ライフサイエンスコーパス: resonator

1 vely in travelling-wave systems (rather than resonators).

2 es to control the resonance frequency of the resonator.

3 resonator and the fundamental mode of a NEMS resonator.

4 selective optical coupling mechanisms to the resonator.

5 driven optical modes via a common mechanical resonator.

6 frequency-tunable high impedance SQUID array resonator.

7 to generate dual-frequency combs in a single resonator.

8 nk resonant circuit to actuate the MEMS/NEMS resonator.

9 (2)) integrated in a silicon nitride grating resonator.

10 tween the capacitive gaps of each split-ring resonator.

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

12 odes in a phononic-bandgap shielded membrane resonator.

13 nd transition to travelling waves within the resonator.

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

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

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

17 een observed for the first time in an AlGaAs resonator.

18 quantum emitter coupled to a nano-mechanical resonator.

19 ent apparatus we consider a nonlinear driven resonator.

20 able ESR spectrometer equipped with a high-Q resonator.

21 directly measuring rotations applied to the resonator.

22 as rate and volume, and the dimension of the resonator.

23 ity factor (Q) whispering-gallery mode (WGM) resonators.

24 bust nonreciprocal coupling between phononic resonators.

25 is control represents a way to cool phononic resonators.

26 mand biosensors based on high quality phonon resonators.

27 ified by measurements on perturbed microwave resonators.

28 quality-factors (Q) in gyroscopic-mode disk resonators.

29 oherence and single-shot readout in photonic resonators.

30 FWM is enhanced with respect to the isolated resonators.

31 e-way propagation of acoustic energy between resonators.

32 significant dissipation mechanisms for these resonators.

33 he torsional resonators with thickness-shear resonators.

34 rials or through coupling between qubits and resonators.

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

36 dies and practical applications based on WGM resonators.

37 er types of MRI scanners and field-enhancing resonators.

38 determined distance of about the size of the resonators.

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

40 ing of two mutually coupled active microring resonators.

41 f optomechanical states between two separate resonators.

42 s are self-sustaining optical wavepackets in resonators.

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

44 s in an array of two or three weakly coupled resonators.

45 lators, based upon photonic crystal nanobeam resonators.

46 pological insulator using negatively coupled resonators.

47 tion processes of qubits placed in different resonators.

48 than to the detailed structure of individual resonators.

49 based on two side coupled silicon microring resonators.

50 h nanophotonic interface for carbon nanotube resonators.

51 e of their ability to confine light, optical resonators(1-3) are of great importance to science and t

52 memory integrated in a nanophotonic diamond resonator(17-19) to implement asynchronous photonic Bell

53 olecular scale, such as in a carbon nanotube resonator(3-7), their vibrations become increasingly cou

54 queezing(1,3) in a superconducting microwave resonator(4).

55 ons as optical waveguides, filters and laser resonators(4), for improving light-harvesting technologi

56 , using frequency locked microtoroid optical resonators, a 3 orders of magnitude improvement in detec

57 f biosensor microscopy that we call Photonic Resonator Absorption Microscopy (PRAM).

58 regains certain characteristics of a linear resonator, albeit at large amplitudes.

59 ectrons in a dot integrated with a microwave resonator, allowing us to study the electrons' response

60 rser or denser arrangement of the split cube resonators, allowing to cover the entire atmospheric tra

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

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

63 bitrary number of optical sources by using a resonator and evaluate advantages and drawbacks of reson

64 luding thermal noise, frequency noise of the resonator and noise in the feedback circuitry.

65 Using the suspended microchannel resonator and protein synthesis assays, we quantify mass

66 several vibration modes of a microplate MEMS resonator and the fundamental mode of a NEMS resonator.

67 r is presented that has a number of discrete resonators and an exponential frequency distribution.

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

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

70 cal motion is key to characterize mechanical resonators and exploit them for new applications.

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

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

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

74 igm to construct NLMMs consisting of coupled resonators and pave the way toward the utilization of NL

75 Our results pave the path for integrated SiC resonators and resonant gyroscopes with Q-factors beyond

76 including nanolasers, quantum optomechanical resonators, and integrated photonic circuits.

