ライフサイエンスコーパス: plasmon

1 rotational-vibrational modes using graphene plasmon.

2 in order to blue-shift the back-side surface plasmon.

3 system eventually generates the high-energy plasmon.

4 ntrols the amplitude or phase of propagating plasmons.

5 which then couple to ultraconfined acoustic plasmons.

6 ometals and discovery of behavior of nascent plasmons.

7 e nanoparticles suggests a new type of these plasmons.

8 tudies of how the environment affects mid-IR plasmons.

9 atter quasiparticles, such as excitons(6) or plasmons(7), on an attosecond timescale.

10 Chemical reactions induced by plasmons achieve effective solar-to-chemical energy conv

11 ricated submicrometre pillars covered with a plasmon-active nanometric gold layer, integrated in an o

12 We show that graphene acoustic plasmons allow ultrasensitive measurements of absorption

13 oupling between porous graphene (PG) surface plasmons and anisotropic black phosphorus (BP) localized

14 aves are excited at interfaces, like surface plasmons and have the potential to deliver electrical po

15 by the strong field confinement of graphene plasmons and high physisorption of gas molecules on the

16 ted power in the characterization of surface plasmons and other electronic excitations, as it uniquel

17 e formalism gives a complete account of both plasmons and plasmon-emitter interactions at the nanosca

18 oth surface plasmon polaritons and localized plasmons and summarize the exciting progress it has open

19 ow that the coherence length of the graphene plasmons and the thermally emitted photons can be as lar

20 design methodology, the swore-shaped surface plasmon antenna has both edges corrugated with an array

21 s to interband screening; so, dispersionless plasmons are a universal intrinsic phenomenon in quasi-2

22 Acoustic graphene plasmons are highly confined electromagnetic modes carry

23 tipolar spontaneous emission enhancement, to plasmon-assisted energy transfer and enhancement of two-

24 Plasmon-assisted photocatalytic efficiencies can improve

25 mproved plasmonic sensing, spectroscopy, and plasmon-based optical devices.

26 the possible excitation of localized surface plasmons because of the presence of nanogroove.

27 of -R capped Au(333)(SR)(79) all exhibit two plasmon-bleaching signals independent of the -R group as

28 f elementary excitations such as phonons and plasmons can be tuned in layered vdW systems via stackin

29 ed single, nanometer-scale acoustic graphene plasmon cavities, reaching mode volume confinement facto

30 The strong energy coupling between plasmon cavity modes and excited photosynthetic fluoresc

31 3 cm that generate coupled localised surface plasmons (cLSPs) and is covalently modified with an apta

32 fluidic devices were adapted for (i) surface plasmon coupled enhancement (SPCE) of fluorescence for d

33 ons are so closely apposed that they exhibit plasmon coupling and induce an unexpected contraction of

34 or nano-heterostructures with strong exciton-plasmon coupling have been proposed for applications in

35 f the in-plane azimuthal angle for photon-to-plasmon coupling, which manifests as directly observable

36 s in plasmonic nanostructures, generated via plasmon decay, play key roles in applications such as ph

37 Plasmons depend strongly on dimensionality: while plasmo

38 an serve as a telltale signature of undamped plasmons directly accessible in near-field imaging exper

39 about the underlying mechanistic details of plasmon-driven charge transfer.

40 The plasmon-driven chemistry of ferri-/ferrocyanide ions ins

41 he current mechanistic background for future plasmon-driven chemistry studies and applications.

42 But for such plasmon-driven chemistry to be precisely understood and

43 monic noble metal nanostructures for various plasmon-driven energy conversions and design of photochr

44 Interrogating the plasmon-driven processes over a wide range of temperatur

45 el understanding of the mechanism behind the plasmon-driven synthesis of Au nanostars and illustrate

46 ign this as a signature for lasing involving plasmon emission.

47 Plasmon-emitter interactions are of central importance i

48 ives a complete account of both plasmons and plasmon-emitter interactions at the nanoscale, constitut

49 We consider a broad array of plasmon-emitter interactions ranging from dipolar and mu

50 n the amplitude and spectral distribution of plasmon-emitter interactions.

51 platform to include nonclassical effects in plasmon-enabled nanophotonic phenomena.

