ライフサイエンスコーパス: waveguide

1 oss of the THz wave propagating through this waveguide.

2 nsverse-magnetic modes of the parallel-plate waveguide.

3 ndex single crystal (GRISC) optically active waveguide.

4 lignment of 2D flakes within the optofluidic waveguide.

5 as 0.91 +/- 0.01 observed in a 1,100-nm-wide waveguide.

6 pumped current source enclosed by a tapered waveguide.

7 egions and the light transmitted through the waveguide.

8 ted energy densities within the nanoscale LD waveguide.

9 tunable frequency and bandwidth in a diamond waveguide.

10 istribution matching the mode of the coaxial waveguide.

11 ingle microwave photon propagating through a waveguide.

12 of adsorption of the organic molecules on a waveguide.

13 on of light through a channel silicate glass waveguide.

14 se of the light exiting at the output of the waveguide.

15 case of ballistic propagation of light in a waveguide.

16 n to be that of photon tunneling to a nearby waveguide.

17 n of the channel along the length of the MMI waveguide.

18 arated atomic dipoles mediated by an optical waveguide.

19 of 0.90 +/- 0.01 from another (800-nm-wide) waveguide.

20 within an effective mid-latitude atmospheric waveguide.

21 device that integrates a TI with a photonic waveguide.

22 n and (3) to full reflection into the second waveguide.

23 directed formation of broadband, cylindrical waveguides.

24 ling spin waves in the input junction of the waveguides.

25 or cold atoms propagating in crossed optical waveguides.

26 -assembled nanoparticles behave as plasmonic waveguides.

27 the diverse optical properties of dielectric waveguides.

28 essive performances compared to conventional waveguides.

29 pling and thermal isolation between ILDs and waveguides.

30 the non-chiral geometry and material of the waveguides.

31 id-state quantum emitter-with low-loss Si3N4 waveguides.

32 ma using straight long-range surface plasmon waveguides.

33 nons are combined with photonic and phononic waveguides.

34 dic array of silicon strips between adjacent waveguides.

35 plates that form an array of parallel-plate waveguides.

36 ly weak in conventional nanophotonic silicon waveguides.

37 ivalent to a stacked array of parallel-plate waveguides.

38 ments as well, such as vertical silicon slot waveguides.

39 n polariton with dielectric-loaded plasmonic waveguiding.

40 e polarization-entangled states in an AlGaAs waveguide, aided by the PMD and without any compensation

41 n the electric field distribution around the waveguide, allowing accurate, frequency-dependent liquid

42 ential of GaNAs alloys for III-nitride based waveguide and photonic circuit design applications.

43 methods along with electrochemical, optical waveguide and polymer based sensors.

44 Interaction between photons in the waveguide and surface electrons in a Bi2Se3 layer genera

45 ntation, allowing direct integration of GaAs waveguides and cavities containing self-assembled InAs/G

46 otonic crystals, enabling components such as waveguides and cavities.

47 goal by hybrid on-chip integration of Si3N4 waveguides and GaAs nanophotonic geometries with InAs qu

48 livery system, consisting of silicon nitride waveguides and grating couplers for out-of-plane light e

49 ght-emitting materials with planar plasmonic waveguides and offers great potential for developing int

50 ly efficient optical interface between Si3N4 waveguides and single-quantum dots in GaAs geometries, w

51 es when compared with conventional plasmonic waveguides and, at the same time, retain the light local

52 and their realization to offer miniaturized waveguides, antennas and shielding patterns are on anvil

53 backscattering suppression around the curved waveguide are further demonstrated.

54 Thanks to these properties, our nonlinear waveguides are able to produce a pi nonlinear phase shif

55 g one-dimensional arrays of randomly coupled waveguides arranged on linear and ring topologies, we ar

56 on spatial diversity uses a length-variable waveguide array to create the optical time delays, which

57 xploits spatial diversity in an equal length waveguide array.

58 ate, implemented in integrated laser-written waveguide arrays.