77 ach for metamaterials incorporating internal resonators, and provide numerical and experimental evide

78 ecule to have energy equipartition among the resonators, and suppress FWM by making the two Signal wa

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

80 of conductively-coupled split-cube magnetic resonators, appropriately rotated to each other to besto

81 Microring resonators are a type of whispering gallery mode sensor

82 The SiC disk resonators are anchored upon an acoustically-engineered

83 However, when the resonators are closer, the finite-size and geometry of t

84 ng PCM-clad silicon waveguides and microring resonators are demonstrated.

85 Mechanical resonators are important components of devices that rang

86 Such deeply subwavelength resonators are of interest for high-density optoelectron

87 Dual-mode electromagnetic resonators are used in numerous systems and applications

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

89 Mechanical resonators are widely used as precision clocks and sensi

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

91 strate the use of silicon photonic microring resonator arrays as a postcolumn detector for capillary

92 ed the utility of silicon photonic microring resonator arrays as a quantitative mass concentration de

93 teins, exemplifying the promise of microring resonators arrays as a biocompatible detector for capill

94 a family of single crystal silicon Lame-mode resonators as a function of temperature, from 80-300 K.

95 the possibility of using high-quality-factor resonators as quantum memories(3,9).

96 By dynamically modulating a resonator at frequencies commensurate with its mode spac

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

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

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

100 o/nano-electromechanical systems (MEMS/NEMS) resonators at their fundamental and higher order vibrati

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

102 urfaces, consisting of a graded array of rod resonators attached to an elastic substrate that, togeth

103 s a new biological sensor which represents a resonator based on a segment of a rectangular waveguide

104 repetition rate in externally driven optical resonators based on the gain-through-filtering process,

105 A split-cube-resonator-based metamaterial structure that can act as a

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

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

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

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

110 nstrating that two-qubit gates mediated by a resonator can achieve fidelities >99% under realistic co

111 shows for the first time that a metamaterial resonator can be detuned during transmission and tuned d

112 Systems of closely-spaced resonators can be strongly coupled by interactions media

113 We show that networks of coplanar waveguide resonators can create a class of materials that constitu

114 ics based on micro-electro-mechanical-system resonators can manipulate hard X-ray pulses on time scal

115 ent a two-dimensional optomechanical crystal resonator capable of achieving large cooperativity C and

116 carrier lifetimes using a passive microwave resonator circuit.

117 tic topological matter (here twisted optical resonators). Combined with advances in Rydberg-mediated

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

119 Capacitively-transduced SiC BAW disk resonators consistently display gyroscopic m = 3 modes w

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

121 Lattices of coplanar waveguide resonators constitute artificial materials for microwave

122 Driven passive optical resonators constitute the ideal platform for OFC generat

123 quantization of a megahertz radio-frequency resonator, cooled it to the ground state, and stabilized

124 ed, operated, and measured through a readout resonator coupled with an ancillary superconducting qubi

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

126 of hexagonal-shaped complementary split ring resonators (CSRRs), arranged in a honey-cell configurati

127 s high-momenta mode become possible with our resonator design that can boost the coupling efficiency

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

129 sion, imposing restrictions on materials and resonator design.

130 It is shown that the damping within the resonators determines the trade-off between the frequenc

131 We first test the automatic resonator detuning on-the-bench, and subsequently evalua

132 Despite the numerous works on coupled resonator devices, which showed record conversion effici

133 oustic detection in a differential Helmholtz resonator (DHR).

134 With the reduction of resonator diameter, high repetition rates up to 1 THz be

135 es destabilized by the interplay between the resonator dispersion and the Kerr nonlinearity of the co

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

137 does not require specific engineering of the resonator dispersion to generate frequency-agile OFCs.

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

139 r magnesium fluoride whispering gallery mode resonator enables both high passive stability and 1 kHz

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

141 that are computationally efficient for large resonator ensembles.

