ライフサイエンスコーパス: absorber

1 been observed comparing to that of un-bended absorber.

2 bled flexible and conformable wideband radar absorber.

3 arbazole (KR131) with compositive perovskite absorber.

4 uction in a bioreactor integrated with a gas absorber.

5 single photons in a deeply subwavelength 50% absorber.

6 ehave as a perfect scatterer or as a perfect absorber.

7 the methylammonium moiety of the perovskite absorber.

8 layer separating the solution from the solar absorber.

9 erformance and the angular dependence of the absorber.

10 e through strong plasmonic resonances in the absorber.

11 luster featuring a molecularly defined light absorber.

12 ent photon tunneling from the emitter to the absorber.

13 s used to deposit Cu2ZnSn(S1-xSex)4 (CZTSSe) absorber.

14 g the conventional absorber with a plasmonic absorber.

15 ermally function material as a switchable IR absorber.

16 oelectric device covered with a conventional absorber.

17 HPs) as solution-processed photovoltaic (PV) absorbers.

18 and materials for the stabilization of light absorbers.

19 ll of them were found to be good solar light absorbers.

20 nous (melanin) and exogenous (gold nanorods) absorbers.

21 re used to identify high and low cholesterol absorbers.

22 dinium lead iodide (FAPbI3) perovskite solar absorbers.

23 tegration on surfaces of semiconductor light absorbers.

24 nductor layers of the converted metamaterial absorbers.

25 nd-capture efficacy and render sperm perfect absorbers.

26 light management offered by the metamaterial absorbers.

27 rent methods for fabricating selective solar absorbers.

28 ation of the dynamic distribution of optical absorbers.

29 ide double perovskites to compete with APbX3 absorbers.

30 thin the emerging Pb-based halide perovskite absorbers.

31 ssure oscillations in the air contacting the absorbers.

32 tentially nontoxic and defect-tolerant solar absorbers.

33 monium tin iodide ({en}MASnI3) perovskite as absorbers.

34 development of 1.5-1.6 eV bandgap perovskite absorbers.

35 port a mechanism to chemically stabilize PSC absorbers.

36 olors, corresponding to the bandgap of three absorbers.

37 p-TCO and n-type Si as a prototypical light absorber, a rectifying heterojunction capable of light d

38 e proposed system acts as an omnidirectional absorber across a broad spectral range.

39 ron conjugation and are efficient UV-vis-NIR absorbers, active up to ca. 2400 nm.

40 magnetic analysis of the ultra-thin resonant absorbers along with their complex characterization by a

41 ice integrates a multiwalled carbon nanotube absorber and a one-dimensional Si/SiO2 photonic-crystal

42 trate the use of a common graphene saturable absorber and a single gain medium (Tm(3+):ZBLAN fiber) t

43 )-Ru(b) (II)-OH2](4+), combines both a light absorber and a water oxidation catalyst in a single mole

44 timate interfacial contact between the light absorber and catalyst.

45 in (2 nm), silica layer that separates light absorber and catalyst.

46 NH3PbI3 perovskite material if used as light absorber and charge transport layer.

47 tion loss and impedance matching between the absorber and free space.

48 morphology and electronic properties of the absorber and it clearly improved the solar cell performa

49 The interface between the light absorber and p-TCO is crucial to produce selective hole

50 nts approaching the theoretical limit of the absorber and results in a solar-to-hydrogen efficiency o

51 mework for dystrophin to function as a shock absorber and signaling hub.

52 ver, efficient collection of sunlight in the absorber and spectral control in the emitter are particu

53 umulation of N-nitrosomorpholine in both the absorber and washwater increased linearly with both NO a

54 ccumulation of N-nitromorpholine in both the absorber and washwater positively correlated with flue g

55 tial to form total N-nitrosamines within the absorber and washwater units of a laboratory-scale CO2 c

56 ectrodes functionalized with molecular light absorbers and catalysts.

57 lled carbon nanotubes (SWCNTs) are promising absorbers and emitters to enable novel photonic applicat

58 bsorbers and scatterers, simultaneous photon absorbers and emitters, and all the way to simultaneous

59 spectral range, to metamaterial-based ideal absorbers and epsilon-near-zero components, where the in

60 elopment of such systems containing QD light absorbers and molecular catalysts for H2 formation.

