ライフサイエンスコーパス: optical property

1 ms enables the control of its electrical and optical properties.

2 at have shown many intriguing electrical and optical properties.

3 which is of vital importance to tailor their optical properties.

4 future refinements in the modelling of leaf optical properties.

5 dal biohybrid nanoparticles showing distinct optical properties.

6 considerable attention owing to the distinct optical properties.

7 various ordered structures to achieve novel optical properties.

8 not completely, irreversible changes in the optical properties.

9 nal modulation to the realization of tunable optical properties.

10 nment, and offer convenient readout of their optical properties.

11 ers, which helps achieve good electronic and optical properties.

12 aces exhibiting unusual linear and nonlinear optical properties.

13 structural coloration often yields emergent optical properties.

14 conform to objects' surface and change their optical properties.

15 ble surface area, and tunable electronic and optical properties.

16 ectronic devices due to their electronic and optical properties.

17 unusually high thermal stability and unique optical properties.

18 be their molecular electronic structures and optical properties.

19 xtremely anisotropic electronic, thermal and optical properties.

20 beneficial mechanical, energy conversion and optical properties.

21 signals or distorted by variations in tissue optical properties.

22 exhibit distinct electrical, mechanical and optical properties.

23 ectronics due to their unique electronic and optical properties.

24 tremely large wave vectors exhibiting unique optical properties.

25 ove 850 degrees C without degradation of its optical properties.

26 onal materials with desirable electronic and optical properties.

27 ophenes with tunable chemical, magnetic, and optical properties.

28 tightly bound excitons, which dominate their optical properties.

29 roperties can be insufficient to predict SOA optical properties.

30 of the doping concentration on their electro-optical properties.

31 d for decades, including how it manifests in optical properties.

32 ts of both linear and second-order nonlinear optical properties.

33 nanoparticle devices with precisely designed optical properties.

34 , can be engaged to dynamically change their optical properties.

35 the Ag domain, which in turn influences its optical properties.

36 ole in materials' mechanical, electrical and optical properties.

37 d, hence, for example, for in situ tuning of optical properties.

38 uding excitons and trions, that dominate the optical properties.

39 of their experimental and theoretical (chir)optical properties.

40 f membrane textures, surface chemistries and optical properties.

41 nd their complex viewing-direction-dependent optical properties.

42 nd strategies for the dynamic control of the optical properties.

43 field provides a new method to extend their optical properties.

44 to be reported to significantly modify their optical properties.

45 entimeters) and heterogeneous electrical and optical properties.

46 sing their unique and tunable electronic and optical properties.

47 an significantly affect their electrical and optical properties.

48 ts of strain on the electronic, magnetic and optical properties.

49 anotubes (SWNTs) offer unique electrical and optical properties.

50 potassium nanosensor (K(+) NS) modulates its optical properties (absorbance and fluorescence) accordi

51 While commonly utilized optical properties also correlate with DOM composition,

52 Anisotropic optical properties also give rise to a magnetic writing

53 ) has a dramatic impact on the corresponding optical properties and band energy structure, leading to

54 With the advantages of excellent optical properties and biocompatibility, single-strand D

55 spacer layer, which changes the metamaterial optical properties and causes a localized increase in em

56 sition method has a significant influence on optical properties and composition of the films, but neg

57 uding large absorption coefficients, tunable optical properties and controllable dimensions, high pho

58 Moreover, redox/optical properties and DFT calculations of (R2N)PPn/(R2N

59 g to direct electronic bandgaps, distinctive optical properties and great potential in optoelectronic

60 here are significant regional differences in optical properties and height and thickness of the CCLB.

61 ires characteristics of AuNPs such as unique optical properties and large surface area, SNPs as ampli

62 sure compression can systematically tune the optical properties and mechanical stability of the molec

63 aspects of conjugated polymer nanoparticles optical properties and phenomena, and discuss the curren

64 Our enhanced understanding of optical properties and recombination processes elucidate

65 We use an empirical model to quantify optical properties and sampling depth from sub-diffuse r

66 hts into the effect of the Pt dopants on the optical properties and stability of the cluster.

