
251 been dedicated to developing high-efficiency solar steam generation devices, challenges remain in ter
252                    The current challenge for solar steam generation is to develop easy-to-manufacture
253 with a concave structure for high-efficiency solar steam generation under 1 sun illumination is used.
254                                          The solar steam process, akin to the natural water cycle, is
255  of energy storage, wastewater treatment and solar-steam-assisted desalination.
256 d or electrically proximate wind/storage and solar/storage facilities across the U.S. and determine t
257 likely occurred within less than 10 My after Solar System formation.
258 ly 750,000 known asteroids and comets in the Solar System is thought to have originated outside it, d
259 there has been no way of telling whether the Solar System is typical of planetary systems.
260 lude that Pluto's atmosphere is unique among Solar System planetary atmospheres, as its radiative ene
261 bundances and planetary configuration of the Solar System today, but there has been no way of telling
262 active earlier in its history.Mars hosts the solar system's largest volcanoes, but their formation ra
263 predicted chaotic dynamical behaviour of the Solar System, and provides a constraint for refining num
264  powerful persistently active volcano in the Solar System, Loki Patera.
265 y to addressing numerous questions about our solar system.
266 nation compared with other reservoirs in the solar system.
267 s of atmospheric circulation not seen in the solar system.
268 rganic-rich asteroids that reside within the Solar System.
269                     Ground-based 1-m Swedish Solar Telescope (SST)/CRISP, Halpha 6562.8 A observation
270 hose observed in a C1.5 flare by the Swedish Solar Telescope.
271                                              Solar thermal energy conversion has attracted substantia
272                 The development of molecular solar thermal systems presents one approach to address t
273  work shows the potential for unconcentrated solar thermal systems to reach stagnation temperatures e
274 rates, large phase-change enthalpy, and high solar-thermal energy conversion efficiency.
275  for their promising applications for direct solar-thermal-electric conversion.
276                        For the production of solar thermochemical fuels arid regions are best-suited,
277  The production of alternative fuels via the solar thermochemical pathway has the potential to provid
278                                          The solar thermochemical route also promises to be an attrac
279 ferrocyanide redox battery with a high ideal solar-to-chemical conversion efficiency of 3.0% without
280 that mimic natural photosynthesis to achieve solar-to-chemical conversion is of great promise for fut
281 ater splitting using hybrid perovskites with solar-to-hydrogen efficiencies beyond 15%.
282  cold urticaria, delayed-pressure urticaria, solar urticaria, heat urticaria, vibratory angioedema, c
283 vels in mouse skin are induced by short-term solar UV irradiation, and a long-term skin carcinogenesi
284 ental threats, including microbes, injuries, solar UV radiation, and allergens.
285 terborne pathogens of humans and wildlife to solar UV, and use the DNA action spectrum to model how d
286 Moreover, we show that TRAF1 is required for solar UV-induced extracellular signal-regulated kinase-5
287                However, the coupling between solar variability and local climate varied with time, wi
288 l properties of heterogeneous interfaces for solar water splitting applications using first-principle
289            It also unlocks opportunities for solar water splitting using hybrid perovskites with sola
290 n p-Si and a RED stack, successfully enables solar water splitting without the need for an external b
291 xistence of the Sun's hot atmosphere and the solar wind acceleration continues to be an outstanding p
292 ficant spatial/temporal gradients in ambient solar wind conditions are present.
293  believed to be the main driver to transport solar wind into the Earth's magnetosphere when the magne
294                The magnetopause deflects the solar wind plasma and confines Earth's magnetic field.
295 ce the first quantitative estimate of global solar wind variations over the last 400 years.
296 uires accurate reconstruction of the ambient solar wind with which they interact, and that simple ass
297 netic field produces a magnetopause with the solar wind, and substantially increases their energy dep
298 ncluding photolysis and radiolysis of water, solar wind-surface interactions and gas-phase collisions
299 ated with Alfvenic waves that help drive the solar wind.
300          The photolytic lifetime of IMD at a solar zenith angle of 35 degrees is calculated to be 16

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