ライフサイエンスコーパス: resonator

1 , using Mach-Zehnder interferometers or ring resonators).

2 n, when larger perturbations are made to the resonator.

3 of mechanical motion--from a nanomechanical resonator.

4 d by residual thermal-photons in the readout resonator.

5 superconducting qubit coupled to a microwave resonator.

6 ano-fibre with a side-coupled toroidal micro-resonator.

7 tem that consists of two bright and one dark resonator.

8 ween the pump and signal in the small volume resonator.

9 RGO-ZnO NW adsorption on the DNA immobilized resonator.

10 n a custom GaN-based high-quality (Q-factor) resonator.

11 odes in a phononic-bandgap shielded membrane resonator.

12 nd transition to travelling waves within the resonator.

13 entical) states of light to circulate in the resonator.

14 al study of the mechanical modes in the ring resonator.

15 and large tunability of subwavelength, low-Q resonators.

16 of a linear array of coupled superconducting resonators.

17 ssive (lossy) and active (with gain) optical resonators.

18 oaded with complementary electric split ring resonators.

19 dies and practical applications based on WGM resonators.

20 sensor using silicon nitride (SiN) microring resonators.

21 ions between optical cavities and mechanical resonators.

22 d numerical characterization of Silicon disk resonators.

23 near mode coupling among micro and nano beam resonators.

24 ve been observed in polar dielectric optical resonators.

25 , nanometre features into tunable mechanical resonators.

26 lossy pseudo-isospectral chains of photonic resonators.

27 (buckliballs) with embedded electromagnetic resonators.

28 cient spin-photon interfaces such as optical resonators.

29 surfaces of inverted-wedge silica microdisk resonators.

30 ase bandwidth, number of modes, or number of resonators.

31 ucial requirement for quantum computing with resonators.

32 a-only resonators are realized in the hybrid resonators.

33 ng the folding state of Miura-ori split-ring resonators.

34 determined distance of about the size of the resonators.

35 h slit being loaded by an array of Helmholtz resonators.

36 ing of two mutually coupled active microring resonators.

37 f optomechanical states between two separate resonators.

38 s are self-sustaining optical wavepackets in resonators.

39 ver many hours with a suspended microchannel resonator, accurately defined the drug sensitivity or re

40 en a whispering-gallery-mode (WGM) microdisk resonator and a fiber taper which exchange energies at t

41 ough assembling and testing of a microtoroid resonator and a radio frequency (RF) microelectromechani

42 ehavior in two-region coupling between a WGM resonator and a waveguide will benefit both fundamental

43 ed on the detuning between a passive optical resonator and an external pump laser.

44 terised using a 15 GHz split post dielectric resonator and had real relative permittivities in the ra

45 a tunable quarter wavelength superconducting resonator and modulate its resonant frequency at twice i

46 zation of our method for any type of optical resonator and noise characteristics.

47 multaneously through a suspended nanochannel resonator and show that four resonant modes are sufficie

48 ections between the "quasi-open" boundary of resonator and the "close" boundary of reflector.

49 iples in a silica microtoroid optomechanical resonator and use quantitative heterodyne spectroscopy t

50 , planar integrated circuits, compact high Q-resonators and broadband, slow-light devices in the THz

51 e characteristics of whispering-gallery-mode resonators and demonstrate a resonator-stabilized laser

52 n with improved performance over silica-only resonators and electro-optic modulation not achievable i

53 Its high Q-factor has been exploited to make resonators and filters in microwave devices, but it also

54 bons functioning as both localized plasmonic resonators and local Joule heaters upon application of a

55 ear, which are not as apparent in individual resonators and may be associated with interference betwe

56 damental aspects of classical nanomechanical resonators and pave the way to a new generation of chemi

57 ect state in a chain of dielectric microwave resonators and show that the functionality of the system

58 To demonstrate detectability using the ring resonators and to optimise conditions for solid-phase am

59 te vibration modes in a micromechanical disk-resonator, and is not externally applied.

60 illating state, with 185+/-15 photons in the resonator, and one with zero oscillation amplitude.

