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1 rpendicularly through the axis of an optical waveguide.
2 t forms an air-gap hybrid photonic-plasmonic waveguide.
3 ng as resonant mirrors in the otherwise open waveguide.
4 e local polarization state of light inside a waveguide.
5 the polarization state of light within that waveguide.
6 ed by the incorporation of antibodies in the waveguide.
7 conducting qubits(8) along a one-dimensional waveguide.
8 ne that can be used as a crystalline optical waveguide.
9 n top of a lithographically defined metallic waveguide.
10 ITO) is used as the semiconductor in the MOS waveguide.
11 ss mechanism by scattering energy out of the waveguide.
12 n to be that of photon tunneling to a nearby waveguide.
13 n of the channel along the length of the MMI waveguide.
14 arated atomic dipoles mediated by an optical waveguide.
15 of 0.90 +/- 0.01 from another (800-nm-wide) waveguide.
16 l-internal-reflection design in a thin-plate waveguide.
17 within an effective mid-latitude atmospheric waveguide.
18 device that integrates a TI with a photonic waveguide.
19 n and (3) to full reflection into the second waveguide.
20 oss of the THz wave propagating through this waveguide.
21 ain a structural wave cloak and a structural waveguide.
22 the performance of the SLL cloak and the SLL waveguide.
23 ined transversely and delivered axially in a waveguide.
24 ection of intracavity emission with a single waveguide.
25 me using integrated TiO(2)-on-LiNbO(3) (ToL) waveguides.
26 by a factor of ~9 in comparison to nonporous waveguides.
27 interfere destructively in the side coupled waveguides.
28 con photonics devices based on rib and strip waveguides.
29 tforward integration with silicon integrated waveguides.
30 ling spin waves in the input junction of the waveguides.
31 id-state quantum emitter-with low-loss Si3N4 waveguides.
32 dic array of silicon strips between adjacent waveguides.
33 ly weak in conventional nanophotonic silicon waveguides.
34 ivalent to a stacked array of parallel-plate waveguides.
35 ments as well, such as vertical silicon slot waveguides.
36 into a six-way crossing of photonic crystal waveguides.
37 wave mixing in low-loss spiralled multi-mode waveguides.
38 enhanced spontaneous emission, and nanoscale waveguiding.
39 n polariton with dielectric-loaded plasmonic waveguiding.
40 l-free sub-diffraction light confinement and waveguiding.
41 is resonator was connected through a coaxial-waveguide adapter to the S parameter meter, by means of
42 tegrated photonic devices based on Si(3)N(4) waveguides allow for the exploitation of nonlinear frequ
43 n the electric field distribution around the waveguide, allowing accurate, frequency-dependent liquid
44 g in straight and curve substrate integrated waveguides, also validating properties of position-indep
45 he quasi-continuous spectrum of modes in the waveguide-an effect that is not achievable using small a
48 upling of SPEs with the guided mode of a SiN waveguide and study how the on-chip single photon extrac
50 y photonic applications ranging from optical waveguides and antennas to signal-enhanced fluorescent s
51 ntation, allowing direct integration of GaAs waveguides and cavities containing self-assembled InAs/G
55 goal by hybrid on-chip integration of Si3N4 waveguides and GaAs nanophotonic geometries with InAs qu
56 lectrode ion-trap chip(8,9) using integrated waveguides and grating couplers, which delivers all the
58 de semiconductor (CMOS) compatible thin film waveguides and microfluidics shows great promise toward
59 ble photonic switches using PCM-clad silicon waveguides and microring resonators are demonstrated.