61 Interactions between absorbers and plasmonic metasurfaces can give rise to un

62 sorbers or scatterers to simultaneous photon absorbers and scatterers, simultaneous photon absorbers

63 tanding of light-matter interactions between absorbers and surface plasmons to enable practical optoe

64 sing ideal double- and triple-junction light absorbers and the electrochemical load curves for CO2 re

65 he poor optoelectronic quality of perovskite absorbers and their PCEs have stagnated at <15%.

66 ly investigate the practical use of proposed absorbers and/or photothermal converters in integrated t

67 uning the band-gaps of triple-junction light absorbers and/or the ratio of catalyst-to-PV area, and t

68 rated and encapsulated inside of a gold foil absorber, and a superconducting transition-edge-sensor m

69 th back electron transfer of the ZrOCo light absorber, and is further aided by the instant desorption

70 ons as soft actuators, sensors, robust shock absorbers, and environmental remediation.

71 es, such as metamaterials, waveguides, light absorbers, and light emitters.

72 ic analogs of the lead perovskite solar-cell absorbers APbX3 (A = monovalent cation; X = Br or I).

73 t a promise of MXenes in broadband saturable absorber applications due to metallic characteristics, w

74 bsorptive switching, optical modulation, and absorber applications.

75 netic field and current distributions in the absorber are investigated to explain the physical origin

76 Broadband absorbers are essential components of many light detecti

77 Single-, double-, and triple-junction light absorbers are found to be optimal for electrochemical lo

78 anic perovskites (e.g., CH3NH3PbI3) as light absorbers are promising players in the field of third-ge

79 the resonance behaviour in the metamaterial absorber, are modulated externally with applied voltage

80 ing light-trapping structures in a thin film absorber as a model system.

81 Applications in energy absorbers as well as mechanical sensors and actuators ar

82 n from two galaxies associated with two such absorbers at a redshift of z 4.

83 ction (RCS) of the cylinder with and without absorber attachment has been compared and excellent abso

84 and characterization of a novel metamaterial absorber based camera with subwavelength spatial resolut

85 adband, polarization independent, wide-angle absorber based on a metallic metasurface architecture, w

86 ve lead-based hybrid inorganic-organic solar absorber based on a photoactive organic cation.

87 a resonant and dynamically tunable broadband absorber based on vanadium dioxide (VO2) phase transitio

88 broadband, polarization-independent optical absorbers based on a three-layer ultrathin film composed

89 Resonant absorbers based on nanostructured materials are promisin

90 We demonstrate that the metamaterial perfect absorber behaves as a meta-cavity bounded between a reso

91 a treatment, has improved the quality of the absorber(|)buffer interface, pushed the device efficienc

92 es the temperature of the underlying silicon absorber by as much as 13 degrees C due to radiative coo

93 Because a solar absorber by necessity faces the sky, it also naturally h

94 re, we show the advantages of particle-based absorbers by transferring the HNTs to a polymer substrat

95 Here, we introduce a class of particle absorbers called transferable hyperbolic metamaterial pa

96 With this model, metamaterial perfect absorber can be redefined as a meta-cavity exhibiting hi

97 r and the spectrally selective solar thermal absorber can direct PV band to PV modules and absorb the

98 Thus, Ohmic loss dominated metamaterial absorbers can be converted into photovoltaic near-perfec

99 aracteristics of the semiconductors in those absorbers can enable the exchange of undesired resistive

100 Broadband tunable absorbers can find applications in absorption filters, t

101 This demonstrates that perovskite absorbers can function at the highest efficiencies in si

102 hough intended to control emissions from the absorber, can contribute to additional nitrosamine forma

103 recent progress in the development of light absorber-catalyst assemblies for the reduction and oxida

104 m may exhibit either liquid-spring or energy-absorber characteristics.

105 ere we identify three distinct mode types of absorber-coated plasmonic metasurfaces: localized and pr

106 e tuned by controlling the morphology of the absorber coating and the spectral overlap of the absorbe

107 is low but are absorbed for more crystalline absorber coatings.