67 The optical properties and stability of the obtained silica

68 transfer model for explaining organic matter optical properties and suggest that future research shou

69 ccurate determination of the complete set of optical properties and the phase function of a turbid me

70 because of their bio-compatibility, tunable optical properties and their ability to be excited by in

71 chemical stability, magnetic, electrical and optical properties) and catalytic applications (e.g. oxy

72 c and crystalline structures, stoichiometry, optical properties, and integration with magnetooptical

73 new physical phenomena, novel electronic and optical properties, and new device concepts not observed

74 The relationship among leaf Chl, leaf optical properties, and photosynthetic biochemical capac

75 In order to relate DOM molecular weight, optical properties, and reactive species production, Suw

76 a reaction cycle intermediate with kinetics, optical properties, and reactivity indicative of an Fe(4

77 iocompatibility, highly functional surfaces, optical properties, and robust physical properties.

78 NPs, including large surface area and unique optical properties, and strong interaction of biotin wit

79 attention due to interesting electrical and optical properties, and their potential integration into

80 port the synthesis, structure determination, optical properties, and theoretical analysis of the elec

81 Optical properties appear to be particularly predetermin

82 tiscale natural fibers from wood have unique optical properties applicable to different kinds of opto

83 These distinctive optical properties are attributable to the folding of th

84 Their electrical and optical properties are examined relative to other p-type

85 The synthesis, structure, magnetic and optical properties are reported including, notably, inte

86 These dramatic enhancements in optical properties are similar to those of super-acid tr

87 While chiral optical properties are weak in most of naturally occurri

88 tenoid-shaped particles exhibit controllable optical properties as a result of their concave menisci,

89 unfavorable environments and maintain their optical properties associated with proton pumping.

90 al mechanical reinforcement, electrical, and optical properties at highly reduced volume fraction.

91 ecently shown to induce superconducting-like optical properties at temperatures far greater than the

92 asurement of aerosol physical, chemical, and optical properties at the megacity of Shanghai for two m

93 is disrupted, leading to a variation in the optical properties at the micrometer scale.

94 nt modification in electrical resistance and optical properties being capable of multi-modal readout.

95 omophoric electronic coupling with redox and optical properties being highly length-dependent.

96 The advantages of GNPs lie in its superior optical property, biocompatibility and versatile conjuga

97 nlinear metasurfaces with homogeneous linear optical properties but spatially varying effective nonli

98 reening quantum dots not only based on their optical properties, but also their surrounding surface t

99 bles the dynamic switching of the non-linear optical properties by controlling the arrangement of ant

100 rests in bioapplications due to their unique optical properties by converting near infrared excitatio

101 s that have the ability to reversibly change optical properties by electric charge insertion/extracti

102 The tunable optical properties by precise control of WS2 layers coul

103 We demonstrate tuning of the optical properties by taking advantage of the magnetic f

104 volume fulvic acid (FA) isolates (n = 6) for optical properties, C and N content, and (13)C NMR spect

105 models of transport, excitonic, and magneto-optical properties can be efficiently developed.

106 hin NWs, their composition and the resulting optical properties can be readily tuned by an anion-exch

107 are artificially engineered materials whose optical properties can be specifically tailored to manif

108 ptical functionality because the bandgap and optical properties can be tuned by changing the composit

109 cture, and hence well-defined electronic and optical properties, can be grown by self-assembly using

110 kable interest due to their unique nonlinear optical properties capable of converting incident near-i

111 erstand aspects such as aerosol composition, optical properties, cloud condensation, and ice nucleati

112 Their extraordinary electrical and optical properties combined with the abundance of the ra

113 The optical properties, composition and sources of the winte

114 (0.014-0.041 mug/ml in phantoms), and (III) optical-property corrected PpIX estimates were more high

115 state optical spectra defy simple structure-optical property correlations.

116 Quantitative understanding of retrieved BrC optical properties could be improved with more explicit

117 als, combined with their rich electronic and optical properties, could lead to new magnetic, magnetoe

118 asmonic nanostructures boast broadly tunable optical properties coupled with catalytically active sur

119 le also exhibiting the desired catalytic and optical properties derived from the integrated Au25 (SG)

120 xture volume comprises a surface layer whose optical properties differ substantially from those of th

121 These optical properties drive development and use of fluoresc

122 However, our knowledge of when the optical properties emerge in the hierarchical organizati

123 combined with large-area monolayer MoS2 for optical property enhancement and array processing, our r

124 ed for biomedical applications due to unique optical properties, established synthesis methods, and b

125 the outstanding structural, electronic, and optical properties for the development of a sustainable

126 tational studies supported interpretation of optical properties for the selected compounds.