52 ides a route to substantially increasing the plasmon enhanced optical transmission through metal grat

53 performance of a recently developed surface plasmon-enhanced optical sensor that utilizes two-photon

54 dium to support a highly-penetrating surface plasmon evanescent field that extends well into the diel

55 posites that allow the dynamic tuning of the plasmon excitation by controlling their orientation usin

56 nostructures and their dynamic modulation of plasmon excitation further allow them to be conveniently

57 Here, we demonstrate that the plasmon excitation of nickel induces the transfer of bot

58 he light-intensity-dependent activity in the plasmon-excitation-driven reduction of CO(2) on Au nanop

59 directional frequency range near the surface plasmon frequency, where the surface plasmon polariton p

60 Localized surface plasmons generated on metallic nanostructures provide an

61 photochemical process, the exact function of plasmon-generated hot holes in regulating the morphology

62 reaking in Bi(2)Te(3) TI thin films: surface plasmon generation, charge transfer, and application of

63 Our model is developed by combining plasmon hybridization theory with transformation optics,

64 Here we show that the plasmons in real quasi-2D metals are qualitatively diffe

65 However, besides graphene, plasmons in real, atomically thin quasi-2D materials wer

66 Plasmons in such ultranarrow gaps can exhibit nonlocal r

67 on theorem with nonlocal response of surface plasmons in the random phase approximation, we show that

68 s of conductivity as well as two independent plasmons in the same nanoparticle with very different el

69 ons depend strongly on dimensionality: while plasmons in three-dimensional systems start with finite

70 tart with finite energy at wavevector q = 0, plasmons in traditional two-dimensional (2D) electron ga

71 hout spin flip is required to keep these two plasmons independent.

72 n mechanistic knowledge, we investigated the plasmon-induced dissociation of a single-molecule strong

73 In Ag-CsPbBr(3) nanocrystals, both the plasmon-induced hot electron and the resonant energy tra

74 n this article, we demonstrate an asymmetric plasmon-induced hot-carrier Seebeck photodetection schem

75 and a small footprint (~1 mum in length) via plasmon-induced transparency (PIT) configuration.

76 STO) is investigated, and also a high-energy plasmon is observed.

77 In addition, coupled-plasmon-like and inter-band transition-like modes occur

78 The localized surface plasmons (LSPs) on the NPG sheet, partially hybridized w

79 osites could amplify the signal generated by plasmon material and increase the sensitivity of molecul

80 external gate voltage, we find that graphene plasmons mediate the optical nonlinearity and modify the

81 Plasmon-mediated carrier transfer (PMCT) at metal-semico

82 xtracting 16 per cent of the energy from the plasmon mode as light.

83 spatial resolution along one axis due to the plasmon mode attenuation distance (tens of mum, typicall

84 t-coupling scheme to extract energy from the plasmon mode.

85 demonstrate coupling the front and back-side plasmon modes by using a lower refractive index substrat

86 ential excitation of bonding and antibonding plasmon modes for a system composed of two coupled dipol

87 Coupling between the two plasmon modes is then demonstrated by introducing aqueou

88 ng the near field of the full set of nanorod plasmon modes of either parity.

89 nteraction of sonoluminescence light with UV plasmon modes of the metal.

90 Sharp chiral wrinkles lead to chiral plasmon modes with high dissymmetry factors (~0.20).

91 emonstrate a three-dimensionally-tapered gap plasmon nanocavity that overcomes this fundamental limit

92 is reported for the synthesis of rod-shaped plasmon nanostructures which are vertically self-aligned

93 netic core (MP@silica@Au); 2) use of surface plasmons of Au nanoshells with a magnetic core for spont

94 Research on plasmons of gold nanoparticles has gained broad interest

95 e we develop a theoretical model for surface plasmons of interacting nanoparticles to reduce the comp

96 over, our ab initio calculations reveal that plasmons of monolayer metallic transition metal dichalco

97 modes to identify the role of the generated plasmons on the electrochemical response.