108 aqueous protons based on catalysts and light absorbers composed solely of earth abundant elements rem

109 taic analysis, a new ideal bandgap (1.35 eV) absorber composition (MAPb0.5 Sn0.5 (I0.8 Br0.2 )3 ) is

110 fuels are investigated as functions of light-absorber composition and configuration, and catalyst com

111 water solvent, the relative position of the absorber conduction band and the catalyst Fermi level fa

112 the printed graphene nano-flakes enables the absorber conformably bending and attaching to a metal cy

113 cancer therapy which uses an antibody-photo absorber conjugate (APC) and near infrared light exposur

114 and polarization-independent nearly perfect absorber consisting of mirror-backed nanoporous alumina.

115 e complex unit cell of the metasurface solar absorber consists of eight pairs of gold nano-resonators

116 perform better than nanostructured plasmonic absorber counterparts in terms of bandwidth, polarizatio

117 he acoustic equivalent of a coherent perfect absorber coupled to a coherent laser.

118 The absorber covers both X (8-12 GHz) and Ku (12-18 GHz) ban

119 rst halide double perovskite evaluated as an absorber, Cs2AgBiBr6 (1), has a bandgap of 1.95 eV.

120 are transferrable to arbitrary semiconductor absorbers, D(2)GIS devices offer a high-performance para

121 how the trapping efficiency of an individual absorber decreases as the number of absorbers in the clu

122 measurements of the stacked graphene-quartz absorbers demonstrated excellent broadband absorption of

123 demonstration redirects the broadband super absorber design to extreme simplicity, higher performanc

124 Such broadband absorber designs are ultrathin compared to carbon nanotu

125 Similar to the planar absorber, different dimensional absorbers including cyli

126 ynamic tuning of the distribution of optical absorbers dispersed within phase-change materials, to si

127 rs in the cluster increases and/or the inter-absorber distance decreases.

128 s, we have shown that metallic layers in the absorbers do not necessarily constitute undesired resist

129 We found that mechanical kneading of the absorber dramatically improves spectral quality by reduc

130 racterize the galaxies associated with these absorbers due to the intrinsic faintness of the galaxies

131 work as wideband spectral-selective emitters/absorbers due to the topological change in isofrequency

132 the silver back electrode to enforce also an absorber effective surface-plasmon-polariton mode.

133 This bound requires that a good absorber emits a portion of the absorbed energy back to

134 stal emitter on the same substrate, with the absorber-emitter areas optimized to tune the energy bala

135 thanks to the nanophotonic properties of the absorber-emitter surface, reaches experimental efficienc

136 y above the photovoltaic bandgap using a hot absorber-emitter, solar thermophotovoltaics promise to l

137 ic materials as they are simultaneous photon absorbers, emitters, and scatterers.

138 ctric multilayered metamaterials become good absorbers/emitters for visible light and good reflectors

139 In addition to near-ideal absorption, our absorbers exhibit omnidirectional independence for incid

140 They were shown to be good two-photon absorbers, exhibiting high two-photon absorption coeffic

141 , we suppressed carrier recombination in the absorber, facilitated carrier injection into the carrier

142 id in rational design of the polycrystalline absorber films, leading to their enhanced performance.

143 In the absorber, flue gas NOx drives nitrosamine and nitramine

144 nanoclusters (BSA-AuNCs) were used as an IFE absorber/fluorophore pair.

145 reported as a low-cost, solution-processable absorber for a thin-film solar cell with a power-convers

146 making selenium an attractive high-band-gap absorber for multi-junction device applications.Wide ban

147 has recently been identified as a promising absorber for solar cells.

148 nadate, which is identified as a novel light absorber for solar fuel applications, is prepared in a w

149 silicon, III-V compounds, and other optical absorbers for both photocathodes and photoanodes.

150 ) junctions are demonstrated to be efficient absorbers for integrated solar-driven hydrogen productio

151 quantum dots (CQDs) are new-generation light absorbers for photocatalytic H2 evolution in aqueous sol

152 temperature, rendering them promising light absorbers for photovoltaic applications.

