ライフサイエンスコーパス: plasmon

1 nsing capabilities of metal nanowire surface plasmons.

2 on InSb as a tunable coupler for THz surface plasmons.

3 ing spectra of the incident nanowire surface plasmons.

4 hot electrons from localized and propagating plasmons.

5 standing of phonon coupling with photons and plasmons.

6 OAM are derived, i.e., photons, phonons, and plasmons.

7 adiative decay of tunnelling-induced surface plasmons.

8 to the electrical generation and control of plasmons.

9 ointing toward the possibility of supporting plasmons.

10 dentify features associated with chiral edge plasmons, a signature that robust edge channels are intr

11 us structures combined with their broad band plasmon absorption could pave the way for novel and comp

12 es C, which addresses a major shortcoming in plasmon actuated cargo delivery systems.

13 pling between graphene mid-infrared (mid-IR) plasmons and IR active optical phonons in silicon nitrid

14 eing searched, especially those with tunable plasmons and low loss in the visible-ultraviolet range.

15 These modes include surface plasmons and quasi-guided modes, and by tailoring the ab

16 lution is discussed, using localized surface plasmons and surface plasmon polaritons to create confin

17 tions cannot be considered as fully coherent plasmons and they are damped even in the optical limit,

18 it a linear dispersion (thus called acoustic plasmons) and a further reduced wavelength, implying an

19 s, local electromagnetic fields (tip-induced plasmons), and molecular vibrations.

20 trons generated by localized and propagating plasmons, and demonstrate wavelength-controlled polarity

21 Graphene plasmons are known to offer an unprecedented level of co

22 The correlated plasmons are tunable: they diminish as extra oxygen plan

23 Supported by theoretical calculations, these plasmons arise from the nanometre-spaced confinement of

24 Although plasmon-assisted hot carriers in metals have already ena

25 lattice are greatly amplified by the surface plasmon at the interface of the graphene and the ZnO.

26 making borophene the first material with 2D plasmons at such high frequencies, notably with no neces

27 a unique interplay of excitons, phonons, and plasmons at the nanoscale.

28 ers to generate hot carriers by slowing down plasmons at the taper apex.

29 tropy, can further permit the fine-tuning of plasmon behaviors in borophene, potentially a tantalizin

30 Resonant coupling of plasmons between the gold grating and graphene result in

31 olling, detecting and generating propagating plasmons by all-electrical means is at the heart of on-c

32 eraction between the dye dipoles and surface plasmons can be finely tuned by coupling the dye molecul

33 Such plasmons commonly occur in metals, but many metals have

34 probably due to lower oscillator strength of plasmon compared to the coronene.

35 anced electromagnetic field generated by the plasmon coupling between sharp tips and cores of two Au

36 cantly different dipolar and charge transfer plasmon (CTP) resonances, respectively.

37 the metal gate below the graphene, and that plasmon damping at positive carrier densities is dominat

38 riers excited via Landau damping (during the plasmon decay) are responsible for the photocatalytic pr

39 The unavoidable energy loss from plasmon decay, initially seen as a detriment, has now ex

40 ere, we present an all-graphene mid-infrared plasmon detector operating at room temperature, where a

41 Specifically, the dual-plasmon device produces a net photocurrent whose polarit

42 ducer (NOFT) that utilizes strong near-field plasmon-dielectric interactions to measure local forces

43 ts indeed mimic a 2D electron gas, and their plasmon dispersion in the small wavevector (q) limit acc

44 We clarify mechanistic questions regarding plasmon-driven chemistry and nanoscale photocatalysis wi

45 Empirical evidence of plasmon-driven electron transfer is provided for the fir

46 demonstrates the single molecule response of plasmon-driven electron transfer occurring in single nan

47 ng that are highlights of recent examples of plasmon-driven hot electron photochemical reactions with

48 ce converts the natural decay product of the plasmon-electronic heat-directly into a voltage through

49 Plasmon-enhanced electromagnetic fields in an array of g

50 nance of the GNR array, indicating a surface-plasmon-enhanced excitation and radiative mechanism for

51 of plasmon-mediated chemical transformations.Plasmon-enhanced photocatalysis holds promise for the co

52 is study can facilitate the incorporation of plasmon-enhanced transition metal dichalcogenide structu

53 .The creation of energetic electrons through plasmon excitation has implications in optical energy co

54 The creation of energetic electrons through plasmon excitation of nanostructures before thermalizati

55 propagation associated with the diffractive plasmon excitation, our waveguides provide polarization

56 e dielectric grating to optimize the surface plasmon excitation.