61 rption processes in a silicon nanomechanical resonator, and perform a measurement similar to that use

62 rochannels embedded within a micromechanical resonator, and the elongation of these fibrils under a c

63 rved at the perimeter of acoustic or optical resonators, and by the appearance of a Fabry-Perot inter

64 ed lasing, single-mode lasing from multimode resonators, and non-reciprocal effects in conjunction wi

65 tween the gain and loss in the two microring resonators, and the incorporation of phase modulators in

66 Small resonator antennas, such as metaresonator antennas, have

67 om single- and multilayer QD films on silver resonators are described quantitatively by a photophysic

68 Electromagnetic resonators are integrated with advanced elastic material

69 However, real resonators are not smooth and electrodes have their intr

70 tic modulation not achievable in silica-only resonators are realized in the hybrid resonators.

71 Whispering gallery mode (WGM) resonators are small, radially symmetric dielectrics tha

72 These resonators are typically described in terms of a spheric

73 Traditionally, the over-coupled microring resonators are used to form the differentiators with 1 <

74 Systems of coupled mechanical resonators are useful for quantum information processing

75 he combination of silicon photonic microring resonator arrays and nanodiscs enables rapid interrogati

76 suggested that silicon metasurfaces with Mie resonator arrays can provide useful insights to guide fu

77 ailability of on-chip solid-state mechanical resonators as light-matter quantum interfaces.

78 n a fiber taper is moved laterally above the resonator at fixed vertical distance.

79 eveal the environmental sensitivities of the resonator at the thermodynamical noise limit and long-te

80 from intentionally varying a parameter in a resonator at twice its resonant frequency, has been succ

81 the light fields coupled into and out of the resonator at two distinct regions and the light transmit

82 method can realize anomalous dispersion for resonators at almost any wavelength and simultaneously a

83 , including an array of coupled on-chip ring resonators at communication wavelengths.

84 , robust, and easily assembled gold nano-gap resonators at room temperature.

85 acterize the stability of whispering-gallery resonators at their fundamental noise limits.

86 posited on gold electrodes of quartz crystal resonators (Au-QCRs) or Au-glass slides by oxidative pot

87 sample restrictions imposed by conventional resonator-based ESR detection and renders the technique

88 avefunction and the potential for mechanical-resonator-based quantum information and metrology applic

89 We show that ring-resonator-based spontaneous four-wave mixing photon-pair

90 m the Larmor radiation of adjacent plasmonic resonators because their inclusion in a simple model acc

91 structures for switchable microwave overtone resonators, binary and quadrature phase-shift keying mod

92 novel approach to effectively tuning a laser resonator but also new insight into potential applicatio

93 hase shift (NRPS) in interferometers or ring resonators, but to date NRPS requires TM-modes, so the T

94 squared thermal motion of a micro-mechanical resonator by exploiting the intrinsic nonlinearity of th

95 ontaneous four-wave mixing in a silicon ring resonator by studying the corresponding stimulated proce

96 a radio-frequency micromechanical plate-type resonator by the radiation pressure force generated by a

97 were inscribed in the proximity of the ring resonator by using 3-dimensional femtosecond laser inscr

98 iple eigenmode frequencies of nanomechanical resonators can determine the position and mass of surfac

99 s of hundreds of nanometers, while microwave resonators can extend the entanglement to macroscopic di

100 t of the material refractive index along the resonator chain.

101 The band-structure of the finite periodic PT resonator chains is compared to infinite chains in order

102 r system is composed of an array of five SAW resonators coated with three types of odorant-binding pr

103 As such, nanoscale resonators composed of these materials demonstrate figur

104 ear diatomic elastic metamaterial using dual-resonator concept to obtain large asymmetric elastic wav

105 nances in ultrathin metal nano-strip optical resonators consisting of an array of metallic subwavelen

106 We find that an optimal 6 dB undercoupled resonator consumes 40% less power in our platform to ach

107 e propose an approach that uses a mechanical resonator coupled with the optical fibre system to produ

108 rid structures comprising graphene plasmonic resonators coupled to conventional split-ring resonators

109 ures of a superconducting coplanar waveguide resonator (CPWR) coupled to a sphere of yttrium-iron gar

110 ers, we create whispering-gallery mode (WGM) resonators defined by circular pn junctions, induced by

111 e, Kim et al. propose a concentric racetrack-resonator design where the dispersion can be engineered

112 sion, imposing restrictions on materials and resonator design.