153 cent surge of interest towards high-band gap absorbers for tandem applications led us to reconsider t

154 We design a dual-band absorber formed by combining two cross-shaped metallic r

155 rate from the sum of the rates of individual absorbers forming the cluster to the effective collectiv

156 uantitative conversion of the rather weak IR-absorber H2S into SO2, which provides a significantly mo

157 UV-assisted conversion of the rather weak IR-absorber H2S into the more pronouncedly responding SO2 i

158 principal tissue fluorophores (flavins) and absorbers (haemoglobin).

159 ate that the hosts of these high-metallicity absorbers have physical properties similar to massive st

160 using alkyl ammonium metal halides as light absorbers have the right combination of high power conve

161 hores are rare, and molecular engineering of absorbers having such properties has proven challenging.

162 e they allow rational integration of a light absorber, hole acceptor, and electron acceptor or cataly

163 cture is also suitable as the higher bandgap absorber in a dual-absorber tandem device.

164 te but have not shown high performance as an absorber in a standalone system.

165 re and concurrent formation of reduced light absorber in less than 1 picosecond (ps).

166 a simple way to realize a broadband perfect absorber in the visible and near-infrared (NIR) regions

167 technique that has been developed to detect absorbers in a sample.

168 odes in dye-sensitized solar cells and light absorbers in perovskite-based solar cells for electricit

169 ars attracted considerable interest as photo absorbers in PV applications with record efficiencies no

170 o-dimensional hybrid perovskites are used as absorbers in solar cells.

171 warmer gas that has been traced by metal ion absorbers in the circumgalactic medium.

172 dividual absorber decreases as the number of absorbers in the cluster increases and/or the inter-abso

173 istribution of both endogenous and exogenous absorbers in the mouse retina.

174 nstrate here that CDs act as excellent light-absorbers in two semibiological photosynthetic systems u

175 olarization independent, extremely efficient absorbers (in principle being capable to reach A > 99%)

176 induced hole transfer from a molecular light absorber, in the form of a free-base porphyrin, coupled

177 o the planar absorber, different dimensional absorbers including cylinders and spheres also exhibit t

178 This absorber integrates both the plasmonic resonances and th

179 combines the receiver front end circuit and absorber into a monolithic integrated device, eliminatin

180 Broadband absorbers introduced in this study perform better than n

181 Here, a spin wave absorber is demonstrated comprising a yttrium iron garne

182 high-temperature stable broadband plasmonic absorber is designed, fabricated, and optically characte

183 omnidirectional nanophotonic solar selective absorber is fabricated on a large scale using a template

184 backscattered when the crystallinity of the absorber is low but are absorbed for more crystalline ab

185 ed a structure in which the perovskite light absorber is placed between carrier-selective electron- a

186 r, development of ideal bandgap (1.3-1.4 eV) absorbers is pivotal to further improve PCE of single ju

187 An attractive feature of perovskite absorbers is the possibility of tailoring their properti

188 sign of single mode lasers, coherent perfect absorbers, isolators, and diodes.

189 ct of level alignment between the perovskite absorber layer and carrier-transporting materials on the

190 electro-optical properties of the perovskite absorber layer are most critical to device operation cha

191 l2 treatment, we obtain a well-sintered CdTe absorber layer from the new ink and demonstrate thin-fil

192 The absorber layer is only 100 nm thick, and can be processe

193 cing a photovoltaic device with a switchable absorber layer that dynamically responds to sunlight.

194 hylamine complex is re-formed, returning the absorber layer to the transparent state in which the dev

195 umination, photothermal heating switches the absorber layer-composed of a metal halide perovskite-met

196 record efficiency for sub-400 nm thick CdTe absorber layer.

197 tallic substrates can potentially be used as absorber layers for fabrication of low-cost, high-perfor

198 By incorporating Se in the sulfide film, absorber layers with 1.55 eV bandgap, ideal for single-j

199 ed that our method forced light to go around absorbers, leading to even higher signal improvement tha

200 se Kirchhoff's law prescribes that only good absorbers make good thermal emitters.

201 On the heels of metamaterial absorbers (MAs) which produce near perfect electromagnet

202 omposite spray coatings for use as a thermal absorber material for high-power laser calorimeters.

203 se as an alternative, highly efficient solar absorber material for photovoltaic application.

204 ctor material that has been considered as an absorber material in thin film solar cells due to its op

205 Tin sulfide (SnS), as a promising absorber material in thin-film photovoltaic devices, is

206 ameters in the range of 7-50 nm were used as absorber materials for electromagnetic waves.

