ライフサイエンスコーパス: resonant

1 h electromagnetic analysis of the ultra-thin resonant absorbers along with their complex characteriza

2 This is obtained by combining resonant absorption and thermoelectric junctions within

3 curs when the plasmonic structure aligns its resonant absorption spectrum with incident illumination

4 ctured materials enable spectrally selective resonant absorption, where the resonant bandwidth and ab

5 ltrasonic spectral evolution, measured using resonant acoustic and ultrasonic spectroscopy, for both

6 M and PV cells in the local circuit entrains resonant activity in the narrow 5- to 30-Hz band and the

7 elationship involves the phenomenon of quasi-resonant amplification (QRA) of synoptic-scale waves wit

8 By combining near-impulsive resonant and non-resonant excitation, the desired fifth-

9 tum regime of ultracold chemistry, observing resonant and nonresonant barrier tunnelling, matter-wave

10 A theory for the calculation of resonant and nonresonant hole-burning (HB) spectra of pi

11 in multivariable sensors that result in non-resonant and resonant electrical sensors as well as mate

12 its the generic capabilities of all types of resonant and wave-guiding systems in photonics, cavity q

13 Kepler-223 system, model these variations as resonant-angle librations, and compute the long-term sta

14 py on hematite particles (10 and 50 nm) with resonant anomalous X-ray reflectivity (RAXR) to single c

15 Time-resolved resonant anomalous X-ray reflectivity measurements at 25

16 Here, we report on all-optical resonant as well as Raman-based coherent control of a si

17 The (13)C{(15)N} REDOR experiments resonant at 165 ppm show an incomplete buildup of the RE

18 Only one mode out of about 20,000 can be resonant at a time.

19 AuNSs performed superior compared to the non-resonant AuNPs.

20 vitro and in vivo the heat generation of the resonant AuNSs performed superior compared to the non-re

21 each bar is a composite on its own, multiple resonant band gaps appear in the compound system which d

22 lly selective resonant absorption, where the resonant bandwidth and absorption intensity can be engin

23 However, due to the limited resonant bandwidth, most periodic plasmonic nanostructur

24 theoretically and experimentally analyze the resonant behavior of individual 3 x 3 gold particle olig

25 ble spectral features include characteristic resonant behaviour, shape-dependent depolarization ratio

26 zoelectric plasmonic metasurface forming the resonant body of a nanomechanical resonator with simulta

27 nge forces along the cubic direction tied to resonant bonding and low lattice thermal conductivity.

28 This behavior has been described in terms of resonant bonding, but puzzles remain, particularly regar

29 atomic interaction induced by a weakening of resonant bonding.

30 Considering a fiber with resonant Bragg gratings as an example, the mechanism of

31 sition of the lowest exciton state, that is, resonant burning allows the protein to access only its c

32 cription of HB data for both nonresonant and resonant burning conditions.

33 Thus, platforms like resonant cavities and photonic crystals that enable the

34 Resonant cavities are essential building blocks governin

35 Resonant cavities are one of the basic building blocks i

36 etically the existence of geometry-invariant resonant cavities, that is, resonators whose eigenfreque

37 geometry, and, thus, the size and shape of a resonant cavity is selected to operate at a specific fre

38 enhanced by placing the quantum system in a resonant cavity.

39 r System by disrupting a theoretical initial resonant chain similar to that observed in Kepler-223.

40 The six inner planets form a near-resonant chain, such that their orbital periods (1.51, 2

41 , and compute the long-term stability of the resonant chain.

42 ation of the trapping process, revealing the resonant character of the trapping efficiency maxima.

43 pecific stimulation efficacy depended on the resonant characteristics of the underlying tremor networ

44 r coils of micron pitch we realize microwave resonant circuits with large electromechanical coupling

45 chmark the unique properties by performing a resonant coherent THz control experiment with few 10 fs

46 ntaining mechanical stability even under the resonant condition of the metallic nanoparticle.

47 gradually transferred into MoS2 under quasi-resonant conditions as compared with their direct photop

48 luminated with monochromatic light under off-resonant conditions.

49 nditions that gradually localizes one of the resonant configurations on compression.

50 ss the underlying physics, particularly, the resonant coupling between molecular and antenna excitati

51 Resonant coupling of plasmons between the gold grating a

52 polarizing reflection can be explained by a resonant coupling with the first-order, in-plane, Bragg

53 xhibits extremely low loss and does not show resonant coupling with the MHA layer.