127 Metamaterials, which derive their optical properties from sub-wavelength structures, have

128 e oxygenated hexagonal carbon framework with optical properties governed by its internal structure ra

129 The particles were characterized for their optical properties, growth rate, elemental composition,

130 materials, the coupling of polarization with optical properties has received, since 2009, renewed att

131 Dissolved organic matter optical properties have been attributed to a charge-tran

132 Existing studies on fluorophore optical properties have been focused almost exclusively

133 roduced small or negligible changes in their optical properties; however, when measurable, these chan

134 table imaging modality for reconstruction of optical properties in a highly scattering medium, such a

135 ications are contingent upon retaining their optical properties in an aqueous environment.

136 , can produce novel electronic, magnetic and optical properties in many materials.

137 odified counteranions can be used to control optical properties in materials.

138 uctures comprised of elements with different optical properties in order to achieve features such as

139 es have been made, tuning and modulating the optical properties in real time remains a challenge.

140 gh the compounds have similar electronic and optical properties in solution, they behave differently

141 bly separated will be subjected to different optical properties in the media through which they trave

142 chemical vapour deposited graphene has good optical properties in the mid-infrared range.

143 ctive bulk meta-structure with extraordinary optical properties in the visible range.

144 in living animals because of their excellent optical properties including large absorption coefficien

145 for such applications due to their inherent optical properties, including large anti-Stokes shift, d

146 Corrole derivatives exhibit a rich array of optical properties, including substituent-sensitive Sore

147 ic components are arranged can greatly alter optical properties, including tunable color and asymmetr

148 uctures were designed and fabricated and the optical properties investigated in the wavelength region

149 centers exhibiting different electronic and optical properties is a key step toward the bottom-up co

150 ngineer metamaterials with tunable nonlinear optical properties is crucial for nonlinear optics.

151 lids, giving rise to reversible switching of optical properties, magnetic exchange interactions, and

152 issolved organic carbon (DOC) concentration, optical properties, molecular size distribution, molecul

153 electronic energy transfer and the resulting optical properties, most of the current solution-based p

154 overcome in order to unlock many remarkable optical properties not present artificial optical system

155 The optical properties of a dimer type nanoantenna loaded wi

156 is the possibility to engineer a priori the optical properties of a disordered distribution in an am

157 urrents to access the molecular dynamics and optical properties of a fullerene layer.

158 report the design, synthesis, and nonlinear optical properties of a series of electron-rich thiophen

159 Here, we examine how the optical properties of a suspension of plasmonic nanopart

160 By taking advantage of the optical properties of a thin birefringent coating on the

161 of methylglyoxal uptake on the physical and optical properties of aerosol containing amines or ammon

162 With this novel measurement method the optical properties of airborne dust can be directly meas

163 Here, we describe optical properties of bistable bubble domain (BD) textur

164 novel sensor, which measures characteristic optical properties of blood, has been evaluated in an ex

165 otential avenue to fully exploit the electro-optical properties of blue phases, which have been hinde

166 ation, combining it with OD and studying the optical properties of both components and their combinat

167 The structural, morphological, and optical properties of both the batches of CdS quantum do

168 g growth may be used as a way to improve the optical properties of both the GaAs and ZnSe layers on e

169 tance, it has been a challenge to retain the optical properties of Bragg mirrors in optical systems a

170 The optical properties of BrC aerosol change in subtle ways

171 ive to black carbon (BC) alone, the combined optical properties of BrC and BC slow the net rate of pr

172 The chemical composition and optical properties of BrC chromophores were investigated

173 The molecular basis of the optical properties of chromophoric dissolved organic mat

174 n and scattering control.Controlling all the optical properties of dielectric waveguides is a challen

175 h for simultaneously controlling the diverse optical properties of dielectric waveguides.

176 sity Functional Theory (DFT) analysis of the optical properties of dilute-As GaN1-xAsx alloys with ar

177 The optical properties of dissolved organic matter influence

178 for the first time, the observed changes in optical properties of DNA-wrapped SWCNTs with ionic stre

179 lecular weight and chemical reduction on the optical properties of DOM (absorbance and fluorescence)

180 lyze trends in the electronic structures and optical properties of expanded, contracted, and isomeric

181 We report on the nonlinear optical properties of few-layer GaSe using multiphoton m

182 on conditions, particle characteristics, and optical properties of fresh and photochemically processe

183 In this work, we unveil the optical properties of gap surface plasmons in silver nan

184 We investigated the optical properties of Ge nanocrystals surrounded by Ge3N

185 In this paper, we characterize the nonlinear optical properties of GeSbS glasses, and show negligible

186 Combining the chemical and optical properties of GO with the versatility of the VHH

187 adsorbents are claimed to be the origin for optical properties of GO.