98 and with a sharp Fermi edge accompanied by a plasmon peak, characteristic of delocalized metallic ele

99 etal/dielectric." Interestingly, the surface plasmon polariton (SPP) at a metal/dielectric interface

100 th dual high-Q Rayleigh anomaly (RA)-surface plasmon polariton (SPP) resonances for multiparameter se

101 t broadband frequency scanning spoof surface plasmon polariton (SSPP) based design for efficient endf

102 surface plasmon frequency, where the surface plasmon polariton propagates along one but not the oppos

103 e of an external magnetic field, the surface plasmon polariton that exists at the metal-dielectric in

104 As surface-plasmon-polariton (SPP) waves are localized, signal dela

105 Our calculation reveals that the surface plasmon-polariton at metal-dielectric interfaces remains

106 ~10 mum) were shown to be sufficient for the plasmon-polariton generation and strong laser field conf

107 e the strong interaction between the surface plasmon polaritons (SPPs) and excitons in the WSe(2) to

108 en an ultrathin gold film supporting surface plasmon polaritons and a scanning probe tip, that can pr

109 as a characterization tool for both surface plasmon polaritons and localized plasmons and summarize

110 This is due to the conversion of surface plasmon polaritons into a freely propagating field and t

111 shows that the propagation length of surface plasmon polaritons supported at the sodium-quartz interf

112 luctuations in the electric field of surface plasmon polaritons undergoing random scattering on a rou

113 ided crossing of exciton, cavity photons and plasmon polaritons with effective separation energy exce

114 two-dimensional photonic crystal for surface plasmon polaritons.

115 benefits this provides for coupling surface plasmon-polaritons (SPPs) to photon emission in 2D semic

116 d through the generation of highly localized plasmon-polaritons on the surface of mitochondrial crist

117 and self-assembly ability, combined with the plasmon properties, stability, stimuli-response, and del

118 and self-assembly ability, combined with the plasmon property, stability, stimuli-response, and deliv

119 Fiber optic-surface plasmon resonance (FO-SPR) can overcome these limitation

120 is study, a solid-phase, fiber optic surface plasmon resonance (FO-SPR) technique is presented as an

121 ly sensitive and low cost Long Range Surface Plasmon Resonance (LRSPR) biosensor for detecting uric a

122 stance- and size-dependent localized surface plasmon resonance (LSPR) between fluorescent quantum dot

123 iosensor that exploits the localized surface plasmon resonance (LSPR) effect of silver nanostructures

124 n, we demonstrate that the localized surface plasmon resonance (LSPR) excitation of Au nanorods (NRs)

125 lasmon resonance (SPR) and localized surface plasmon resonance (LSPR) have shown promises.

126 which means it can sustain localized surface plasmon resonance (LSPR) in its nanocrystalline form.

127 Localized surface plasmon resonance (LSPR) is shown to be effective in tra

128 ield that results from the localized surface plasmon resonance (LSPR) is strengthening the HCO(3)(-)

129 ld of optically stimulated localized surface plasmon resonance (LSPR) modes in nanorod antennas.

130 t assays (ELISA) using the localized surface plasmon resonance (LSPR) of metal nanoparticles has emer

131 method exploits the fact that the localized plasmon resonance (LSPR) of the plasmonic nanoparticles

132 man scattering by exciting localized surface plasmon resonance (LSPR) on metal substrates.

133 ld nanorods (GNR) with the localized Surface Plasmon Resonance (LSPR) peak in the visible range for b

134 rs that utilize the unique localized surface plasmon resonance (LSPR) properties of chemically synthe

135 ubstantially affects their localized surface plasmon resonance (LSPR) properties that together allow

136 es (AuNPLs) exhibit strong localized surface plasmon resonance (LSPR) scattering and display as red s

137 ghlight case studies where localized surface plasmon resonance (LSPR) scattering is used for tracking

138 een a challenging task for localized surface plasmon resonance (LSPR) spectroscopy, presenting only a

139 based on the principle of localized surface plasmon resonance (LSPR) to detect the DNA-polymerase re

140 and verified findings with localized surface plasmon resonance (LSPR).

141 fect of Au colloids (i.e., localized surface plasmon resonance (LSPRs)) in conjunction with the versa

142 Surface plasmon resonance (SPR) analysis confirmed that rHDL/Do

143 nuclear magnetic resonance (NMR) and surface plasmon resonance (SPR) analysis.

144 By combining surface plasmon resonance (SPR) and electrolyte gated field-effe

145 action kinetics have been studied by surface plasmon resonance (SPR) and fluorescence spectroscopy.

146 Conventional techniques such as surface plasmon resonance (SPR) and isothermal titration calorim

147 Techniques based on propagating surface plasmon resonance (SPR) and localized surface plasmon re

148 ctable shifts (Deltatheta(r)) in the surface plasmon resonance (SPR) angle.