57 id-Infrared fingerprint region with a single plasmon excitation.

58 interference effects associated with surface plasmon excitations at a single metal-dielectric interfa

59 Plasmon excitations can be dynamically switched off by l

60 and graphene result in strong enhancement of plasmon excitations in the atomic monolayer.

61 on of the grating is hidden, and the surface plasmon excitations, though localized at the surface, ar

62 en conducted on electrochemistry mediated by plasmon excitations.

63 ell interpreted by the dispersion of surface plasmon excited in the air TiO2 InSb trilayer system.

64 precision allows one to systematically tune plasmon-excition interaction strength and decay lifetime

65 The unique ability to control surface plasmon/exciton interactions within such superlattice mi

66 r, and GaAs as an active mediator of surface plasmons for enhancing carrier generation and photon emi

67 electric function allow one to calculate the plasmon frequencies (omega) in the selected example stru

68 These correlated plasmons have multiple plasmon frequencies and low loss in the visible-ultravio

69 The plasmon frequencies that are not damped by single-partic

70 ion limit through the excitation of graphene plasmons (GPs).

71 These correlated plasmons have multiple plasmon frequencies and low loss

72 The near-field plasmon hybridization between individual Ag nanodisks an

73 Plasmon hybridization theory, inspired by molecular orbi

74 plasmonic antennas: Structural asymmetry and plasmon hybridization through strong coupling.

75 We reveal the presence of intrinsic 2D Dirac plasmons in 3D nanoporous graphene disclosing strong pla

76 monstrate real-space imaging of acoustic THz plasmons in a graphene photodetector with split-gate arc

77 over an anomalous form of tunable correlated plasmons in a Mott-like insulating oxide from the Sr1-xN

78 real-space imaging of strongly confined THz plasmons in graphene and 2DEGs has been elusive so far-o

79 however, electrical detection of propagating plasmons in graphene has not yet been realized.

80 re typically generated from either localized plasmons in metal nanoparticles or propagating plasmons

81 They range from light waves or surface plasmons in nanoplasmonic devices to sound waves in acou

82 asmons in metal nanoparticles or propagating plasmons in patterned metal nanostructures.

83 lt of non-radiative relaxation pathways, the plasmons in such sub-nanometre cavities generate hot cha

84 an improved field confinement, analogous to plasmons in two-dimensional electron gases (2DEGs) near

85 unique means by which to in situ realize the plasmon-induced effects toward the target reaction.

86 nocages with hollow interior performed newly plasmon-induced effects, which was characteristic of pho

87 Such plasmon-induced electrochemical processes open up new po

88 Plasmon-induced fluorescence enhancement was found to be

89 Here we report plasmon-induced formation of nanoscale quantized conduct

90 suppression of peroxide formation instead of plasmon-induced heating that would cause a negative effe

91 We concluded that the plasmon-induced hot electron transfer governed the suppr

92 simultaneously generate these heterogeneous plasmon-induced hot electrons and exploit their cooperat

93 unications, and photoconversion applications.Plasmon-induced hot electrons have potential application

94 Plasmon-induced hot-electron generation has recently rec

95 Plasmon-induced phenomena have recently attracted consid

96 The plasmons intensity, energy, and depth of interface plasm

97 r photonic applications due to their exciton-plasmon interactions.

98 demonstrate better performance when surface plasmon is located in front of a solar cell.

99 of metal nanoparticles and their associated plasmons is currently enabling many promising applicatio

100 l catalyze studies involving quantum optics, plasmon laser physics, strong coupling, and nonlinear ph

101 intuitive, first-order interference model of plasmon-light interactions, we demonstrate a simple and

102 als and reaffirms the practical potential of plasmon-mediated chemical transformations.Plasmon-enhanc

103 ectron microscopy to stimulate and image the plasmon-mediated growth of triangular Ag nanoprisms in s

104 The investigation highlights the scope of plasmon-mediated light emission as a unique probe of hig

105 Herein, a near-ideal plasmon-mediated photocatalyst system is developed.

106 Cs is suitable for the construction of other plasmon-mediated photocatalysts.

107 Plasmon-mediated photocatalytic systems generally suffer

108 of patterned monomolecular layers in surface plasmon microscopy (SPM) is suggested.