188 ion of the silver shell, and the anisotropic optical properties of gold nanorods were maintained.

189 The electronic and optical properties of graphene are greatly dependent on

190 and impact of quinones/hydroquinones on the optical properties of HS and CDOM.

191 orically struggled to match the high-quality optical properties of II-VI quantum dots.

192 in a solid material, play a key role in the optical properties of insulators and semiconductors.

193 We demonstrate the high structural and optical properties of InxGa1-xN epilayers (0 </= x </= 2

194 Trends in the electronic structures and optical properties of isomeric porphyrins are examined b

195 discuss theoretical methods for modeling the optical properties of lanthanide-doped materials.

196 The structural, transport, and optical properties of LAO/STO heterostructures grown on

197 ia opsins by modifying fundamental nonlinear optical properties of light interacting with the retinal

198 Optical properties of lithium triborate (LBO) in the ter

199 common owing to the spatiotemporally varying optical properties of living specimens.

200 escence, that are responsible for the unique optical properties of materials and structures found in

201 work and the excitonic model to describe the optical properties of melanin.

202 The catalytic and optical properties of metal nanoparticles can be combine

203 -probes is of immense interest due to unique optical properties of metal nanoparticles.

204 r the possibility of studying the non-linear optical properties of metal-organic structures as well a

205 The optical properties of metallic nanoparticles with nanome

206 The optical properties of metallic nanoparticles with plasmo

207 We studied the optical properties of metalorganic chemical vapour depos

208 Syntheses and optical properties of mono- and bis-chromene-annulated b

209 of T-Hg(2+)-T recognition mechanism with the optical properties of MWCNTs on lateral flow strip, opti

210 for the first time, the linear and nonlinear optical properties of natural silk fibers have been stud

211 We study optical properties of near-infrared absorbing colloidal

212 tical description of the electrochemical and optical properties of Ni and NiFe oxyhydroxide electroca

213 Physical geometry and optical properties of objects are correlated: cylinders

214 re we demonstrate an approach for decoupling optical properties of objects from their physical shape

215 Exploration of optical properties of organic crystalline semiconductors

216 useful imaging probes, the limited intrinsic optical properties of peptides must be overcome.

217 ings provide insights to improve the electro-optical properties of perovskite thin films towards larg

218 this Review gives emphasis to the nonlinear optical properties of photoactive materials for the func

219 of magnitude, giving simultaneous access to optical properties of plasmonic metamaterials, as well a

220 ents of fuel-use and emissions and real-time optical properties of pollutants from traditional and al

221 switches relying on the intrinsic nonlinear optical properties of push-pull substituted azobenzenes.

222 We provide ways of characterizing the optical properties of SERRS nanoparticles using UV/VIS a

223 tion and photoluminescence and show that the optical properties of single crystals are almost identic

224 This paper exploits the chirality-dependent optical properties of single-wall carbon nanotubes for a

225 s techniques have been exploited to tune the optical properties of such systems, the presence of exte

226 nd surface in determining the electronic and optical properties of the 58e nanoclusters.

227 odoluminescence (CL) spectra showed that the optical properties of the alpha-Si3N4 nanowires can be c

228 ) from the ocean influences the chemical and optical properties of the atmosphere, and the olfactory

229 iometric imaging is strongly affected by the optical properties of the brain.

230 The emerging optical properties of the degraded solvent present chall

231 ain extensibility, toughness and potentially optical properties of the dissociation products are tuna

232 For low vacancy doping levels the NIR optical properties of the dually plasmonic NPCs are dete

233 both the material quality and the favorable optical properties of the Eu ions.

234 riant gammaS-G18V, dramatically altering the optical properties of the eye lens.

235 First, optical properties of the individual pigment chromophore

236 The optical properties of the layers have been studied by co

237 aced on the analytical tools for probing the optical properties of the luminescent nanocrystals.