149 this essential polymer is sensed, a surface plasmon resonance (SPR) assay using varied PG surface pr

150 The first assay is surface plasmon resonance (SPR) based and can quantitate both an

151 Surface plasmon resonance (SPR) based dopamine sensor is realize

152 The Surface Plasmon resonance (SPR) based label-free detection of sm

153 Surface plasmon resonance (SPR) based sensing is an attractive a

154 Surface plasmon resonance (SPR) based sensors allow the evaluati

155 r 0.075-3500 ppm, LFIAs with C only, surface plasmon resonance (SPR) binding experiments on the immob

156 on of misfolded proteins employing a surface plasmon resonance (SPR) biosensor and heat shock protein

157 , by coupling the MIP biosensor with surface plasmon resonance (SPR) detection.

158 Herein, a surface plasmon resonance (SPR) enhanced DNA biosensor has been

159 tive inhibition assay (SIA) based on surface plasmon resonance (SPR) for the rapid detection of Campy

160 nted optical-based biosensors namely Surface Plasmon Resonance (SPR) has been extensively investigate

161 neous microRNA (miRNA) detections by surface plasmon resonance (SPR) imaging measurements on SPR chip

162 ow-cost metallic nanostructure-based surface plasmon resonance (SPR) imaging platform, comprising mul

163 anosheets functionalized fiber optic surface plasmon resonance (SPR) immunosensor has been reported f

164 amount of cellular uptake of EVs by surface plasmon resonance (SPR) in real-time.

165 Surface plasmon resonance (SPR) measurements confirmed that muta

166 hed heme specificity and affinity by surface plasmon resonance (SPR) of the four Cluster C proteins i

167 Surface plasmon resonance (SPR) offers exceptional advantages su

168 geometrical features, the effects of surface plasmon resonance (SPR) on sensing as well as current st

169 Characterization of NP627 by surface plasmon resonance (SPR) revealed that PKCdeltaI and NP62

170 e show that this is possible using a surface plasmon resonance (SPR) scattering technique.

171 Surface plasmon resonance (SPR) sensor as an example of portable

172 paratope region, was fabricated on a surface plasmon resonance (SPR) sensor chip to enhance the sensi

173 Fiber optic surface plasmon resonance (SPR) sensor utilizing silver (Ag) and

174 Using surface plasmon resonance (SPR) spectroscopy, we demonstrated th

175 omplex in a form that accumulates on surface plasmon resonance (SPR) surfaces coated with properdin,

176 study, a continuous angular-scanning surface plasmon resonance (SPR) technique is utilized for measur

177 successfully demonstrated the use of surface plasmon resonance (SPR) technology for the first time to

178 The surface plasmon resonance (SPR), an optical biosensor, possessin

179 Here, using surface plasmon resonance (SPR), antigen presentation assays, an

180 with dissipation monitoring (QCM-D), surface plasmon resonance (SPR), atomic force microscopy (AFM),

181 ct transistor (FET)-based biosensor, surface plasmon resonance (SPR)-based biosensor and artificial i

182 ugh it has been widely accepted that surface plasmon resonance (SPR)-generated energetic electrons pl

183 for EP9 which was further studied by surface plasmon resonance (SPR).

184 LF with naringin (NR) was studied by surface plasmon resonance (SPR).

185 cal impedance spectroscopy (EIS) and surface plasmon resonance (SPR).

186 (CRD) of the Wnt receptor FZD8 using surface plasmon resonance (SPR).

187 analog (RESAn1) were investigated by surface plasmon resonance (SPR).

188 urier-transform Infrared (FT-IR) and surface plasmon resonance (SPR).

189 to gold nanorods, and the localized surface plasmon resonance absorbance through the sample was meas

190 Surface plasmon resonance analyses revealed significant binding

191 Using surface plasmon resonance analysis of bi-TPB-PPB antibodies bind

192 Surface plasmon resonance analysis revealed that wtsFae1B's K(d)

193 s and synthetic peptides, along with surface plasmon resonance analysis to measure the kinetics of th

194 re, using immunoblotting, ELISA, and surface plasmon resonance analysis, we report that the iron-regu

195 Using surface plasmon resonance and a panel of anti-gD monoclonal anti

196 ibody avidity was investigated using surface plasmon resonance and B cell ELISPOTs were used to measu

197 using biosensors techniques based on surface plasmon resonance and bio-layer interferometry.