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

143 The resonators exhibit temperature sensitivity of -1.8 GHz K

144 the post-measurement state of the nonlinear resonator exhibits a large correlation with the post-mea

145 n carbide-on-insulator (4H-SiCOI) mechanical resonators fabricated at wafer-level, and reports on ult

146 anescently coupled pair of microdisk optical resonators fabricated from solution-processed colloidal

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

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

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

150 ction-evading measurements in nanomechanical resonators for optical ultrasensitive measurements of mo

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

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

153 Releasing the resonator from our control, we observed its rethermaliza

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

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

156 graphene oxide integrated silicon micro-ring resonator (GOMRR) to a range of vapour phase Volatile Or

157 rigeration of a semiconductor optomechanical resonator >20 K below room temperature based on the emis

158 two-level systems (qubits) in a single-mode resonator has recently been theoretically predicted.

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

160 ly-refrigerating the lattice of a dielectric resonator has the potential to impact several fields inc

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

162 e quantum system on a macroscopic mechanical resonator, has remained elusive.

163 Micro and nanomechanical resonators have been extensively researched in recent de

164 ilicon Microelectromechanical Systems (MEMS) resonators have broad commercial applications for timing

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

166 Microring resonators have optical properties that are sensitive to

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

168 e composite high-overtone bulk acoustic wave resonator (HBAR) is a popular phonon source well suited

169 iques to control the eigenmodes of dual-mode resonators, highlighting the strong connection between t

170 pling the composite to an inductor-capacitor resonator, i.e., an antenna.

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

172 it is possible to use the battery cell as a resonator in a tuned circuit, thereby allowing signals t

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

174 si-standing wave field formed in an acoustic resonator in front of the sensor.

175 dulation of the absorption of the dielectric resonator in the hybrid metamaterial is also demonstrate

176 witching mechanism automatically detunes the resonator in transmit mode, while retaining its sensitiv

177 where the two qubits are placed in different resonators in an array of two or three weakly coupled re

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

179 se structures feature a distributed feedback resonator integrated into a bottom LED electrode.

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

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

182 On one side, the resonator is bounded by a metallic short-circuited wall;

183 The energy damping time in a mechanical resonator is critical to many precision metrology applic

184 ed, hydrogel-interlayer Radio-Frequency (RF) resonator is demonstrated as a highly-responsive, passiv

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

186 m-sealed microelectromechanical silicon ring resonator is employed in this work, with relevance to th

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

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

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

190 However, the performance of MEMS resonators is constrained by dissipation mechanisms, som

191 non transmission coefficient between any two resonators is independent of the direction of transmissi

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

193 and within the extinction spectra of coupled resonators is the dipolar coupling band.

194 ause of the strong nonlinear response of the resonator it works in a practical regime where a linear

195 es counter-propagating lightwaves within the resonator, it also functions as a sensitive gyroscope fo

196 ormula: see text] MHz, greatly exceeding the resonator linewidth [Formula: see text] MHz.

197 For these separations, the microring resonators maintain a linear response over several order

198 orateded either through the use of nonlinear resonator materials or through coupling between qubits a

199 In addition, optically refrigerated resonators may be used in the future as a promising star

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

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

202 closer, the finite-size and geometry of the resonators modifies the excitation modes, in particular

203 g males show enhanced variation in vestigial resonator morphology under varied genetic backgrounds.

204 Our ultra-thin reflectarrays employ resonators of variable sizes to cover the full 2pai phas

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

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

207 For comprehensive analysis, torsional resonators operating on three different modes of vibrati

208 These arrays of electromagnetic resonators (or meta-atoms) carrying short wavelength ele

209 The active tuning of the inter-resonator phase and of their eigenfrequencies allows set

210 action is mediated either by real or virtual resonator photons.