59 ility of the antiresonant reflecting optical waveguide (ARROW) biosensor chip, a detection limit of 0

60 ctromagnetic fields produced by a microstrip waveguide as a function of its gigahertz operating frequ

61 The nanostructures act both as a waveguide as well as a physical surface modification of

62 eguide modes, and enables design of acoustic waveguides as well as seamless integration with electrom

63 ices to sound waves in acoustic-metamaterial waveguides, as well as fermions and phonon polaritons in

64 just the acoustic impedance of the composite waveguide at an impedance-mismatched fluidic interface,

65 ined spoof surface plasmon polaritons (SPPs) waveguides at subwavelength scale enabled by planar stag

66 rence in a silicon-organic hybrid (SOH) slot waveguide based Mach-Zehnder interferometer.

67 o enhance performance of a wide range of SWG waveguide based photonics devices.

68 ising mid - infrared platform for integrated waveguide - based chemical sensing and photodetection.

69 Because these waveguide-based artificial dielectrics are low loss, ine

70 implementation and scalability, the proposed waveguide-based extraction method does not require a vac

71 Herein, we report an integrated channel waveguide-based fluorescent immunosensor with the abilit

72 A waveguide-based scheme relying on photon tunneling is pr

73 ays for future miniaturization of dielectric waveguide-based systems with simultaneous polarization a

74 g, the average insertion loss of a 5 mum SWG waveguide bend is reduced drastically from 5.43 dB to 1.

75 However, the high loss of SWG waveguide bends jeopardizes their applications in integr

76 re-distorted refractive index profile in SWG waveguide bends.

77 demonstrate a set of building blocks such as waveguides, bends, and couplers which can be used to rou

78 valleytronic operations, such as valves and waveguides, but it is technically challenging to realize

79 s to the light-intensity distribution of the waveguide calculated by finite-difference time-domain si

80 toexcited electron-hole pairs in the silicon waveguide can be injected into phosphorene to induce its

81 The acoustic impedance of the composite waveguide can be regulated by merely controlling its cou

82 We find that the micro-discs of the waveguides can be excited by terahertz frequency fields

83 ted by picosecond pulses in microcavity wire waveguides can be understood as the Cherenkov radiation

84 ulations, which reveal that photonic-crystal waveguides can exhibit surprisingly small localized mode

85 LS) coupled with a 250 cm path length liquid waveguide capillary cell (LWCC) and miniature fiber opti

86 520 nm, exploiting a long path-length liquid waveguide capillary cell (LWCC) of 100 cm path length.

87 le-into-liquid sampler coupled with a liquid waveguide capillary cell and total organic carbon analyz

88 Analogously, photons in optical waveguides carry transverse spin angular momentum which

89 nce (MMI) waveguide crosses multiple fluidic waveguide channels on an optofluidic chip to create mult

90 The waveguide chip was activated by (3-Mercaptopropyl) trime

91 e linear, branched and cross-shaped nanoslot waveguide components, which all support resonances due t

92 Furthermore, we show that the waveguide concept can be extended to other metal/dielect

93 tially resolved near field measurements in a waveguide configuration were performed, allowing us to m

94 In the limit of strong waveguide confinement and depending on the velocity of t

95 The structure of these new waveguides consists of an ultrathin metallic strip with

96 ropagation loss than its conventional hybrid waveguiding counterpart, while maintaining strong optica

97 cting photon pairs directly on the chip with waveguide-coupled single-photon detectors.

98 ving the full many-body quantum state of the waveguide-coupled system, illustrating that large photon

99 Parity-time-symmetric (-symmetric) optical waveguide couplers offer new possibilities for fast, ult

100 of the promise that many components, such as waveguides, couplers, interferometers and modulators, co

101 waveguides, with relative energies and inter-waveguide couplings tailored to yield the desired Hamilt

102 nic device consisting of a planar dielectric waveguide covering a gold nanostripe array fabricated on

103 ing element was designed based on a coplanar waveguide (CPW) loaded with a split ring resonator (SRR)

104 Furthermore, broadband coplanar waveguide (CPW) to planar staggered plasmonic waveguide

105 A solid-core multimode interference (MMI) waveguide crosses multiple fluidic waveguide channels on

106 nd quantum sensor with optical and microwave waveguide delivery enables thermometry with single-cell

107 strate lithographically defined nanophotonic waveguide devices for light routing and ion addressing t

108 e mode converters, polarization rotators and waveguide devices supporting asymmetric optical power tr

109 However, spin wave reflection at the waveguide edge has previously limited the stability of i

110 sly acts as a fluidic microvalve and optical waveguide, enabling mechanically reconfigurable light an

111 ficiency of voltage-induced DNA loading into waveguides equipped with nanopores at their floors is fi

112 s produce nonreciprocal mode conversion, the waveguide equivalent of Faraday Rotation (FR).