60 n be integrated with generic planar photonic waveguides and resonators, promising a pathway towards o
61 sults for passive device elements, including waveguides and resonators, which are seamlessly integrat
62 ly efficient optical interface between Si3N4 waveguides and single-quantum dots in GaAs geometries, w
63 we present the realization of such phononic waveguides and the formation of phononic integrated circ
65 etwork is built from a mesh of subwavelength waveguides, and can sustain localised modes and mirror-l
67 missions that leak from the Earth-ionosphere waveguide are primarily responsible for bifurcating the
68 Thanks to these properties, our nonlinear waveguides are able to produce a pi nonlinear phase shif
72 ride thin films, where chirp-modulated taper waveguides are patterned to ensure a broad phase matchin
75 tegration of 'quantum microchiplets'-diamond waveguide arrays containing highly coherent colour centr
76 ility of the antiresonant reflecting optical waveguide (ARROW) biosensor chip, a detection limit of 0
77 ctromagnetic fields produced by a microstrip waveguide as a function of its gigahertz operating frequ
78 generic integral equation and using a set of waveguides as the input and output to the designed metas
79 eguide modes, and enables design of acoustic waveguides as well as seamless integration with electrom
80 ices to sound waves in acoustic-metamaterial waveguides, as well as fermions and phonon polaritons in
81 es a giant atom by coupling small atoms to a waveguide at multiple, but well separated, discrete loca
83 pagating photonic modes make layered crystal waveguides attractive for photonic circuitry and for stu
84 ide array with periodic variations along the waveguide axis, giving rise to nonzero winding number, a
89 implementation and scalability, the proposed waveguide-based extraction method does not require a vac
92 An outlook on the advantages and future of waveguide-based MIR spectroscopy for application in clin
93 4 ng/mL for LPS and 2 ng/mL for LTA using a waveguide-based optical biosensor platform that was deve
95 ays for future miniaturization of dielectric waveguide-based systems with simultaneous polarization a
96 The sensor consisted of As(2)Se(3) optical waveguides built by microelectronic fabrication processe
97 eguides can provide low-loss two-dimensional waveguiding by using space-time wave packets, which are
98 ted by picosecond pulses in microcavity wire waveguides can be understood as the Cherenkov radiation
101 rated that an ultrathin film, being an X-ray waveguide, can also generate fluorescence holograms as a
103 nce (MMI) waveguide crosses multiple fluidic waveguide channels on an optofluidic chip to create mult
104 ansport of energy through 1-dimensional (1D) waveguiding channels can be affected by sub-wavelength d
108 tially resolved near field measurements in a waveguide configuration were performed, allowing us to m
110 d after forward propagating through an ocean waveguide containing 3-D random inhomogeneities from the
111 ropagation loss than its conventional hybrid waveguiding counterpart, while maintaining strong optica
112 ving the full many-body quantum state of the waveguide-coupled system, illustrating that large photon
113 of the promise that many components, such as waveguides, couplers, interferometers and modulators, co
115 nic device consisting of a planar dielectric waveguide covering a gold nanostripe array fabricated on
116 ing element was designed based on a coplanar waveguide (CPW) loaded with a split ring resonator (SRR)
117 A solid-core multimode interference (MMI) waveguide crosses multiple fluidic waveguide channels on
118 nd quantum sensor with optical and microwave waveguide delivery enables thermometry with single-cell
119 method is evaluated by designing a series of waveguide demultiplexers (WDM) and mode converters with
120 ntum to particles in the evanescent field of waveguides depends in a non-trivial way on the polarizat
123 e mode converters, polarization rotators and waveguide devices supporting asymmetric optical power tr
125 ficiency of voltage-induced DNA loading into waveguides equipped with nanopores at their floors is fi
128 served over a broad visible spectrum and the waveguide evanescent wave was used to excite the Raman s
131 lyte molecules, indicating that the hydrogel waveguide film is highly porous to both sizes of molecul
132 are valued for their applications as optical waveguides, filters and laser resonators(4), for improvi
133 attering theories, the thin-film-based X-ray waveguide fluorescence holography becomes a unique in si
134 (PI-SSC) based on phase-matched multi-layer waveguides for efficient coupling between a silicon NW a
135 ssitates the use of dispersive structures or waveguides for extending the field-particle interaction.