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

212 of-of-concept experimental result in a fibre resonator, pioneering a new technique that does not requ

213 s demonstrate the potential of the microring resonator platform as a detector for industrial polymer

214 Our acoustic plasmon resonator platform is scalable and can harness the ultim

215 with generic planar photonic waveguides and resonators, promising a pathway towards on-chip many-bod

216 Here we combined a 14.3 MHz quartz crystal resonator (QCR), actuated and analysed using a fixed fre

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

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

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

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

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

222 With the resonator serving as the frequency-selecting element in

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

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

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

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

227 A 3D array of split ring resonators (SRR) is enveloped by an inductively heated a

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

229 tion (SHG) of vertical and planar split-ring resonators (SRRs) that are broken centro-symmetry config

230 uinely superdirective array using split ring resonators (SRRs).

231 upled to four frequency-selective split-ring resonators (SRRs).

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

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

234 nowire is configured as an electromechanical resonator such that its mechanical vibration is associat

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

236 for achieving critical coupling in waveguide-resonator systems.

237 plitude amplification is reported across the resonators terminals.

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

239 this by using an intermediary nanomechanical resonator that converts the electrical excitation of the

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

241 ment of large-channel suspended microchannel resonators that allow us to monitor buoyant mass of sing

242 e resulted in point-dipole approximations to resonators that are computationally efficient for large

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

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

245 and thermally tensions a suspended graphene resonator, thereby shifting its resonant frequency.

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

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

248 that can automatically detune a metamaterial resonator to enhance magnetic resonance imaging (MRI) pe

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

250 combined with high-quality-factor Si(3)N(4) resonators to provide microcombs with repetition frequen

251 Systems of mechanical resonators typically obey reciprocity, which ensures tha

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

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

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

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

256 This resonator was connected through a coaxial-waveguide adap

257 In addition, a 3D volume slotted-tube resonator was produced that allowed for 2D (1)H-(13)C NM

258 , by directly monitoring the dynamics of the resonators we show that this nonreciprocity can control

259 In an enclosed glass-PDMS-glass (GPG) resonator, we exploit a three-layer microfluidic archite

260 Using a graphene-based magnetic resonator, we realized single, nanometer-scale acoustic

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

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

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

264 tterns with strongly coupled electromagnetic resonators, we transform a single-band FSS to a dual-ban

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

266 ork, using a simple macroscopic, fiber-optic resonator where the nonreciprocity is induced by breakin

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

268 orating a highly specialized radio-frequency resonator, where a high degree of proton-spin polarizati

269 ound the necks of single-resonance Helmholtz resonators, where acoustic energy is concentrated, we sh

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

271 detection of Akhiezer dissipation in a MEMS resonator, which is widely considered to be the ultimate

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

273 ve device elements, including waveguides and resonators, which are seamlessly integrated with convent

274 unit-cell, which consists of four split ring resonators, which are sequentially rotated around the un

275 However, the miniaturization of cavity resonators, which are the essential components of photon

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

277 th high quality factor microwave and optical resonators will enable efficient transduction and create

278 frequency comb threshold of only ~36 uW in a resonator with a 1 THz free spectral range, ~100 times l

279 tion(8-13) bolometer embedded in a microwave resonator with a resonance frequency of 7.9 gigahertz an

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

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

282 and demonstrate a graphene acoustic plasmon resonator with nearly perfect absorption (94%) of incide

283 Here we design a micromechanical resonator with non-monotonic dependence of the eigenfreq

284 stem consists of a temporally modulated ring resonator with spatial coupling between the clockwise an

285 ses electro-optic (EO) phase modulation in a resonator with strong second-order nonlinearity, resulti

286 In this study, we endow a single ring resonator with two independent physical synthetic dimens

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

288 that integrates nanomechanical piezoelectric resonators with a microwave superconducting qubit on the

289 Superconducting resonators with high quality factors have been fabricate

290 limited to low magnetic fields or the use of resonators with high-quality factors.

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

292 We show that Ge-SiC resonators with nanoscale footprint can support sheet an

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

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

295 This is achieved by timing the resonators with the storage ring to diffract X-ray pulse

296 ration, one might even replace the torsional resonators with thickness-shear resonators.

297 e-locked lasers(10) or dispersion-engineered resonators with third-order Kerr nonlinearity(11).

298 Micromechanical resonators with ultra-low energy dissipation are essenti

299 By comparing these Q measurements on resonators with variations in design, dimensions, and an

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