113 An optical mode of a compact Fabry-Perot resonator detects these modes' motion with a measurement

114 We introduce a way of measuring resonator dispersion and detuning of comb modes in a hot

115 show that such constraints can be lifted and resonator dispersion can be engineered to be anomalous o

116 now since an exact one-dimensional harmonic resonator does not exist in nature and has not been crea

117 mensional quantum systems and classical wave resonators due to simple symmetries.

118 mitted by the spins into a coupled microwave resonator during their Larmor precession.

119 ponding electrical admittance spectra of TSM resonators during this process were recorded.

120 metallic patches to U-shaped and split-ring resonator elements, whose spectral response is derived f

121 at asymmetric optical pumping of a symmetric resonator enables a dramatic chiral cooling of clockwise

122 oration of phase modulators in the microring resonators enables continuous wavelength tuning.

123 sly oscillating multiple modes of mechanical resonators, enabling frequency measurements that can pre

124 reported up to now for purely nanomechanical resonators, even if classical mechanical analogies were

125 e separation distance between QDs and silver resonators, excitation wavelength, and QD film thickness

126 The resonators exhibit temperature sensitivity of -1.8 GHz K

127 are combined similar to the case of coupled resonator filters, forming a blazing passband between th

128 ins a challenge owing to the rigidity of the resonator for the generation of coherent loops.

129 factor ( 10(7)) capillary-based optical ring resonators for non-contact detection of air-coupled ultr

130 astically improves intracellular delivery of resonators for several cell types, including mitotic and

131 of intense research in micro- and nanoscale resonators for their use to improve oscillator performan

132 he motional degrees of freedom of an optical resonator, for example, by imparting radiation pressure

133 Dielectric resonators form the building blocks of nano-scale optica

134 with an exponent determined by the 1/f-type resonator frequency noise.

135 nsemble, enables the cooling of a mechanical resonator from room temperature to a fraction of its the

136 g crystalline zinc selenide microcylindrical resonators from our semiconductor fibre platform and dem

137 rption modulators are based on a Fabry-Perot-resonator geometry that allows modulation depths over 30

138 alysed, and results show that the mechanical resonator has the capability to control the dynamics of

139 a in metamaterials through coupled classical resonators has attracted enormous interest.

140 of nonlinear mode coupling in micro and nano resonators has become an imminent necessity for their su

141 re on larger objects such as micromechanical resonators has been so far limited to its coupling to an

142 of quantum devices incorporating mechanical resonators has opened up new frontiers in the study of q

143 Surface binding measurements with WGM resonators have demonstrated competitive analytical dete

144 Nano-mechanical resonators have gained an increasing importance in nanot

145 ultrahigh-Q optical whispering-gallery-mode resonators have served as a platform for low-noise micro

146 m-walk-noise statistics.High-quality optical resonators have the potential to provide a miniaturized

147 licon integrated devices, such as micro-ring resonators, have recently been demonstrated as efficient

148 depositing the dye-doped polymer on the same resonator hosts for multiple cycles.

149 The ring resonator hosts were patterned by a single-mask standard

150 s, as well as the morphology and strength of resonator hot spots.

151 th is demonstrated by encapsulating the ring resonator in a damping medium.

152 Bacteria are adhered to a quartz crystal resonator in an electronic bridge that is driven by a hi

153 a two level qubit coupled with a single-mode resonator in arbitrary coupling strength regimes beyond

154 tum protocol involving initialization of the resonator in its quantum ground state of motion and subs

155 er graphene, loaded on a Si/SiO2 Fabry-Perot resonator in the 545-700 nm range.

156 demonstrate a dynamic mode coupling between resonators in a hybrid metal-semiconductor metamaterial

157 ivation process, indicating potential of TSM resonators in characterization of cells during their tra

158 hitherto no successful measurements of NEMS resonators in the liquid phases of helium.