113 Our monolithic Si-on-BTO waveguides establish a new sensor platform that enables

114 The TEM quasi-single mode THz waveguide excitation and non-dispersive propagation of a

115 Coaxial waveguides exhibit no dispersion and therefore can serve

116 t position than in standard photonic crystal waveguides, exhibit spin-path readout up to 95+/-5% and

117 The GO-coated waveguide exhibits very strong photo-absorption of TE-po

118 rated experimentally with a photonic-crystal waveguide fabricated without any intentional disorder, f

119 The waveguide features lower propagation loss than its conve

120 The feasibility of the waveguide for compact THz components is also studied to

121 d in distinct spatial modes of an integrated waveguide for the first time.

122 ssitates the use of dispersive structures or waveguides for extending the field-particle interaction.

123 reorientational solitons can act as passive waveguides for other weak optical signals, these results

124 class of semiconductor-based slot plasmonic waveguides for subwavelength THz transport.

125 A combination of these waveguides forms a liquid-core multimode interference wa

126 inearity in lithographically easy-to-produce waveguide geometries (such as with a flat, concave exter

127 Several different waveguiding geometries are considered for reducing the e

128 guide have been easily manipulated using the waveguide geometry to densely encode information.

129 Under the optimized waveguide geometry, this is the first demonstration of u

130 This behaviour in a GO-coated waveguide gives the action of an inverted optical switch

131 esonance intensity measurements in resonance waveguide grating (RWG) sensors, we propose to apply res

132 e present the design and characterization of waveguide grating devices that couple visible-wavelength

133 The structured waveguide has a variable thickness in the vicinity of an

134 ight by a graphene-oxide (GO) coated polymer waveguide has been observed in the presence of transvers

135 emerging development of the hybrid plasmonic waveguide has recently received significant attention ow

136 the transverse spatial modes of a multi-mode waveguide have been easily manipulated using the wavegui

137 Devices based on SWG waveguides have demonstrated impressive performances com

138 GeSbS ridge waveguides have recently been demonstrated as a promisin

139 ere are two distinct features related to the waveguide: i) It is not absorptive, on the contrary, wea

140 first demonstration of using such a type of waveguide immunosensor for the detection of microcystin-

141 The device consists of a straight waveguide in which two modes of the same polarization in

142 Applications for smooth electron waveguides in 2D Dirac-Weyl systems are discussed.

143 tters in photonic structures such as optical waveguides in a scalable way, where precise and accurate

144 The approach uses subwavelength grating waveguides in silicon-on-insulator (SOI), which enables

145 esonator is consisted of uniform single-mode waveguides in the semi-circle region, to eliminate bendi

146 ced mode coupling, and adiabatically tapered waveguides in the straight region, to avoid excitation o

147 ating electromagnetic fields produced by the waveguide, in a specimen-free experiment, exert Lorentz

148 ous electromagnetic properties of dielectric waveguides, including mode confinement, polarization, sc

149 propose a novel scheme to realize an optical waveguide induced by an active Raman gain (ARG) process

150 ng is presented as an alternate approach, as waveguides inherently provide a large density of channel

151 ble and bioresorbable, such as embedding the waveguide inside living tissue.

152 Here, we demonstrate a silicon waveguide-integrated light source and photodetector base

153 The gap waveguide intensifies light by nanofocusing it to a mode

154 ontinuously deflect the atomic flux from one waveguide into the other.

155 a polymer coated internal reflection element/waveguide is an established sensor platform for the dete

156 The proposed structured waveguide is an ideal candidate for the demonstration of

157 mance all-optical quantizer based on silicon waveguide is believed to have significant applications i

158 Importantly, the waveguide is compatible with the current complementary m

159 hybrid dielectric-loaded nanoridge plasmonic waveguide is formed.

