ライフサイエンスコーパス: absorber

1 ent photon tunneling from the emitter to the absorber.

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

3 g the conventional absorber with a plasmonic absorber.

4 ermally function material as a switchable IR absorber.

5 oelectric device covered with a conventional absorber.

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

7 bled flexible and conformable wideband radar absorber.

8 arbazole (KR131) with compositive perovskite absorber.

9 uction in a bioreactor integrated with a gas absorber.

10 single photons in a deeply subwavelength 50% absorber.

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

12 the methylammonium moiety of the perovskite absorber.

13 his design and that of an effective acoustic absorber.

14 rmamidinium-cesium lead-trihalide perovskite absorber.

15 yed to further verify the performance of the absorber.

16 dex matching or the inclusion of a broadband absorber.

17 ta source and selection of the semiconductor absorber.

18 a multilayer VO(2) thin film based resonant absorber.

19 yme reactions are driven by artificial light absorbers.

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

21 dinium lead iodide (FAPbI3) perovskite solar absorbers.

22 tegration on surfaces of semiconductor light absorbers.

23 rent methods for fabricating selective solar absorbers.

24 ation of the dynamic distribution of optical absorbers.

25 ide double perovskites to compete with APbX3 absorbers.

26 thin the emerging Pb-based halide perovskite absorbers.

27 ssure oscillations in the air contacting the absorbers.

28 tentially nontoxic and defect-tolerant solar absorbers.

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

30 development of 1.5-1.6 eV bandgap perovskite absorbers.

31 port a mechanism to chemically stabilize PSC absorbers.

32 olors, corresponding to the bandgap of three absorbers.

33 hin films are excellent candidates for solar absorbers.

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

35 hiophene dendrimers that serve as two-photon absorbers.

36 and materials for the stabilization of light absorbers.

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

38 he waveguide were suppressed using spin wave absorbers.

39 ng signal from the aforementioned endogenous absorbers.

40 the solar cells could use narrower-band gap absorbers (1.2-1.4 eV).

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

42 ormamidinium) perovskite composites as light absorbers achieve enhanced efficiency and stability, giv

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

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

45 water oxidation with integration of a light absorber, an electron acceptor, an electron donor, and a

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

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

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

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

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

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

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

53 losses at interfaces between the perovskite absorber and the charge-transport layers.

54 and extraction losses between the perovskite absorber and the hole transport layer (HTL) is reported.

55 ectrodes functionalized with molecular light absorbers and catalysts.

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

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

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

59 absorbers (SAs) are considered as broadband absorbers and have been used in various studies in the p

60 et energy transfer between nanocrystal light absorbers and molecular acceptors suggests that these hy

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

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

63 All quantum dots are simultaneous absorbers and scatterers in the UV-vis wavelength region

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

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

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

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

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

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

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 Broadband absorbers are essential components of many light detecti

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

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

78 x) Cs(y) PbI(3-) (z) Br(z) ) as photovoltaic absorbers, as they enable easier processing and improved

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

80 mical device consisting of bottom p-Si light absorber, atomic layer deposition Al-ZnO passivation lay

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

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

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

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

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

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

87 Resonant absorbers based on nanostructured materials are promisin

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

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

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

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

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

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

94 erovskite deposited on top of the perovskite absorber, called the capping layer.

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

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

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

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

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

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

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

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

103 a unique kind of visible light metamaterial absorber comprising elliptical rings-shaped fractal meta

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

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

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

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

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

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

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

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

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

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

114 conceptually present blackbody-cavity solar absorber designs with nearly ideal spectrally selective

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

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

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

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

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

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

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

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

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

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

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

126 urement results shown that the proposed flat absorber exhibits absorption efficiency higher than 0.8

127 It was found that the proposed absorber exhibits average absorption of over 90% in the

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

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

130 regardless of polarization, while the curved absorber for 6.6-29 GHz (i.e., bandwidth of 126%) or for

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

132 and further its implementation as a thermal absorber for buildings' thermal comfort purpose.

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

134 establishes ZnSe as a state-of-the-art light absorber for photocatalytic and photoelectrochemical H(2

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

136 test the potential of Cu(3)VSe(4) NSs as an absorber for solar photovoltaic devices, Cu(3)VSe(4) NSs

137 olarization- and direction-selective perfect absorber for the infrared region is theoretically and ex

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

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

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

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

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

143 rted that employs carbon dots (CDs) as light absorbers for the conversion of lignocellulose into sust

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

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

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

147 Finally, the proposed absorber has thickness of 3.89 mm, corresponding to lamb

148 eving the broadband response of metamaterial absorbers has been quite challenging due to the inherent

149 optically transparent microwave surfaces and absorbers have been designed and fabricated by exploitin

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

151 tovoltaic devices fabricated from perovskite absorbers have reached power conversion efficiencies abo

152 { en}FA(0.5)MA(0.5)Sn(0.5)Pb(0.5)I(3) light absorbers have substantially enhanced air stability and

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

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

155 ckness ZrB(2) 150 mum Integral Fuel Burnable Absorber (IFBA) is an excellent burnable poison (BP) can

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

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

158 I(3)) solid-solution perovskite as the light absorber in PSCs, delivering promising efficiency of up

159 e-locked QCLs based on polaritonic saturable absorbers in a monolithic single-chip design.