159 ontemporary qubits based on transverse qubit-resonator interaction.

160 that integrates a Fabry-Perot type acoustic resonator into a microfluidic channel to separate submic

161 couple, exchanging energy and elevating the resonator into its desirable second-order resonance oper

162 time the acoustic properties of a lattice of resonators, introducing the concept of acoustic Floquet

163 ic pulse and the mechanical mode of the ring resonator is also studied.

164 The detection volume of our resonator is approximately 0.02 nl, and our approach can

165 ation process within an integrated microring resonator is demonstrated here, by simulations, in the s

166 cross-section of the silicon nitride spiral resonator is designed to possess small and flattened gro

167 The in-plane resonator is fabricated from a silicon-on-insulator wafe

168 an be obtained if the over-coupled microring resonator is fitted by an ideal differentiator with n <

169 The centre frequency of the perturbed resonator is inadvertently drifted from its original val

170 The resonator is structured in such a way that the nonlinear

171 or-Prey), where by the microwave mode of the resonator is the predator and the spin polarization in t

172 .Achieving large tunability of subwavelength resonators is a central challenge in nanophotonics.

173 While nonlinear elasticity in silicon resonators is extremely weak, in this high quality-facto

174 Preparation of these non-classical states in resonators is non-trivial due to their inherent harmonic

175 lecules based on surface acoustic wave (SAW) resonators is presented.

176 reusable and wavelength reconfigurable ring resonator lasers and waveguides of arbitrary shapes to o

177 avity can reduce the damping of a mechanical resonator, leading to parametric instability accompanied

178 antibonding resonances of the Born-Kuhn type resonators, leads to an extremely steep dispersion for a

179 of the time delays from the typical inverse-resonator-linewidth scale to the pulse-duration scale.

180 device formed by a pair of electro-acoustic resonators loaded with suitably tailored non-Foster elec

181 tently matched with a single model involving resonator loss, ohmic charge noise and 1/f-flux noise, a

182 This new class of resonators may inspire alternative design concepts, and

183 e interference in a vertically coupled three-resonator metamaterial system that consists of two brigh

184 cal switches based on three types of optical resonators; microring, Fabry-Perot cavity, and plasmonic

185 Cooling a mechanical resonator mode to a sub-thermal state has been a long-st

186 tor, we dynamically control the chirality of resonator modes and the emission direction of a WGM micr

187 he vicinity of an EP: Away from the EPs, the resonator modes are nonchiral and laser emission is bidi

188 light mediated by a multitude of mechanical resonator modes, with quantum noise suppression up to -2

189 acing in a CMOS-compatible high-Q micro-ring resonator (MRR).

190 omplete expression for the dynamic gain of a resonator neuron model in terms of a cascade of filters

191 ormed by combining two cross-shaped metallic resonators of different sizes within a super-unit-cell a

192 Direct coupling is only possible with resonators of very similar frequency, but by using an in

193 e of spatially graded vertical subwavelength resonators on an elastic substrate, the metawedge can ei

194 We demonstrate that for disk resonators on low-index quartz substrates, the electric

195 tuned and electrostatically driven MEMS arch resonator operated in air.

196 trophotonic technology consists of microring resonators optimally n-doped to support high Q resonance

197 electric and magnetic dipoles of split-ring resonators parallel or anti-parallel to each other, lead

198 Besides providing insights into nonlinear resonator physics, they can be applied in frequency metr

199 It is shown that the graphene resonators produce antenna-coupled blackbody radiation,

200 We map five modes of a silicon microdisk resonator (Q>/=20,000) with both high spatial and spectr

201 se chemosensors comprised the quartz crystal resonator (QCR) or extended-gate field-effect transistor

202 ricated using the sol-gel TiO2 material, and resonator quality factors up to 20,000 were measured.

203 surements are performed by SU-8 optical ring resonators reaching detection limits of 0.86ngcm(-2).