160 hniques, the propagation optical loss of the waveguide is measured to be below 3 dB/cm.

161 ed schemes where usually the optical induced waveguide is passive and is severely attenuated by the D

162 ate structured metal-dielectric-metal (SMDM) waveguide is proposed.

163 es over almost the entire range in which the waveguide is single mode, providing a sensitive and broa

164 ing all the optical properties of dielectric waveguides is a challenging task and often requires comp

165 pling between free space components and slab waveguides is a common requirement for integrated optica

166 f 4 to 50 times with respect to the straight waveguides is achieved, depending on the cavity ring rad

167 The propagation loss of these waveguides is low-on the order of 4 dB/cm.

168 eking better surface plasmon polariton (SPP) waveguides is of critical importance to construct the fr

169 re comprising a periodic array of step-index waveguides is reported.

170 e formed by the interference between the two waveguides is used as a quasi-Bragg splitter to continuo

171 nt advancements toward on-chip semiconductor waveguides, it is anticipated that label-free integrated

172 carefully designing the dimension of the SOH waveguide, large nonlinear coefficients up to 16,000 and

173 a microfabricated free-standing liquid core waveguide (LCW) capillary detection tube of long path le

174 etic field chirality that arises in nanobeam waveguides leads to unidirectional photon emission from

175 Optical waveguide lightmode spectroscopy (OWLS) technique has be

176 l-metal metamaterial, consisting of a square waveguide loaded with complementary electric split ring

177 n, and relatively low refractive indices for waveguide matching.

178 bility with photonic integration in standard waveguide materials.

179 ter use, the biodegradable and biocompatible waveguides may be used for long-term light delivery and

180 paper, we demonstrate the use of metal-clad waveguide (MCWG)-based microscopy for label-free real-ti

181 angular momentum coupling into magneto-optic waveguide media engenders spin-helicity-dependent unidir

182 shifts for evanescent waves in magneto-optic waveguide media.

183 ort the demonstration of such reconfigurable waveguide mesh in silicon.

184 re implemented by a two-dimensional photonic waveguide mesh realizes different functionalities throug

185 onstrate a reconfigurable but simple silicon waveguide mesh with different functionalities.

186 ode with a monolithically integrated optical waveguide mixer that can deliver multicolor light at a c

187 n laser diode (ILD) and a dielectric optical waveguide mixer via a gradient-index (GRIN) lens.

188 ign principle, we experimentally demonstrate waveguide mode converters, polarization rotators and wav

189 uctor (CMOS) process and a sharp fundamental waveguide mode has been observed.

190 phase matching caused by the interplay among waveguide mode, neutral atomic dispersion, and plasma ef

191 ing the incident photons into the horizontal waveguide mode, thus significantly increasing the absorp

192 the effective phase velocity of a high-order waveguide mode.

193 veguide (PPWG) T-junction excited by the TE1 waveguide mode.

194 n spectrum is dominated by Fabry-Perot (F-P) waveguide modes and plasmonic modes.

195 the study of both ordinary and extraordinary waveguide modes in real space, we are able to quantitati

196 itously employed in electromagnetics to find waveguide modes, and enables design of acoustic waveguid

197 n PDA microtube, with a one-dimensional (1D) waveguide nature, the excitation position and emission o

198 optical power over short distances, when the waveguide needs to be biocompatible and bioresorbable, s

199 se modulation experiments, we characterize a waveguide nonlinear parameter of 7 W(-1)/m and nonlinear

200 for the elastic wave eigenmodes in acoustic waveguides of arbitrary cross-section is presented.

201 gth reconfigurable ring resonator lasers and waveguides of arbitrary shapes to out-couple and guide l

202 ultraviolet light is demonstrated in silica waveguides on a silicon chip.

203 cuits consisting of amorphous silicon (a-Si) waveguides on an epitaxial barium titanate (BaTiO3, BTO)

204 he optomechanical cavity by phononic crystal waveguides, or optically through the strong photoelastic

205 m one-way photonic edge states to a selected waveguide output with an isolation ratio in excess of 10

206 d near-field mapping of the THz field at the waveguide output.