238 The optical properties of the modified HBC were investigated

239 orphology, crystal structures, chemical, and optical properties of the MoS2 QDs were characterized by

240 The optical properties of the NPCs can be reversibly switche

241 Structural and electro-optical properties of the perovskite absorber layer are

242 hemically polymerized and the electrical and optical properties of the resulting conductive polymer h

243 The unique optical properties of the resulting nanostructure are hi

244 on process brings about a dramatic change in optical properties of the sample-a change in the color o

245 l the structural, electronic, mechanical and optical properties of the single-layer bismuth iodide (B

246 This changes the optical properties of the strongly coupled plasmonic str

247 cal methods are exploited to investigate the optical properties of the substrates.

248 se), and these have a profound effect on the optical properties of the system, for both one and two p

249 ser optical tweezers can probe the nonlinear optical properties of the trapped species with applicati

250 Indeed, the "design principles" shaping the optical properties of these materials seem to be well ex

251 o model the structural, electrochemical, and optical properties of these materials.

252 which allowed for active manipulation of the optical properties of these molecules by using competing

253 The optical properties of these novel fluorophores have been

254 A systematic characterization of the optical properties of these structures as a function of

255 r potential to manipulate the electrical and optical properties of this class of materials, notwithst

256 Cancer is known to alter the local optical properties of tissues.

257 ing the ability to modify the electronic and optical properties of twisted bilayer graphene with dopi

258 Here, we introduce a method for probing the optical properties of two-dimensional materials via near

259 demonstrated by studying the anisotropic THz optical properties of uniaxial and biaxial oxide crystal

260 s to achieve a very strong dependence of the optical properties on the external environment.

261 The influence of particle size and optical properties on the stability of fish oil-in-water

262 hotonic media with complete control over the optical properties provide a platform for broadband cont

263 ealed a high degree of similarity between RI-optical property relationships across DOM samples of div

264 To date, their nonlinear optical properties remain relatively unexplored.

265 i-responsive polymers (SRPs) exhibit tunable optical properties responding to external stimuli and sh

266 thin metasurface coating can control several optical properties simultaneously over a broad frequency

267 We show that optical properties such as reflectivity and spectral pos

268 The results indicate that the optical properties, such as the lidar backscatter, the d

269 All the dyes exhibit redox and optical properties suitable for cascade energy transfer

270 Our results demonstrate that optical properties suitable for photovoltaic application

271 erials (as-WS2) exhibit distinctly different optical properties than transferred WS2 (x-WS2).

272 able assembly, unveiling exquisitely tunable optical properties that are predicted and explained both

273 oxide-insulator stack and discuss the useful optical properties that arise from combining both phenom

274 dots to exhibit size-tunable electronic and optical properties that enable a wide range of opto-elec

275 ge is to realise a technique of tuning their optical properties that is both fast and efficient.

276 ge is to realise a technique of tuning their optical properties that is both fast and efficient.

277 he BCeq is the mass of ideal BC with defined optical properties that, upon deposition on the aethalom

278 icantly influence electrochemical and linear optical properties, the orientation of the pyrimidine ri

279 For each system, the key optical properties, the principal experimental technique

280 Due to their unique optical properties, these films hold much promise for us

281 erms) have distinct anatomies but convergent optical properties; they all produce angle-dependent sca

282 ence throughout the exchange, allowing their optical properties to be observed in real time, in situ.

283 By coupling strong changes in optical properties to subtle differences in fluid behavi

284 The aerosol optical properties tracked include estimates of total co

285 artificial materials exhibiting fascinating optical properties unavailable in naturally occurring su

286 t can undergo substantial variation of their optical properties upon electron stimulus are of high in

287 ery well to external fields and change their optical properties upon such stimuli.

288 Dynamic control of conductivity and optical properties via atomic structure changes is of te

289 Using optical properties, we described DOM variation across fi

290 The stabilized colloids' optical properties were studied through optical absorpti

291 The measured THz optical properties were then analyzed in terms of refrac

292 erence for high-precision measurement of the optical properties where the speckle can severely distor

293 and a giant CdS shell have shown remarkable optical properties which are promising for applications

294 ctive size tunable electronic, catalytic and optical properties which opened new opportunities for de

295 exchange providing facile tunability of the optical properties, which is usually achieved by mixing

296 roperties (O:C), yet significantly different optical properties, which was attributed to differences

297 pounds give rise to interesting physical and optical properties with applications in biomedicine and

298 t of excitons, control of the electronic and optical properties with strain engineering, or unconvent

299 n additional degree of freedom for adjusting optical properties with the angle of inclination, in add

300 nducting materials (excellent electrical and optical properties) with those of synthetic polymers (me