204 d of an array of moderately coupled nanopost resonators, realizing axicons, vortex beam generators, a

205 an ultimate resolution limited by the micro-resonator resonance linewidth and can be used in any spe

206 W has been obtained in the silicon microring resonator, respectively.

207 The quartz crystal resonator responding only to mass changes in the lower p

208 symmetry in dual-mode planar electromagnetic resonators results in their ability to host two degenera

209 ability is thought to reach a limit with the resonator's ability to resolve thermally induced vibrati

210 To understand better how a resonator's frequency preference emerges from its intrin

211 wo independent methods, the magnitude of the resonator's response to forcing by radiation pressure is

212 s show high reliability and stability of TSM resonator sensors in monitoring the process of platelet

213 his study, quartz thickness-shear mode (TSM) resonator sensors were adopted to monitor the process of

214 ady rise of resonance frequency shift of TSM resonator sensors.

215 A crossed trapezoid resonator shape of rectangular cross section is used to

216 findings will inspire akin designs for other resonator shapes, in different disciplines and applicati

217 We can tune the resonator size and the carrier concentration under the p

218 n addition, we characterize the influence of resonator size on the spectral characteristics of the em

219 based on a scanning Fabry-Perot micro-cavity resonator (SMART) providing a simple, compact and accura

220 Here, we use a suspended microchannel resonator (SMR) to measure single-cell density, volume,

221 to amyloid fibrils by suspended microchannel resonators (SMR).

222 Shear mode solidly mounted resonators (SMRs) are fabricated using an inclined c-axi

223 A single split-ring resonator (SRR) probe for 2D surface mapping and imaging

224 nar waveguide (CPW) loaded with a split ring resonator (SRR), which was fabricated on a DiClad 880 su

225 Split-ring resonators (SRRs) present an attractive avenue for the d

226 Although measurements and predictions of resonator stability usually disregard fluctuations in th

227 ng-gallery-mode resonators and demonstrate a resonator-stabilized laser at this limit by compensating

228 The localized gap plasmon resonators strongly couple light and mechanical motion w

229 Using a new neutron resonator structure we achieved the required intensity g

230 Unlike traditional optomechanical resonators, such extreme optical confinement yields a fa

231 a picometer-scale dynamic deformation of the resonator surface, which we detect through a shift in th

232 a-averaged periodic tangential stress at the resonator surface.

233 Exploiting both effects within a single resonator system-intrinsic InSb wires on a heavily doped

234 time-reversal symmetry within the waveguide-resonator system.

235 for achieving critical coupling in waveguide-resonator systems.

236 The mixer works essentially as a resonator that accumulates an intensive electromagnetic

237 onstrate a high-frequency bulk acoustic wave resonator that is strongly coupled to a superconducting

238 bsorber consists of eight pairs of gold nano-resonators that are separated from a gold ground plane b

239 Micro-pillars are columnar resonators that can be easily arranged in dense arrays o

240 onventional designs using critically coupled resonators that have the maximum light-matter interactio

241 the potential for creating VO2 based hybrid resonators that operate at THz frequencies.

242 layer-loading transmission line model of TSM resonators, the complex shear modulus (G' + jG'') and th

243 onductor optical amplifiers in the microring resonators, the PT-symmetry condition can be achieved by

244 The spin ensemble is coupled to the resonator through its orbitally-averaged excited state,

245 esonators coupled to conventional split-ring resonators, thus demonstrating a type of highly tunable

246 ispersive materials or structures with local resonators, thus resulting in unavoidable distortion of

247 An alternate method is to couple the resonator to a well-controlled two-level system.

248 arth ions strongly coupled to a nanophotonic resonator to demonstrate a significant cavity protection

249 A DC current is applied through the resonator to induce heat and modulate its stiffness, and

250 Here we use a suspended microchannel resonator to monitor the volume and density of single ce

251 have confined the state of a superconducting resonator to the quantum manifold spanned by two coheren

252 NA analysis using silicon photonic microring resonators to detect cDNA reverse transcription products

253 the interaction between the constituent EIT resonators to efficiently manipulate the focusing intens

254 window of the ZnSe material, we expect these resonators to find use in applications ranging from spec

255 We show that a system with two resonators ultrastrongly coupled to a single qubit can b

256 e correlations in the emitted phonons as the resonator undergoes a parametric instability formally eq

257 ges in a system of two-dimensional arrays of resonators undergoing dynamic modulation of refractive i

258 ) chip featuring an array of 64 optical ring resonators used as refractive index sensors for real-tim

259 ipatively cool a room temperature mechanical resonator using a nitrogen-vacancy centre ensemble.