109 For this purpose, a high-resolution plasmon microscopy was used.

110 manipulate strong coupling between the Bragg-plasmon mode supported by an organo-metallic array and m

111 reedom in graphene, including the collective plasmon modes via the Coulomb interaction, which opens u

112 ime domains have inspired the development of plasmon nanolasers based on mode analysis and time-depen

113 In contrast, plasmon nanolasers can overcome the diffraction limit of

114 Plasmon nanolasers designed by band-structure engineerin

115 oscale to the nanoscale, with an emphasis on plasmon nanolasers.

116 perimental results that rear-located surface plasmon on bare metallic nanoparticles is preferred, the

117 corresponding to the coupling of individual plasmon oscillations at medium- and substrate-related di

118 The intensity ratio between plasmon peak of Au nanoparticles and in-plane dipolar pe

119 ature, which is a manifestation of increased plasmon-phonon coupling strength.

120 the existence of a thermally excited hybrid plasmon-phonon mode.

121 dy observes increased modal splitting of two plasmon-phonon polariton hybrid modes with temperature,

122 ering from STV-NPs is excited by the surface plasmon polariton and collected from an objective lens m

123 We report longer surface plasmon polariton propagation distance based on crystall

124 First, long-range surface plasmon polariton waveguides show propagation distances

125 rt a guiding approach that integrates hybrid plasmon polariton with dielectric-loaded plasmonic waveg

126 rid structure mediated by an exciton-surface plasmon polariton-exciton conversion mechanism, allowing

127 ns intensity, energy, and depth of interface plasmon-polariton penetration were studied by scanning r

128 -thin ThermoPhotoVoltaic cells using surface-plasmon-polariton thermal emitters, that the resonant na

129 us applications of PINEM have imaged surface plasmon-polariton waves on conducting nanomaterials.

130 Surface-plasmon-polariton waves propagating at the interface bet

131 for sub-diffractional modes in comparison to plasmon-polariton-based nanophotonics.

132 s of microns, mediated by an exciton-surface-plasmon-polariton-exciton conversion mechanism.

133 circuits based on active control of Surface Plasmon Polaritons (SPPs) at degenerate PN(+)-junction i

134 materials via near-field coupling to surface plasmon polaritons (SPPs).

135 using localized surface plasmons and surface plasmon polaritons to create confined excitation volumes

136 surface that supports propagation of surface plasmon polaritons with a deposited gold layer, which ex

137 rough a glass hemisphere, generating surface plasmon polaritons.

138 ne, electrically tunable and highly confined plasmon-polaritons were predicted and observed, opening

139 e allows for low loss propagation of surface plasmon-polaritons, as evidenced by comparing the reflec

140 ects involving electron-phonon interactions, plasmons, polarons, and a phonon analog of the vacuum Ra

141 Resonant optical excitation of surface plasmons produces energetic hot electrons that can be co

142 Here, we use graphene plasmons, propagating at extremely slow velocities close

143 hotocurrent maps are used to investigate the plasmon propagation and interference, decay, thermal dif

144 eature collective oscillations of electrons (plasmons), providing huge electromagnetic fields on the

145 noassay (10 min) using a fiber-optic surface plasmon resonance (FO-SPR) biosensor for detection of IF

146 F-93, are grown on fiber optic based surface plasmon resonance (FO-SPR) sensors.

147 d, sensitive and multiplexed imaging surface plasmon resonance (iSPR) biosensor assay was developed a

148 ors based on utilizing the localized surface plasmon resonance (LSPR) and extraordinary optical trans

149 e and saliva) by combining localized surface plasmon resonance (LSPR) and molecular imprinted polymer

150 s suitable for multiplexed localized surface plasmon resonance (LSPR) biosensing have been created by

151 pressure, resulting in its localized surface plasmon resonance (LSPR) intensity change of in-plane di

152 ediated by excitation of a localized surface plasmon resonance (LSPR) is a prototype example of such

153 in molecule influences the localized surface plasmon resonance (LSPR) measurement response and provid

154 es of sensors based on the localised surface plasmon resonance (LSPR) of gold nanoparticles deposited

155 Here, we introduce a localized surface plasmon resonance (LSPR) sensing approach to quantitativ

156 good conductivity and high localized surface plasmon resonance (LSPR) sensitivity.