207 metallic, in contrast to other 2D saturable absorber materials reported so far to be operative for m

208 eir growing potential as versatile saturable absorber materials.

209 the high-performance perovskite photovoltaic absorbers, methylammonium lead iodide (MAPbI3) and forma

210 d impedance matching between the emitter and absorber modes along with their coupling to the free-car

211 hosphates (TMPs) covalently bound to organic absorber molecules to form nanostructured superlattices.

212 (Ga(1-x)Zn(x))(N(1-x)O(x)) is a visible absorber of interest for solar fuel generation.

213 site in which the MWCNTs act as an efficient absorber of laser light while the much larger rGO sheets

214 radicals from H2O2, as well as an excellent absorber of microwave irradiation.

215 Hemodialysis patients are high absorbers of intestinal cholesterol; they benefit less t

216 Nitrophenols are well-known absorbers of near-UV/blue radiation and are considered t

217 ly atmosphere was free of the appropriate UV absorbers, of which ozone is the most important in the m

218 rates of diffusing molecules by clusters of absorbers on lattices of different packing symmetries.

219 development of nanomaterial-based saturable absorbers opening new avenues toward advanced photonic d

220 , we realize optically transparent broadband absorbers operating in the millimetre wave regime achiev

221 Our data suggests that the absorbers' operation can also be extended to microwave a

222 ffect nitrosamine accumulation in either the absorber or the washwater unit.

223 erials that range optically from pure photon absorbers or scatterers to simultaneous photon absorbers

224 es) and emerging technologies such as narrow absorber organic semiconductors or quantum nanocrystals.

225 ieved by a uniform vibration of the resonant absorber, owing to the Doppler effect, renders resonant

226 has not been demonstrated to date in a dual absorber photoelectrochemical cell.

227 n this initial study, integrated metasurface absorber pyroelectric sensors are implemented and tested

228 t gain-free omnidirectionally non-reflecting absorbers.Reflectionless absorption independent of the a

229 aster the absorption of CO2, the smaller the absorber required.

230 cells containing the lead-halide perovskite absorbers RPbX3 (R = organic cation; X = Br(-) or I(-)),

231 atic actuation of the plasmonic metamaterial absorber's position leads to a dynamic change of the Sal

232 addition, the fast development of saturable absorber (SA) towards the long wavelengths motivates the

233 n nanotube polymer composite based saturable absorber (SA), we demonstrated the laser output power of

234 Saturable absorbers (SA) operating at terahertz (THz) frequencies

235 round the 2 mum band, conventional saturable absorbers (SAs) possess small modulation depth and slow

236 ts through media consisting of subwavelength absorber-scatterer structures, an approach that should a

237 ters, and all the way to simultaneous photon absorbers, scatterers, and emitters in the UV-vis wavele

238 is transmitted through such a suspension of absorber-scatterers, in other words, how the various spa

239 pecifically designed semiconductor saturable absorber (SESAM) as the SA.

240 s because of the potential to scale down the absorber size, and the resulting capacitance and dark cu

241 Perovskite-absorber solar cells fabricated with spiro(TFSI)2 show i

242 he HTM in both dye-sensitized and perovskite-absorber solar cells in an inert atmosphere using spiro(

243 te dye-sensitized solar cells and perovskite-absorber solar cells, relies on an uncontrolled oxidativ

244 as a sample holder, and the influence of the absorber solution was evaluated.

245 monly attributed to the requirement that the absorber spatial distribution is heterogeneous relative

246 on par with those of notable selective solar absorbers (SSAs) in the literature, while the wide-angle

247 uses nanomechanical actuation of metasurface absorber strips placed near a mirror in order to control

248 l water splitting utilizes customized tandem absorber structures to mimic the Z-scheme of natural pho

249 a NIR BODIPY subcell and a matching "green" absorber subcell, complementary absorption is achieved,

250 uch higher possible efficiencies than single absorber systems.

251 ble as the higher bandgap absorber in a dual-absorber tandem device.

252 absorbing, yet CHA-SOA was a more efficient absorber than HXL-SOA.