198 We validated a subset using surface plasmon resonance and cell binding assays.

199 parin and extracellular matrix while surface plasmon resonance and cell-based assays confirmed that A

200 Surface plasmon resonance and co-immunoprecipitation independent

201 Surface plasmon resonance and crystallography techniques demonst

202 Surface plasmon resonance and differential scanning fluorimetry

203 ray of biochemical assays, including surface plasmon resonance and ELISA, discovered that fibronectin

204 l fluid-phase C3(H(2)O), measured by surface plasmon resonance and flow cytometry.

205 reviewed, and their integration into surface plasmon resonance and fluorescent sandwich immunoassay f

206 , evanescent wave, refractive index, surface plasmon resonance and holography based sensor designs, a

207 robust biosensor based on localized surface plasmon resonance and hybridization chain reaction.

208 As indicated by the surface plasmon resonance and isothermal titration calorimetry d

209 ; immunoprecipitation, pulldown, and surface plasmon resonance assays; and immunofluorescence, small-

210 a single-domain crystal structure support a plasmon resonance at approximately 280 nm with better qu

211 Moreover, surface plasmon resonance binding affinity assay showed that PB

212 rminal binding domain, BG(ZP-C), and surface plasmon resonance binding measurements with TGF-beta2 va

213 n orthogonal WIP1 activity assay and surface plasmon resonance binding studies.

214 centration, we developed a localized surface plasmon resonance biosensor based on succinimidyl-ester-

215 scence and colorimetric sensors, and surface plasmon resonance biosensors.

216 ere, we combine protein engineering, surface plasmon resonance characterization, and molecular dynami

217 at combines multiple features of the surface plasmon resonance curve and allows for a more precise an

218 cin-galectin-3 interaction, shown by surface plasmon resonance data indicating that recombinant lubri

219 Mutagenesis coupled with surface plasmon resonance demonstrate the gC1qR Zn2+ site contri

220 e experimentally observed an angular surface plasmon resonance dip at 74 degrees with the ultralow-in

221 b visible light due to the localized surface plasmon resonance effect of gold, can decarboxylate a wi

222 Surface plasmon resonance experiments established Vgamma9Vdelta2

223 Results from surface plasmon resonance experiments revealed that hyen D, E, L

224 Using solid-phase binding assays and surface plasmon resonance experiments with purified proteins, we

225 dicted by the model and validated by surface plasmon resonance experiments, multivalent interactions

226 ent control over their size, morphology, and plasmon resonance frequency.

227 ostructures, we are able to vary the surface plasmon resonance from 551 to 693 nm.

228 Surface plasmon resonance imaging (SPRI) is a powerful label-fre

229 Like the surface plasmon resonance imaging (SPRi) technique, the presente

230 the detection of VOCs in solution by surface plasmon resonance imaging (SPRi).

231 Surface plasmon resonance indicates that the ability to stabiliz

232 those derived from multi-parametric surface plasmon resonance measurements and molecular dynamics si

233 Results of surface plasmon resonance measurements supported a bivalent bind

234 Surface plasmon resonance microscopy (SPRM) is a versatile platf

235 ed by theoretically fitting the longitudinal plasmon resonance of GNRs obtained by UV-visible spectro

236 he Au NP excited by the laser at the surface plasmon resonance peak can generate a nanoscale bubble,

237 The shift in the plasmon resonance peak reflects the amount of secreted p

238 including size, shape, capping, and surface plasmon resonance profile, dose range, and exposure time

239 variant in SP6 (p.(Ala273Lys)) using surface plasmon resonance protein-DNA binding studies.

240 ticles, much more reliably than any observed plasmon resonance shifts.

241 Surface plasmon resonance shows that serotonin adsorbs with mill

242 nd isothermal titration calorimetry, surface plasmon resonance spectroscopy, and molecular modeling,

243 Surface plasmon resonance studies revealed that while this moiet

244 A further surface plasmon resonance study showed that this modification di

245 nsing performance of a prism-coupled surface plasmon resonance system by Gaussian beam shaping and mu

246 confirmed as a drug target by using surface plasmon resonance technology and through interaction wit

247 be observed because of the localized surface plasmon resonance that causes impedance matching.