157 high surface sensitivity, localized surface plasmon resonance (LSPR) sensors have proven widely usef

158 An operando localized surface plasmon resonance (LSPR) spectrometer was utilized to ac

159 ematically investigate the localized surface plasmon resonance (LSPR)-coupled fluorescence enhancemen

160 ey exhibit the property of localised surface plasmon resonance (LSPR).

161 y quartz crystal microbalance (QCM), surface plasmon resonance (SPR) and X-ray photoelectron spectros

162 hotonic-based detection systems like Surface Plasmon Resonance (SPR) assays, Impedance-based method,

163 e and spermidine, the characteristic surface plasmon resonance (SPR) band of Tyr-Au NPs was red-shift

164 steps toward a rapid cost-effective surface plasmon resonance (SPR) based method for measuring the R

165 clic polymer chains, and show unique surface plasmon resonance (SPR) behaviors.

166 A label-free and enzyme-free surface plasmon resonance (SPR) biosensing strategy has been dev

167 In this work, we have presented a surface plasmon resonance (SPR) biosensor technique for the dete

168 affinity constants determined using surface plasmon resonance (SPR) biosensor technology are 262 +/-

169 age of pregnancy, a GO-peptide-based surface plasmon resonance (SPR) biosensor.

170 Surface plasmon resonance (SPR) biosensors are most commonly app

171 d environments, demonstrating that a surface plasmon resonance (SPR) can be excited in this case.

172 olecules and examine a generation of surface plasmon resonance (SPR) for plasmonic sensing.

173 good agreement with that measured by surface plasmon resonance (SPR) for the same binding reaction.

174 ting peptides in a hydrolysate using Surface Plasmon Resonance (SPR) for their antioxidant properties

175 and robust; it can be used with most surface plasmon resonance (SPR) imaging instruments.

176 A simplified coupling of surface plasmon resonance (SPR) immuno-biosensing with ambient i

177 Surface plasmon resonance (SPR) immunosensor using 4-mercaptoben

178 Surface Plasmon Resonance (SPR) in combination with different am

179 sorbed on graphene oxide (GO)-coated Surface Plasmon Resonance (SPR) interfaces.

180 Surface Plasmon Resonance (SPR) is a powerful technique for stud

181 Surface plasmon resonance (SPR) is the current standard tool use

182 We have used temperature gradient surface plasmon resonance (SPR) measurements to quantitatively e

183 Here we show the potential of surface plasmon resonance (SPR) method coupled to atomic force m

184 rojunction system, which include the surface plasmon resonance (SPR) of Au nanoparticles, low overpot

185 strate the capabilities of localized surface plasmon resonance (SPR) phenomenon to study non-covalent

186 and monkey antiheroin antibodies by surface plasmon resonance (SPR) revealed low nanomolar antiserum

187 A Surface Plasmon Resonance (SPR) sensor chip consisting of four s

188 A chip-based ultrasensitive surface plasmon resonance (SPR) sensor in a checkerboard nanostr

189 Moreover, surface plasmon resonance (SPR) showed that longer chain of synt

190 Surface plasmon resonance (SPR) spectroscopy is an advanced tool

191 l amide derivatives were screened by surface plasmon resonance (SPR) to determine the binding dissoci

192 Atomic force microscopy (AFM), surface plasmon resonance (SPR), and molecular simulations were

193 ng fluorescence, Raman spectroscopy, surface plasmon resonance (SPR), electrochemiluminescence and co

194 rmal titration calorimetry (ITC) and surface plasmon resonance (SPR), respectively.

195 Using surface plasmon resonance (SPR), we found that IL-1RAcP also doe

196 With surface plasmon resonance (SPR), we present this diversified col

197 ly recognizable color change, due to surface plasmon resonance (SPR), which occurs in about 30min of

198 surfaces on sensing films for use in surface plasmon resonance (SPR)-based immunoaffinity biosensors.