54 ny-body condensate of optical phonons around resonant defects.

55 Improved chemically actuated resonant devices (CARDs) are fabricated in a single step

56 t lead to the first generation of deformable resonant devices.

57 a finite periodic Parity Time chain made of resonant dielectric cylinders is considered.

58 This paper presents the first electronically resonant DOVE spectra and demonstrates the capabilities

59 itude over conventional controls when a near resonant driving field is modulated by Slepians, and how

60 s a quantum CNOT gate to be implemented with resonant driving in 200 nanoseconds.

61 d electron injection and transport, possibly resonant due to the high electric field present (>3 MV/c

62 estingly, the results obtained from showcase resonant dye and nonresonant thiophenol monolayers adsor

63 plasmon-mediated efficiency enhancement is a resonant effect, and therefore, dependent on the wavelen

64 The origin of this non-resonant effect, extraordinarily strong among other non-

65 The resonant elastic X-ray response at the K-edge, which was

66 We show that the line-shape of the measured resonant elastic X-ray response can be explained with th

67 Here we observed with resonant elastic X-ray scattering a distinct type of ele

68 able sensors that result in non-resonant and resonant electrical sensors as well as material- and str

69 A doubly-resonant electro-optic modulator (EOM) is a promising pl

70 These states assist resonant electron tunnelling processes across the barrie

71 f both modes is slow compared to the rate of resonant energy exchange, the decay is accompanied by am

72 We further show that a simple Forster resonant energy transfer (FRET) network model accurately

73 emblies is responsible for phenomena such as resonant energy transfer and intermolecular charge trans

74 The resonant enhancement is observed only for the long traje

75 ucing dissipative losses and achieving large resonant enhancement of both electric and magnetic field

76 he cavity-photon lifetime, thereby promising resonant enhancement of linear and nonlinear optical eff

77 sensitivity to driving field ellipticity and resonant enhancement.

78 ed via non-gravitational thermal forces into resonant escape routes that, in turn, pushed them onto p

79 entified below a temperature of 60 K at near-resonant excitation and assigned to exciton, trion and l

80 nescence intensity from Er ions in GaN under resonant excitation excitations were performed.

81 Resonant excitation of polaritonic states and their inte

82 By employing the resonant excitation wavelengths lambdaexc = 244 nm and l

83 By combining near-impulsive resonant and non-resonant excitation, the desired fifth-order signal of a

84 y detecting their anti-Stokes emission under resonant excitation.

85 ur data revealed nearly ring-shaped magnetic resonant excitations surrounding (pi, pi) at approximate

86 oupling to nucleobases, charge-transfer, and resonant excitonic coupling between DAPIs.

87 rplay between the chiral imprint of DNA, off-resonant excitonic coupling to nucleobases, charge-trans

88 al approach is also given to capture all the resonant features of this kind of spoof-LSPs.

89 sitioning of the electrostrictive layer, and resonant fibre vibration modes tunable under AC-driving

90 ptically interacting with a cavity - such as resonant field buildup - have remained confined to narro

91 etometry and a frequency-swept ferromagnetic resonant flip-chip technique, respectively.

92 nearity in optical circuits can lead to both resonant four-wave mixing and photon blockade, which can

93 The low temperature quality factors and resonant frequencies are shown to significantly decrease

94 The magnetic properties and ferromagnetic resonant frequencies were experimentally characterized b

95 cal cavities transmit light only at discrete resonant frequencies, which are well-separated in micro-

96 ly and in simulations, that the subthreshold resonant frequency (242Hz for weak stimuli) increased co

97 PSC trains, the threshold amplitude at spike resonant frequency (317Hz) was lower than the single ESP

98 mics of zero temperature coefficients at the resonant frequency (tau f ), which can be realized throu

99 h superconducting resonator and modulate its resonant frequency at twice its value with an amplitude

100 weak stimuli) increased continuously to the resonant frequency for spiking (285Hz).

101 At the bending resonant frequency of the sensors (1.69 kHz) an output v

102 relationship between the final value of the resonant frequency shift and adsorption capacity was obs

103 res and a QCM allows optical spectra and QCM resonant frequency shifts to be recorded simultaneously

104 19% (95% CI, 4.62% to 17.76%, P = .002); and resonant frequency, 9.34% (95% CI, 3.21% to 15.47%, P =

105 e crystal boundary conditions and associated resonant frequency, which translate into phase noise mea

106 to realize wave attenuation based on locally resonant frequency.