207 with precise control over the ratio between waveguide outputs.

208 d by more than two orders of magnitude for a waveguide pair with an edge-to-edge distance of lambda/

209 emonstrated comprising a yttrium iron garnet waveguide partially covered by gold.

210 oherent lengths in thin film lithium niobate waveguides patterned with the gradient metasurfaces.

211 itter to the band edge of a photonic crystal waveguide (PCW) provides a unique platform for tuning th

212 for atoms trapped within a photonic crystal waveguide (PCW).

213 leading to unique staggered EM coupling and waveguiding phenomenon.

214 tegrating a small triangular septum into the waveguide plate, we are able to direct the THz light dow

215 of graphene with a critically coupled planar waveguide platform that enables highly sensitive detecti

216 of TE-polarised light--and acts as a TM-pass waveguide polariser.

217 hat can deliver multicolor light at a common waveguide port to achieve multicolor modulation of the s

218 r splitting router based on a parallel-plate waveguide (PPWG) T-junction excited by the TE1 waveguide

219 eguide that allows for multi-modal tuning of waveguide properties through core liquids and pressure/d

220 The waveguiding properties of silk fibroin of largely unproc

221 with the diffractive plasmon excitation, our waveguides provide polarization separation.

222 The reported composite waveguide provides a new method for sound regulation at

223 aveguide (CPW) to planar staggered plasmonic waveguide (PSPW) transitions are designed to achieve smo

224 scale enabled by planar staggered plasmonic waveguides (PSPWs).

225 Here we use passive ocean acoustic waveguide remote sensing (POAWRS) in an important North

226 Plasmon waveguide resonance (PWR) allows following GPCR lipid re

227 n temperatures of a superconducting coplanar waveguide resonator (CPWR) coupled to a sphere of yttriu

228 hat breaks time-reversal symmetry within the waveguide-resonator system.

229 onditions for achieving critical coupling in waveguide-resonator systems.

230 erent transverse mode families in multi-mode waveguides results in periodic disruption of dispersion

231 Epitaxially grown GaAs slab waveguides serve as optical transducer for tailored evan

232 First, long-range surface plasmon polariton waveguides show propagation distances of a few centimete

233 We developed a device composed of an optical waveguide, six electrodes and two microfluidic channels

234 The waveguide structure was fabricated by the complementary

235 ctness and environmental robustness from the waveguide structure.

236 characteristic absorption regime, our mid-IR waveguide successfully perform label-free monitoring of

237 as pressure and the length and radius of the waveguide such that bright coherent high-order harmonics

238 ng to a number of elaborate designs, such as waveguide supperlattice and nanophotonic cloaking, among

239 coupling efficiency of the VCSEL emission to waveguided surface plasmon polariton modes has been opti

240 first time that the design of an optofluidic waveguide system can be optimised to enable simultaneous

241 usability of the integrated ring resonator - waveguide system was examined by depositing, removing, a

242 zation-dependent beam-splitter in the hybrid waveguide system.

243 Implementation of THz coaxial waveguide systems however requires THz beams with radial

244 will evolve into the parabolic pulses in the waveguide taper designed.

245 In particular, we use waveguide tapers to improve the efficiency of excitation

246 ts recent advances on mid-infrared thin-film waveguide technology and on-chip photonics facilitating

247 We demonstrate a photonic waveguide technology based on a two-material core, in wh

248 nce and versatility of GaAs/AlGaAs thin-film waveguide technology in combination with quantum cascade

249 s forms a liquid-core multimode interference waveguide that allows for multi-modal tuning of waveguid

250 We used an integrated plasmonic gap waveguide that strongly confines light within a nonlinea

251 and liquid-core polydimethylsiloxane (PDMS) waveguides that also provides fully functioning microval

252 Specifically, we experimentally demonstrated waveguides that are spaced by a distance of approximatel

253 of fabricating metal-nanostripes-dielectric waveguides that can be used as essential elements in opt

254 silicon using a new class of optomechanical waveguides that control both light and sound.