199 Surface plasmon resonance (SPR)-biosensor experiments show that

200 und VU0463271 was demonstrated using surface plasmon resonance (SPR).

201 m albumin (BSA) with AP and AS using surface plasmon resonance (SPR).

202 ric, and 10(3) and 10(4)L.mol(-1) by surface plasmon resonance (steady-state equilibrium and kinetic

203 f native state mass spectrometry and surface plasmon resonance a 3-unsubstituted 2,4-oxazolidinedione

204 its monomeric form; (ii) ranking, by surface plasmon resonance affinity measurements, of the resultin

205 orescein isothiocyanate-probing, and surface plasmon resonance analysis.

206 We used surface plasmon resonance and cell-based assays to investigate t

207 Surface plasmon resonance and cell-binding assays indicated that

208 Surface plasmon resonance and cellular thermal-shift-assays conf

209 Surface plasmon resonance and co-immunoprecipitation confirmed t

210 quantified binding interactions with surface plasmon resonance and fluorescence polarization.

211 By using surface plasmon resonance and fluorescence spectroscopy we here

212 Combining surface plasmon resonance and high-resolution mass spectrometry

213 Using surface plasmon resonance and leakage assays with model vesicles

214 Here, using surface plasmon resonance and neutron reflection, we characteriz

215 Hits were validated by surface plasmon resonance and X-ray crystallography.

216 erformed allergen binding studies by surface plasmon resonance as well as flow cytometry.

217 to exhibit metallic behavior, with a surface plasmon resonance band around 510 nm.

218 abrication and characterization of a surface plasmon resonance based fiber optic xanthine sensor usin

219 hat our in-house developed Localized Surface Plasmon Resonance biosensor with self-assembly gold nano

220 The contribution of plasmon resonance confinement to the abnormal lower ther

221 We present three experimental surface plasmon resonance data sets, in which antibody residues

222 Surface plasmon resonance diffraction and electrophoretic mobili

223 o induce an enhancement of localized surface plasmon resonance due to the coupling of plasmonic field

224 Plasmon resonance energy transfer from the Au NPs to the

225 Using real-time surface plasmon resonance experiments and interaction studies in

226 a combination of X-ray diffraction, surface plasmon resonance experiments and molecular dynamics sim

227 Surface plasmon resonance experiments resulted in the validation

228 trated in co-immunoprecipitation and surface plasmon resonance experiments.

229 The giant surface plasmon resonance gives rise to strong enhancement of th

230 Plasmon resonance heterogeneities were identified and st

231 Competition mass spectrometry and surface plasmon resonance identified new monomer complexes, as w

232 Surface plasmon resonance imaging (SPRi) was used as a detection

233 nucleotide polymorphisms (SNPs) on a surface plasmon resonance imaging sensor is investigated.

234 nt nature corresponding to localized surface plasmon resonance in present nanocages can potentially o

235 Ga-rich GFO NCs exhibit a localized surface plasmon resonance in the near-infrared at approximately

236 In case of coronene, a clear signature of plasmon resonance is observed in the analysis of forward

237 Herein, Biacore surface plasmon resonance is used to identify an antibody bindin

238 plane, which leads to a drastic narrowing of plasmon resonance lineshapes (down to a few nm full-widt

239 mes higher than that of conventional surface plasmon resonance measurements.

240 -ray photoelectron spectroscopy, and surface plasmon resonance methods.

241 a-reactor geometry efficiently harnesses the plasmon resonance of aluminum to supply energetic hot-ca

242 I) taking advantage of the localized surface plasmon resonance of gold nanoparticles (AuNPs) synthesi

243 hrough gold nanorods whose localized surface plasmon resonance overlaps with the excitation laser.

244 f electrically-excitable cells using surface plasmon resonance phenomena.

245 Surface plasmon resonance revealed that both small molecules wer

246 Surface plasmon resonance showed a NOTA-conjugated ligand bindin

247 Antibody kinetics determined by Surface Plasmon Resonance showed that adjuvanted G generated 10-

248 Cross-linking experiments as well as surface Plasmon resonance showed that Fre interacts with MsrQ to

249 Surface plasmon resonance shows that the affinity of human CD1d-

250 e, we used X-ray crystallography and surface plasmon resonance spectroscopy of alpha7-acetylcholine-b

251 lycosaminoglycan binding ability, as surface plasmon resonance spectroscopy showed that nitration red

252 monstrated in ligand overlay assays, surface plasmon resonance studies and SPOT peptide arrays.