136 approach for fabricating mesoporous chitosan waveguides for improving the measurement sensitivity of
137 alls show considerable potential as magnonic waveguides for on-chip control of the spatial extent and
138 e steps within strongly interacting electron waveguides formed at the lanthanum aluminate-strontium t
140 y couple part of the incident light into the waveguide generating bandgaps in the transmittance spect
141 e present the design and characterization of waveguide grating devices that couple visible-wavelength
143 emerging development of the hybrid plasmonic waveguide has recently received significant attention ow
144 ere are two distinct features related to the waveguide: i) It is not absorptive, on the contrary, wea
145 ed to simultaneously image two acrylic, FTIR waveguide imaging elements from below, at frame rates up
147 to mechanically reconfigure organic optical waveguides in order to attain spatial control over their
148 rds the practical implementation of magnonic waveguides in the form of domain walls in future spin wa
149 ily realized in an air environment, acoustic waveguiding in an underwater environment remains elusive
150 ous electromagnetic properties of dielectric waveguides, including mode confinement, polarization, sc
151 propose a novel scheme to realize an optical waveguide induced by an active Raman gain (ARG) process
152 ng is presented as an alternate approach, as waveguides inherently provide a large density of channel
154 e present an experimental demonstration of a waveguide-integrated DLA that was designed using a photo
159 ed schemes where usually the optical induced waveguide is passive and is severely attenuated by the D
160 ing all the optical properties of dielectric waveguides is a challenging task and often requires comp
161 pling between free space components and slab waveguides is a common requirement for integrated optica
162 f 4 to 50 times with respect to the straight waveguides is achieved, depending on the cavity ring rad
165 timization of acrylate based-hydrogel as the waveguide layer formed from PEG diacrylate (PEGDA, M(n)
169 heating provided by plasmonic absorption of waveguided light and resulting inhomogeneous thermally i
173 ve integration, they have suffered from high waveguide losses that prevent the realization of efficie
176 als allow macromolecules to diffuse into the waveguide, maximizing their interaction with the optical
178 iety of unconventional optical responses and waveguiding mechanisms, which can be, in principle, reco
181 re implemented by a two-dimensional photonic waveguide mesh realizes different functionalities throug
183 ieved by reading the intensity change of the waveguide mode at lambda = 2.65 mum, which overlap with
184 ign principle, we experimentally demonstrate waveguide mode converters, polarization rotators and wav
192 we are able to obtain good confinement of a waveguided mode within the QD medium, which allows for d
193 ized ordinary and TM polarized extraordinary waveguide modes can be supported in MoS(2) microcrystals
194 n overcome these issues and can characterize waveguide modes down to a resolution of tens of nanomete
195 we visualize the electric field profiles of waveguide modes in real space and time and extract the t
196 the study of both ordinary and extraordinary waveguide modes in real space, we are able to quantitati
197 emission of photons trapped in substrate and waveguide modes significantly enhance light extraction w
199 are demonstrated as a platform for realizing waveguide modes, and cathodoluminescence spectroscopy is
200 itously employed in electromagnetics to find waveguide modes, and enables design of acoustic waveguid
201 By monitoring the phase velocity of the waveguide modes, we detect incoherent A-exciton bleachin
202 esonator based on a segment of a rectangular waveguide of 8 GHz band with shear dimensions of 28.5 x
204 cal properties and the capability of optical waveguiding of molecular crystals have attracted researc
205 ibit a cutoff width, and thus enables linear waveguiding of the polaritons in arbitrarily narrow ribb
208 cuits consisting of amorphous silicon (a-Si) waveguides on an epitaxial barium titanate (BaTiO3, BTO)
211 m one-way photonic edge states to a selected waveguide output with an isolation ratio in excess of 10
212 omically layered crystals can act as optical waveguides over a broad range of the electromagnetic spe
213 performance for structural wave cloaking and waveguiding over a broadband operating frequency range.
214 d by more than two orders of magnitude for a waveguide pair with an edge-to-edge distance of lambda/3
215 oherent lengths in thin film lithium niobate waveguides patterned with the gradient metasurfaces.