248 n industry standard sensors based on surface plasmon resonance that require spectral or angular inter

249 In this study, we used surface plasmon resonance to evaluate the affinity between LRP-1

250 We quantify this interaction with surface plasmon resonance to measure equilibrium dissociation co

251 Contrary to this model, using surface plasmon resonance to monitor real-time binding of recomb

252 Here, we used surface plasmon resonance to show that the ectodomain of gH/gL b

253 d the comparatively high-sensitivity surface plasmon resonance wavelength, lambda, while the change i

254 o (genetics and ChIP-seq), in vitro (surface plasmon resonance) and phylogenetic analyses identified

255 fector functions, as demonstrated by surface plasmon resonance, Ab-dependent cellular phagocytosis, a

256 n enzyme-linked immunosorbent assay, surface plasmon resonance, and competitive human serum bacterici

257 Using site-directed mutagenesis, surface plasmon resonance, and crystallography, Philips et al. e

258 for its cognate pMHC, as measured by surface plasmon resonance, and specifically stained cells presen

259 ifferential scanning calorimetry and surface plasmon resonance, but these biophysical methods suffer

260 rrogated their FcgammaRI binding via surface plasmon resonance, enzyme-linked immunosorbent assay, an

261 e sensors such as those based on the surface plasmon resonance, optical waveguides, etc.

262 ate binding affinity, as measured by surface plasmon resonance, paralleled substrate phosphorylation.

263 try, luminescence, refractive index, surface plasmon resonance, photonic crystals, turbidity, mechani

264 with computational image processing, surface plasmon resonance, Raman spectra, and laser tweezer as w

265 resonance, lipid-binding assays, and surface plasmon resonance, this work identifies the critical Dab

266 Here, using surface plasmon resonance, tryptophan fluorescence, and analysis

267 hermal shift assay and validation by surface plasmon resonance, we found eight hits toward the tandem

268 Using comparative genomics and surface plasmon resonance, we identified parasite-derived peptid

269 s and several biochemical assays and surface plasmon resonance, we report that our nanobody, hC3Nb2,

270 nostars demonstrated a pronounced multipolar plasmon resonance, which has not been observed in previo

271 Using recombinant proteins and surface plasmon resonance-based binding assays, we show that the

272 fragment phage display libraries and surface plasmon resonance.

273 ectrons, therefore supporting a high quality plasmon resonance.

274 trons and consequently in low quality of the plasmon resonance.

275 have a K(D) of 3.3 x 10(-6) M using surface plasmon resonance.

276 ring in length and flexibility using surface plasmon resonance.

277 A(121) with VEGFR1 and VEGF-R2 using surface plasmon resonance.

278 Localized surface plasmon resonances (LSPR) of nanostructures can be tuned

279 ibutes, especially tunable localized surface plasmon resonances (LSPRs) and super-ionic behavior.

280 Localized surface plasmon resonances (LSPRs) have attracted much recent at

281 n exhibit tunable infrared localized surface plasmon resonances (LSPRs).

282 The consequent change in localized surface plasmon resonances alters the visible absorbance of drie

283 paper reports how the spectral linewidths of plasmon resonances can be narrowed down to a few nanomet

284 -equilibrium excitation of localized surface plasmon resonances coupled to nonlinear oscillators and

285 cement through the excitation of the surface plasmon resonances in bow-tie nanoantennas forming the a

286 esults contribute to the understanding of UV plasmon resonances in colloidal liquid-metal EGaIn nanop

287 has been used to image the mode structure of plasmon resonances in metal nanostructures, and is made

288 By the photoexcitation of localized surface plasmon resonances of metal nanoparticles, one can gener

289 Surface plasmon resonances of metallic nanostructures offer grea

290 nanoparticles which excite localized surface plasmon resonances that are primarily responsible for th

291 phate, or carboxyfluorescein are tethered to plasmon-resonant hollow gold nanoshells (HGN) tuned to a

292 By matching the surface plasmon-resonant wavelength of the nanoparticle tag to t

293 Our acoustic plasmon resonator platform is scalable and can harness t

294 the -R group as well as solvent, indicating plasmon splitting and quantum effect in the ultrasmall c

295 he resonance condition of the nearby surface plasmon, this high refractive index coating creates an e

296 This opens the possibility of tracking plasmon wave packets in real time for novel imaging tech

297 opic black phosphorus (BP) localized surface plasmons, which made the electrochemical performance of

298 space light coupled to conventional graphene plasmons, which then couple to ultraconfined acoustic pl

299 al media supports the propagation of surface plasmons with drastically enhanced intensity over multip

300 the originally prepared excitons and surface plasmons, with the rate constant of about 5.7 x 10(7) s(