107 two microwave parameters; quality factor and resonant frequency.

108 MPR, in these optimal models, the values of resonant- (fres) and phasonant- (fvarphi = 0) frequencie

109 the elastodynamic response and show that the resonant gaps are efficient in attenuating wave propagat

110 the method is also applicable to guided mode resonant grating and many other areas.

111 h a modulator by demonstrating the optically-resonant half of the device.

112 ation of the ultradense electron bunch under resonant helical motion in CP laser fields.

113 We demonstrate that photoconductance at resonant illumination arises due to the Coulomb interact

114 en a window resonance in argon, which is off-resonant in the field-free case, is shifted into resonan

115 road range of Zeeman energies, and appear in resonant inelastic light scattering experiments as well-

116 Resonant inelastic light-scattering spectra reveal low-l

117 The combination of X-ray absorption and 1s3p resonant inelastic X-ray scattering (Kbeta RIXS) allows

118 Here, we carry out resonant inelastic x-ray scattering (RIXS) experiments o

119 -mediated pairing for superconductivity; and resonant inelastic X-ray scattering (RIXS) provides a co

120 Here we combine X-ray absorption and resonant inelastic X-ray scattering (RIXS) spectroscopie

121 e we show the realization of high resolution resonant inelastic X-ray scattering (RIXS) with a stable

122 -PES), X-ray emission spectroscopy (XES) and resonant inelastic X-ray scattering (RIXS).

123 n microscopy, X-ray absorption spectroscopy, resonant inelastic X-ray scattering and neutron scatteri

124 Here, we implement magnetic resonant inelastic X-ray scattering at a free-electron l

125 ure and its ultrafast dynamics accessed with resonant inelastic X-ray scattering at the N 1s level us

126 n GaTa4Se8 by means of excitation spectra of resonant inelastic X-ray scattering at the Ta L3 and L2

127 2Os2O7 with neutron diffraction and then via resonant inelastic X-ray scattering determine the salien

128 Here we use resonant inelastic X-ray scattering over a wide temperat

129 Combined soft X-ray absorption spectroscopy, resonant inelastic X-ray scattering spectroscopy, X-ray

130 Here the authors use resonant inelastic X-ray scattering to demonstrate that

131 Here we use resonant inelastic X-ray scattering to follow the evolut

132 Combining resonant inelastic X-ray scattering with detailed modell

133 able of the oxygen K-edge, metal L-edge, and resonant inelastic X-ray scattering, are discussed.

134 ion reaction conditions using (57)Fe nuclear resonant inelastic X-ray scattering.

135 s, as observed from optical spectroscopy and resonant inelastic X-ray scattering.

136 edge X-ray absorption spectroscopy, and 1s2p resonant inelastic X-ray scattering.

137 n0.6]O2 with XANES, soft X-ray spectroscopy, resonant inelastic X-ray spectroscopy, and Raman spectro

138 in time by a surface-specific, vibrationally resonant, infrared-visible sum-frequency probe.

139 that are not observed in the absence of the resonant interaction of the plasmons with the excitons.

140 subthreshold oscillations (STOs) depend upon resonant interactions between neighboring neurons suppor

141 nductors in a hybrid microcavity, exploiting resonant interactions between these materials would perm

142 finding is played by the Umklapp (flip-over) resonant interactions, typical of discrete systems.

143 formation pathways by observing the multiple resonant, internal quantum transitions using ultrafast t

144 mation of the local charge anisotropy of the resonant ions, we obtained spectroscopic information fro

145 The protocol requires a single, far-off-resonant laser that is not specific to the molecule, so

146 cement in sensitivity and a narrowing of the resonant linewidths as the light incidence angle was inc

147 veal a dissipation mechanism attributable to resonant localized states in graphene encapsulated withi

148 d to rGO nanoparticles exhibit the effect of resonant LSP coupling on the emission processes.

149 x-ray magnetic circular dichroism and x-ray resonant magnetic reflectivity, which enables magnetic c

150 oism (XMCD), and specular/off-specular x-ray resonant magnetic scattering (XRMS) measurements as a fu

151 on through a microfluidic channel with 10-12 resonant mass sensors distributed along its length, weig

152 Rapid resonant mechanical scanning of the illumination beam co

153 prove upon the fundamental thermal limits of resonant mechanical sensors, which cannot be attained th

154 Surface-enhanced infrared spectroscopy using resonant metal nanoantennas, or short "resonant SEIRA",

155 Resonant metal nanostructures exhibit an optically induc

156 Resonant metamaterials have been proposed to reflect or

157 r behaves as a meta-cavity bounded between a resonant metasurface and a metallic thin-film reflector.