260 al qubit encoded in a superconducting cavity resonator using four-component cat states.

261 y (Q) factor ring, disk and photonic crystal resonators using a hybrid silicon-on-lithium-niobate mat

262 S/ZnS quantum dots (QDs) on silver plasmonic resonators using photoluminescence (PL) and excitation s

263 The laser resonator was fabricated with a chaotic, D-shaped cavity

264 probe immobilised on the surface of the ring resonators was carried out and detected through the shif

265 th use of the MIP film-coated quartz crystal resonator, was found to be 5.5.

266 Reusability of the integrated ring resonator - waveguide system was examined by depositing,

267 fiber-coupled whispering-gallery-mode (WGM) resonator, we dynamically control the chirality of reson

268 Using a high-Q microtoroid resonator, we realize highly non-reciprocal transport at

269 our wave mixing (SFWM) in an AlGaN microring resonator, we show design techniques to satisfy the phas

270 Using a concentric racetrack-shaped resonator, we show that such constraints can be lifted a

271 Using coplanar photonic bandgap resonators, we drive Rabi oscillations on nuclear spins

272 dex-contrast flexible optical waveguides and resonators were fabricated using the sol-gel TiO2 materi

273 metric resonance in a micromachined membrane resonator when electrically undamped.

274 tum states in circular graphene p-n junction resonators when a relatively small critical magnetic fie

275 ors in the quantum regime.Coupled mechanical resonators where each mode can be separately controlled

276 ng architectures especially in coupled laser resonators where the beam passes through the fan-out ele

277 es in frequency (Deltaf) of a quartz-crystal resonator, which are converted into Deltam using the Sau

278 is based on the electromagnetic modes of its resonator, which provides the feedback required for osci

279 Our designs are based on low-loss dielectric resonators, which introduce a dense spectrum of optical

280 spersion and detuning of comb modes in a hot resonator while generating an optical frequency comb.

281 ometry-invariant resonant cavities, that is, resonators whose eigenfrequencies are invariant with res

282 tasurface comprised of coupled subwavelength resonators, whose optical responses exhibit a remarkable

283 imode nature of the membrane and Fabry-Perot resonators will allow multimode entanglement involving e

284 ining NV spins with levitated optomechanical resonators will provide a hybrid quantum system for nove

285 a silicon-based high-contrast grating (HCG) resonator with a spectral linewidth of ~500 pm that is s

286 idered, and the principle of selectivity for resonator with an arbitrary number of ferroelectric laye

287 The sensor is a microwave microstrip planar resonator with an enhanced quality factor using a regene

288 al, we employ a nonlinear optical micro-ring resonator with high-Q resonant modes for infrared input

289 orming the resonant body of a nanomechanical resonator with simultaneously tailored optical and elect

290 y of a driven system using a micromechanical resonator with two nonlinearly coupled vibrational modes

291 etween two spatially and frequency separated resonators with a mass ratio of 4.

292 antenna substrates and polarization-enabled resonators with angle-insensitive functionalities.

293 fied by engineering both the optical and THz resonators with appropriate effective indices.

294 w class of microwave thin film bulk acoustic resonators with multiband resonance frequency switching

295 ation rotators based on phased arrays of Mie resonators with negligible insertion losses.

296 Lithium-niobate-silica hybrid resonators with quality factors higher than 10(5) are fa

297 the first time that harmonic nanomechanical resonators with relatively high quality factors, such as

298 current technology by using superconducting resonators with tunable boundary conditions.

299 ice is inspired by an asymmetric Fabry-Perot resonator, with pixels comprising a scattering nanopost

300 uced by the near-field coupling of the three resonators within the unit cell.