253 metamaterials (GC-HMM) as multiband perfect absorber that can offer extremely high flexibility in en

254 t a semiconductor-based multilayer selective absorber that exploits the sharp drop in optical absorpt

255 emonstrate an infrared broadband metasurface absorber that is suitable for increasing the response sp

256 boron based solid samples, including neutron absorbers that are important in nuclear technology.

257 nd presents a new library of long-wavelength absorbers that efficiently populate long-lived T1 states

258 The crystalline solids are "black absorbers" that exhibit continuous absorptions spanning

259 s are platinized (Pt-TiO2) so that the light absorber (the dyad), the electron conduit (TiO2), and th

260 ss and therefore the thermal capacity of the absorber, the detector keeps the high response speed and

261 t using non-native genetically-encoded light-absorbers, thereby augmenting energy transfer and trappi

262 ions of flexible conductors, shock/vibration absorbers, thermal shock barriers, thermal insulation/fl

263 chnique uses a simultaneous variation of the absorber thickness and the excitation wavelength.

264 y and ultra-small thickness of the plasmonic absorber, this hybrid detector constitutes an ideal comp

265 at can be integrated with a Salisbury screen absorber to construct an absorbing membrane for a microb

266 ht is achieved by moving a thin metamaterial absorber to control its interaction with the standing wa

267 his method is not limited by the size of the absorber to form a sub-acoustic optical focus.

268 PVP-AuNPs can be a powerful absorber to influence the emission of the fluorophore, B

269 he size of radioactive inclusions within the absorber to scales below 50 nm such that decay products

270 nge of applications from ultrafast saturable absorbers to gas sensors to fillers for composite reinfo

271 ceeds 2%, a record for a single oxide photon absorber, to the best of our knowledge.

272 When placed on a silicon absorber under sunlight, such a blackbody preserves or e

273 A solar absorber, under the sun, is heated up by sunlight.

274 tal N-nitrosamines in the solvent within the absorber unit and upon a pressure-cooker treatment that

275 romoted total N-nitrosamine formation in the absorber unit at concentrations permitted in drinking wa

276 idative degradation of primary amines in the absorber unit, a process known to produce a wide spectru

277 s requires the use of multiple complementary absorbers, usually incorporated in tandem cells or in ca

278 e 3 to afford a pair of strong visible-light absorbers was also demonstrated.

279 r selectively removing nitrosamines from the absorber waterwash effluent with activated-carbon sorben

280 all of the decay energy is contained in the absorber, we measure a single spectral peak for each iso

281 Using metamaterial absorbers, we have shown that metallic layers in the abs

282 ility of synthesizing PT-symmetric saturable absorbers, where a nonlinear wave finds a lossless path

283 sensor with a metasurface-enabled ultra-thin absorber, which provides spectrally- and polarization-di

284 promising way to design electrically tunable absorbers, which may contribute toward the realization o

285 s, and a narrow-band near-infrared plasmonic absorber with 100% absorption efficiency, high quality f

286 y efficiency upon replacing the conventional absorber with a plasmonic absorber.

287 A broadband absorber with an average high absorption of 95% and a to

288 hole transfer coupling of a molecular light absorber with an Earth-abundant metal oxide catalyst by

289 rber coating and the spectral overlap of the absorber with the plasmonic modes.

290 city of a nanoengineered plasmonic thin-film absorber with the robustness and linear response of a th

291 a broadband polarization-independent perfect absorber with wide-angle near unity absorbance in the vi

292 hromophores that make up melanin as Gaussian absorbers with bandwidth related via Frenkel excitons.

293 rated sunlight requires spectrally selective absorbers with exceptionally low emissivity in the therm

294 y require the combination of efficient solar absorbers with high activity electrocatalysts for the hy

295 lesterol stone children were low cholesterol absorbers with intact homeostasis of cholesterol metabol

296 Thin-layer perfect absorbers with periodic hole arrays are designed at visi

297 ese complexes represent a new class of light absorbers with potential application as dyes for charge

298 at provides detailed chemical information of absorbers with sub-micrometer spatial resolution.

299 be converted into photovoltaic near-perfect absorbers with the advantage of harvesting the full pote

300 form, few-layer tungsten disulfide saturable absorber (WS2-SA).