158 This can be used as a non-resonant metasurface that can be integrated with a Salis

159 of waves through a two-dimensional array of resonant metasurface unit-cells with electronically-cont

160 The efficiency of the resonant metawedge shows that large-scale mechanical met

161 a metasurface at the geophysical scale, the resonant metawedge, to control seismic Rayleigh waves.

162 in organic semiconductors (OSECs) induced by resonant microwave absorption in ferromagnetic substrate

163 scence measurements, as the application of a resonant microwave field can selectively modulate the in

164 ntiomers of a large gas-phase molecule using resonant microwave fields are highlighted.

165 anin suppresses multiple scattering, causing resonant Mie scattering predominant.

166 The fundamental intrinsic mechanism of resonant mode coupling is used to redistribute and store

167 ersion can be engineered to be anomalous via resonant mode coupling.

168 temperatures, the efficiency enhancement via resonant mode cross-coupling and matching can be extende

169 the thickness of the film and the plasmonic resonant mode is closely related to the gap distance of

170 ield for small skyrmions can excite skyrmion resonant modes and that a combination of different modes

171 inear optics and nanolasers, where the broad resonant modes can overlap to a significant degree.

172 The excitation of the resonant modes for certain incidence angles leads to neg

173 ear optical micro-ring resonator with high-Q resonant modes for infrared input waves.

174 ness against disorder, resulting in improved resonant modes for sensing and metrology.

175 emonstrate the excitation of dipolar and CTP resonant modes in metallic nanodimers bridged by phase-c

176 ltistable energy transfer between internally resonant modes of an electroelastic crystal plate and us

177 ment by direct coupling of incoming light to resonant modes of subwavelengthscale Mie nanoresonators

178 etamaterial system gives rise to a family of resonant modes such as the surface plasmon polariton (SP

179 ults in their ability to host two degenerate resonant modes.

180 h could be related to the generation of Fano resonant modes.

181 s examples of a potentially broader class of resonant nanophotonic thermoelectric materials for optoe

182 tonics is driven by the ability of optically resonant nanostructures to enhance near-field effects co

183 plasmon-polariton thermal emitters, that the resonant nature of the nanophotonic system significantly

184 anar metasurface-based devices caused by the resonant nature of the plasmonic structures.

185 ed devices such as transmission lines, their resonant networks, and antennas.

186 Here we report non-resonant nonlinear optical measurements at the interface

187 asurfaces consisting of randomly distributed resonant NPs.

188 nanoparticle retains its strong near-IR Fano-resonant optical absorption properties essential for pho

189 Er ions that emits photon at 1.54 mum upon a resonant optical excitation is approximately 68%.

190 Resonant optical excitation of surface plasmons produces

191 s of magnitude fewer spins and which require resonant optical excitations to spin-polarize the ensemb

192 Coupling vibrational transitions to resonant optical modes creates vibrational polaritons sh

193 complex burst-like time evolution under non-resonant optical pulsed excitation.

194 ll as polariton lasing up to 200 K under non-resonant optical pumping.

195 es (NP), which are characterized by a strong resonant optical response in the visible spectral range.

196 ancing the sensitivity (frequency shifts) of resonant optical structures to external perturbations.

197 mble period could be switched by exposure to resonant or nonresonant 24-h or 20-h lighting cycles.

198 ry cilium by using an optical trap to induce resonant oscillation of the structure.

199 Mechanical dampening of resonant oscillations due to the presence of shear force

200 ch other, generating intriguing interference-resonant patterns.

201 izes, and therefore showing distinct plasmon resonant peaks (RP), have been biofunctionalized and cod

202 s not affect the interval of any neighboring resonant peaks, but contributes a weak shift of each pea

203 ly depending on the frequency, with a lot of resonant peaks, corresponding mainly to the natural oute

204 femtosecond excited-state dynamics following resonant photoexcitation enable the selective deformatio

205 Resonant photoionization of atomic xenon was chosen as a

206 ters compared with that via the conventional resonant pi pulse method.

207 nce images, Piezo-Force Microscopy (PFM) and Resonant Piezoelectric Spectroscopy (RPS).