253 Mechanistically, surface plasmon resonance studies identified high-affinity inter

254 cribes fluorescent, luminescent, and surface plasmon resonance systems.

255 Here a novel surface plasmon resonance technique (SPR) is developed and used,

256 We have configured biosensor-based surface plasmon resonance to directly measure the affinity and k

257 We utilized surface plasmon resonance to identify and measure PDGF-to-VEGFR

258 anoparticle characteristic localized surface plasmon resonance wavelength redshifts, and the shift am

259 sis, NMR, isothermal calorimetry and surface plasmon resonance we demonstrate that Rif1 is a high-aff

260 ring, nuclear magnetic resonance and surface-plasmon resonance which indicated that, in addition to t

261 sity 10(22) cm(-3), strong localized surface plasmon resonance) and low-chalcocite CuLiS NCs (Eg = 1.

262 Eg = 1.2 eV, intrinsic, no localized surface plasmon resonance), and back.

263 Using surface plasmon resonance, analytical rheology, and hydrogen-deu

264 rumentation involving nanomaterials, surface plasmon resonance, and aptasensors have developed innova

265 1.8 eV ( approximately 688 nm) is due to the plasmon resonance, arising from the large carrier densit

266 versible immobilization reagents for surface plasmon resonance, as fluorescently labelled monomeric d

267 sults of five independent techniques-surface plasmon resonance, electrochemical impedance spectroscop

268 in complexes and RTA was examined by surface plasmon resonance, isothermal titration calorimetry, mic

269 ng isothermal titration calorimetry, surface plasmon resonance, nuclear magnetic resonance, and X-ray

270 Surface plasmon resonance, performed under different buffer cond

271 -sensitivity immunoassay procedures, surface plasmon resonance, rapid immunoassay chemistries, signal

272 SAEs, assayed by means of ELISA and surface plasmon resonance, were recloned as IgE and antigen-bind

273 Using a surface plasmon resonance-based screening complemented with enzy

274 binant human MGL was confirmed using surface plasmon resonance.

275 ody ligand ZPD-L1_1 was evaluated by surface plasmon resonance.

276 unctional isoforms was assessed with surface plasmon resonance.

277 We confirmed interactions using surface plasmon resonance.

278 t of less than 35 pM, as measured by surface plasmon resonance.

279 ell in vitro stimulation assays, and surface plasmon resonance.

280 e of gold nanoparticles ( 100nm), localized plasmon resonances (LPR) can be coupled by a diffraction

281 Localized surface plasmon resonances (LSPRs) offer the possibility of ligh

282 e solar cells that exploit localized surface plasmon resonances in ultrathin subwavelength plasmonic

283 strates based on metal-insulator-metal (MIM) plasmon resonances with ultra-sharp optical transmission

284 and polarization-dependent infrared surface plasmon resonances.

285 stinct sizes, and therefore showing distinct plasmon resonant peaks (RP), have been biofunctionalized

286 vacancies accompanied by a localized surface plasmon response.

287 be further enhanced by changing the ratio of plasmon-site couplings.

288 lectrically switchable graphene mid-infrared plasmon sources.

289 Surface plasmon (SP) excitations in metals facilitate confinemen

290 particles can be stably trapped in a surface plasmon (SP) standing wave generated by the constructive

291 Here, we show how plasmon strong coupling can be achieved in compact, robu

292 radiative cooling regime between neighboring plasmon-supporting graphene nanostructures in which nonc

293 A method based on plasmon surface resonance absorption and heating was dev

294 Finally, the use of plasmon-tailored excitation fields to achieve subdiffrac

295 c device, the adiabatic nanofocusing surface-plasmon taper.

296 Graphene carries long-lived plasmons that are extremely confined and controllable by

297 For the phonons and plasmons, their OAM are carried by the electrons and ion

298 Decay of plasmons to hot carriers has recently attracted consider

299 We propose that in the absence of plasmon waves in biological samples, these evanescent fi

300 rmally-incident THz wave to standing surface plasmon waves on both thin and thick InSb layers.