223 and enhanced Raman signal intensity, the AlN waveguides provided a sensor platform for nondestructive
224 tential for control of sound by the acoustic waveguiding provided by a ring of regularly spaced holes
225 coupling with interacting qubits in an open waveguide provides a means of synthesizing multi-photon
228 waves, high-acoustic-index-contrast phononic waveguides remain elusive, preventing intricate manipula
229 tion in microelectronics of such crystalline waveguides requires downsizing and precise spatial contr
230 n temperatures of a superconducting coplanar waveguide resonator (CPWR) coupled to a sphere of yttriu
236 ists of an elastic aluminum rod serving as a waveguide sandwiched between two heavy steel plates.
238 rum scanning at the -OH absorption band, the waveguide sensor was able to identify different hydroxyl
243 el for droplet sorting through a micropillar waveguide structure between the channel and the interdig
244 ed on a metal-oxide-semiconductor (MOS) slot waveguide structure consists of two stubs embedded on th
245 in the device consists of a silicon nitride waveguide structure that can be rapidly (<20 mus) reconf
249 characteristic absorption regime, our mid-IR waveguide successfully perform label-free monitoring of
250 many fluidic applications based on efficient waveguiding, such as in vivo ultrasound medical treatmen
251 ng to a number of elaborate designs, such as waveguide supperlattice and nanophotonic cloaking, among
253 first time that the design of an optofluidic waveguide system can be optimised to enable simultaneous
254 The state of the art of new material and waveguide systems used for spectroscopic measurements in
258 ded holes is shown to act as simple acoustic waveguide that can be readily manipulated to control the
260 ls are evolving as new materials for optical waveguides that can be used for transfer of information
262 uidic platform, integrating liquid-core PDMS waveguides, that allows the accurate measurement of abso
264 near process in a commercial lithium-niobate waveguide through optical arbitrary waveform generation,
265 and detection are obtained through the same waveguide thus simplifying the detection scheme and pote
266 se a magnonic counterpart of a core-cladding waveguide to control the wave propagation in the junctio
267 rotocol that allows photons propagating in a waveguide to interact with each other through multiple b
268 ladding that guides light within an air-core waveguide to provide a new platform to explore ENZ prope
269 single-mode, high index-contrast dielectric waveguides to free-space beams forming micron-scale diff
271 riety of functions through a mesh of on-chip waveguides, tunable beam couplers and optical phase shif
272 erview of the emergence of thin film optical waveguides used for evanescent field sensing of liquid c
273 lation can be obtained within any dielectric waveguide using only a whispering-gallery microresonator
276 ng; implementation of plasmonic cavities and waveguides using plasmonic crystals; and development of
278 quartz Love wave device with a layer of SiO2 waveguide was combined with gold nanoparticles (Au NPs)
279 roscopy using aluminum nitride (AlN) optical waveguides was demonstrated for organic compound analysi
280 tonic implementation of evanescently coupled waveguides, we indicate its ability to independently per
281 Unlike in optical fibres and semiconductor waveguides, we observe that the microcavity wire Cherenk
282 resonant waves generated at the edges of the waveguide were suppressed using spin wave absorbers.
284 upconversion photon detector using a similar waveguide, which attains 34% internal conversion efficie
285 and expulsion of water generates a transient waveguide, which entraps the optical field and suppresse
286 rstanding of hyperbolic polaritons in linear waveguides, which is of critical importance for their ap
287 ze intriguing functions, including efficient waveguiding, which requires large impedance mismatches t
289 egion coupling between a WGM resonator and a waveguide will benefit both fundamental studies and prac
290 gle atom or atom-like system coupled to a 1D waveguide with a distant mirror, where guided photons re
291 ed highly confined sub-wavelength dielectric waveguide with a low-visibility and broadband optical ac
292 action of confined THz waves in a novel slot waveguide with an electronically tunable two dimensional
294 rametric downconversion in a lithium niobate waveguide with specially designed geometry and periodic
295 hip optical gain in erbium-based hybrid slot waveguides with a monolithic, CMOS-compatible and scalab
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 DNA molecules into the confines of zero-mode waveguides-zeptolitre optical cavities in which DNA sequ
300 Here, we combine nanophotonic zero-mode waveguides (ZMWs) with fluorescence resonance energy tra