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

161 Organic-inorganic lead halide perovskite absorbers in combination with electron and hole transpor

162 rint, indicating that the diverse electronic absorbers in eumelanin, regardless of transition energy,

163 Semiconducting absorbers in high-performance short-wave infrared (SWIR)

164 emonstrate three types of broadband acoustic absorbers in one-port and two-port systems: broadband ab

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

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

167 nergy bandgap are ideal candidates for light absorbers in tandem solar cells as well as fluorescent m

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

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

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

171 al measurements also show the ability of the absorber, in the Salisbury screen configuration, to achi

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

173 We apply this technique to various solar absorbers-including high-performance lead-iodide-based p

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

175 Broadband absorbers introduced in this study perform better than n

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

177 me alignment-free, a semiconductor saturable absorber is one of the most suitable devices.

178 Searching for Pb-free perovskite solar cell absorbers is currently an attractive research direction.

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

180 eous mixture with carbon nanodot (CND) light absorbers is studied for a range of different carbon dot

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

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

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

184 ases and pinhole formation in the perovskite absorber layer during aggressive aging.

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

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

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

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

189 compositionally engineered perovskite as an absorber layer, and Spiro-OMeTAD as a HTM, several group

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

191 essing and electronic bulk properties in the absorber layer.

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

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

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

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

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

197 been identified as a promising photovoltaic absorber material introduced as an alternate candidate t

198 2D perovskites as active absorber materials in PSCs are also summarized.

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

200 eir growing potential as versatile saturable absorber materials.

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

202 b fiber laser with a semiconductor saturable absorber mirror using TS-DFT.

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

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

205 cribes enantiomerically pure spiroconjugated absorber molecules using 1,1'-binaphthyl-2,2'-diol (BINO

206 er triplet energies for coupling with common absorbers) motivated us to assess the role of exciton de

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

208 ll devices based on the n = 4 perovskites as absorbers of both series exhibit promising performances,

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

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

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

212 onsists the integration of the GOC as a flat absorber on the top of a low iron glass or aluminium-bas

213 in one-port and two-port systems: broadband absorbers (one-port), broadband sparse absorbers (two-po

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

215 traps present in the bulk of the perovskite absorber or at the device heterointerfaces.

216 oclusters that either operate as a broadband absorber or with a reconfigurable reflection band throug

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

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

219 n moth wings forms a metamaterial ultrasound absorber (peak absorption = 72% of sound intensity at 78

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

221 lecular catalysts with low-cost, solid light absorbers presents a promising strategy to construct cat

222 This sound absorber provides moth wings with acoustic camouflage (6

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

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

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

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

227 Saturable Absorber (SA) is a key element of any passive mode-locke

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

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

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

231 ene (Gr) and Carbon nanotube (CNT) saturable absorbers (SAs) are considered as broadband absorbers an

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

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

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

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

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

237 ity to absorb dietary lactose and if lactose-absorbers should thus avoid these products.

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

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

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

241 Spectrally selective solar absorbers (SSAs), which harvest heat from sunlight, are

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

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

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

245 lization of low-cost metal make the proposed absorber suitable in varieties of photonics applications

246 uch higher possible efficiencies than single absorber systems.

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

248 o be 603/33 and 823/69 times more intense IR absorbers than the C-bonded isomers at the CCSD level of

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

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

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

252 ypothesized to function as a molecular shock absorber that mechanically stabilizes the sarcolemma of

253 ble interest in the exploration of new solar absorbers that are environmentally stable, absorb throug

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

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

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

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

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

259 l Zn diffusion, which can penetrate the full absorber thickness already at moderate temperatures.

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

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

262 to improve the bulk properties of perovskite absorbers through the formation of high-quality perovski

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

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

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

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

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

268 iplet exciton transfer from the PbS NC light absorber to the emitter and thus a higher photon upconve

269 re that is also a Lewis-base into perovskite absorbers to broaden their photoresponse and increase th

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 uggest that diverticula function as Helmholz absorbers turning the swim bladder into a high-pass filt

273 dband absorbers (one-port), broadband sparse absorbers (two-port), and broadband duct absorbers (two-

274 rse absorbers (two-port), and broadband duct absorbers (two-port).

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

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

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

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

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

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

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

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

283 e and broadband electromagnetic metamaterial absorber, which can cover either a flat or a bent geomet

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

285 inimize the number of resonances for compact absorbers, while it is beneficial for practical applicat

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

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

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

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

290 g wideband gap semiconductors as prospective absorbers with (3)H and (63)Ni sources.

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

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

293 based on multication mixed-halide perovskite absorbers with nonideal band gaps of 1.5-1.6 eV.

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

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

296 By integrating plasmonic metamaterial absorbers with pyroelectric detectors at the pixel level

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

298 The perovskite absorber, with a bandgap of 1.68 electron volts, remaine

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

300 context of optoelectronic applications, the absorber yields absorbance up to ~ 70% even with the inc