255 uidic platform, integrating liquid-core PDMS waveguides, that allows the accurate measurement of abso

256 By embedding them in nanophotonic waveguides, they provide a promising platform for quantu

257 near process in a commercial lithium-niobate waveguide through optical arbitrary waveform generation,

258 e the light-scattering patterns of a silicon waveguide through wavelength- and polarization-dependent

259 se a magnonic counterpart of a core-cladding waveguide to control the wave propagation in the junctio

260 is paper, we use a multi-mode optomechanical waveguide to create stimulated Brillouin scattering betw

261 rotocol that allows photons propagating in a waveguide to interact with each other through multiple b

262 kefield accelerator, uses a dielectric lined-waveguide to support a wakefield used for acceleration.

263 allic-elliptical discs as whispering gallery waveguides to control artificial-atoms.

264 duction, droplet generation, microfabricated waveguides to deliver UV light to the droplet flow for p

265 single-mode, high index-contrast dielectric waveguides to free-space beams forming micron-scale diff

266 Using an optical network with nonlinear waveguides to represent the graph and a feedback loop, w

267 with the aid of a properly designed coplanar waveguide transducer generating a nonuniform microwave m

268 revealing that the proposed phononic crystal waveguide transducer successfully attenuates second harm

269 evelopment of an ultrasonic phononic crystal waveguide transducer that exhibits both single and multi

270 lation can be obtained within any dielectric waveguide using only a whispering-gallery microresonator

271 rse spatial modes within a single multi-mode waveguide using quantum circuit-building blocks.

272 ted attosecond pulses in a gas-filled hollow waveguide using synthesized few-cycle two-color laser wa

273 ate the launching of THz pulses into coaxial waveguides using the effect of THz pulse generation at s

274 In all above cases, the waveguide was able to couple out and guide the laser emi

275 quartz Love wave device with a layer of SiO2 waveguide was combined with gold nanoparticles (Au NPs)

276 uishable Raman photons emitted into a single waveguide, we observe a quantum interference effect resu

277 Using comb-shaped planar waveguides, we achieve a full thickness (>10 mm) wound c

278 mplemented with silicon nitride nanophotonic waveguides, we observe 97% interference visibility when

279 Unlike in optical fibres and semiconductor waveguides, we observe that the microcavity wire Cherenk

280 ingle-mask standard lithography, whereas the waveguides were inscribed in the proximity of the ring r

281 e necessary anomalous dispersion, multi-mode waveguides were previously implemented in Si3N4 microres

282 The isolators are simple 1D 2-element waveguides, where garnet claddings and longitudinal magn

283 study the paraxial light propagation in the waveguide which shows that the propagation dynamics is l

284 upconversion photon detector using a similar waveguide, which attains 34% internal conversion efficie

285 a pathway to biocompatible and bioresorbable waveguides, which could be used to deliver localized opt

286 monolayer graphene as a mid-infrared surface waveguide, whose optical response is spatially modulated

287 egion coupling between a WGM resonator and a waveguide will benefit both fundamental studies and prac

288 gle atom or atom-like system coupled to a 1D waveguide with a distant mirror, where guided photons re

289 ed highly confined sub-wavelength dielectric waveguide with a low-visibility and broadband optical ac

290 action of confined THz waves in a novel slot waveguide with an electronically tunable two dimensional

291 This is achieved in a two-dimensional waveguide with periodically varying air channel that mod

292 rametric downconversion in a lithium niobate waveguide with specially designed geometry and periodic

293 ance of approximately lambda0/2 and designed waveguides with centre-to-centre spacing as small as 600

294 multipath behavior may be intrinsic to these waveguides with consequent nonlinearity.

295 Here, we combined zero-mode waveguides with fluorescence resonance energy transfer (

296 acturing but previously thought to result in waveguides with high normal dispersion.

297 ory of parabolic pulse generation in passive waveguides with increasing nonlinearity is presented.

298 g us to demonstrate TPA-free CMOS-compatible waveguides with low linear loss ( 1.5 dB/cm) and enhance

299 using an engineered network of laser-written waveguides, with relative energies and inter-waveguide c

300 DNA molecules into the confines of zero-mode waveguides-zeptolitre optical cavities in which DNA sequ

301 Here, we combine nanophotonic zero-mode waveguides (ZMWs) with fluorescence resonance energy tra