208 The result is an 'omni-resonant' planar micro-cavity in which light resonates c

209 In both cases, resonant plasmonic and nanophotonic structures have been

210 a suspended graphene layer to form a doubly resonant plasmonic structure.

211 We embedded resonant polar dielectric microspheres randomly in a pol

212 rt here that MSO neurons in gerbil also have resonant properties and, based on our whole-cell recordi

213 Metallic nanoparticles with strong optically resonant properties behave as nanoscale optical antennas

214 l dangling OH stretch mode is excited with a resonant pump, and its evolution followed in time by a s

215 elayed buildup of excitons under on- and off-resonant pumping conditions allows us to distinguish bet

216 are modulated with wavelength, enabling non-resonant pumping of high-quality micro-lasers and solar-

217 e-acceptor (DBA) systems by stimulated X-ray resonant Raman processes involving various transitions b

218 ed in a 15-nm-thick silica shell wherein the resonant Raman reporter is embedded.

219 f isotope ratio mass spectrometry (IRMS) and resonant Raman spectroscopy (RRS), respectively.

220 Resonant Raman spectroscopy, X-ray photo-electron-spectr

221 uned using an external laser driving a quasi-resonant Raman transition between the BEC components.

222 se two infrared absorption transitions and a resonant Raman transition to create a coherent output be

223 metamaterials could contribute to the broad resonant range for the monolithic metamaterials.

224 uggests that different electric and magnetic resonant ranges of the metamaterials could contribute to

225 sing a combination of our recently validated resonant reflection spectroscopy method combined with op

226 Due to their multipolar resonant response and low intrinsic losses they offer de

227 Conclusion Nonhemodynamic resonant saturation effects are detectable during interi

228 urpose To investigate whether nonhemodynamic resonant saturation effects can be detected in patients

229 Results Nonhemodynamic resonant saturation effects ipsilateral to the seizure o

230 Nonhemodynamic resonant saturation effects resolved in patients with fa

231 ned BiFeO3 films is determined using nuclear resonant scattering and Raman spectroscopy.

232 In non-resonant scattering condition, the cross-section is stro

233 -sub-band phonons show strong damping due to resonant scattering into an intermediate state with a pa

234 a can be explained by the combined result of resonant scattering of phononic heat carriers with magne

235 Specifically, we illustrate how the resonant scattering wavelength of single silicon nanowir

236 The cross section diverges for resonant scattering, and diminishes for non-resonant sca

237 ity differences between Friedel pairs due to resonant scattering, we demonstrate a time-resolved X-ra

238 resonant scattering, and diminishes for non-resonant scattering, when wavelength approaches infinity

239 In this Review, we introduce the concept of resonant SEIRA and discuss the underlying physics, parti

240 using resonant metal nanoantennas, or short "resonant SEIRA", overcomes this limitation.

241 g the sensitivity and broad applicability of resonant SEIRA.

242 the photothermal efficiency of near infrared resonant silica-gold nanoshells (AuNSs) and benchmarked

243 25CuO4 (LBCO) and YBa2Cu3O6.67 (YBCO), using resonant soft X-ray scattering and a model mapped to the

244 inter-spacing (about 1 nm) in BiFeO3, using resonant soft X-ray scattering techniques and soft X-ray

245 y is formed, which is fully characterized by resonant soft X-ray scattering, high-angle annular dark

246 h thermoelectric nanostructures designed for resonant spectrally selective absorption, which creates

247 wn to extend the coherence-time resulting in resonant spin amplification.

248 n's threshold, gives rise to fully coherent, resonant spin tunnelling.

249 -term stability, having been in its current, resonant state for around a million years.

250 itals are main reasons for the generation of resonant states in the GaN wells, which further results

251 lysis of our results links the energy of the resonant states to the local vertex structure of the qua

252 tron-crystal", multiscale phonon scattering, resonant states, anharmonicity, etc.

253 diabatically through weakly coupled but near-resonant states.

254 Each resonant structure consists of a cylindrical mass suspen

255 nts demonstrate that crossed trapezoidal Mie resonant structures enable angle-insensitive, broadband

256 gs), it is not possible to draw Kekule-style resonant structures for the whole molecule: any attempt

257 arrier is realized by burying sub-wavelength resonant structures under the soil surface.

258 avelengths from 10-to-100 m with meter-sized resonant structures.

259 (ultrasonic) metamaterials based on locally-resonant sub-wavelength porous rubber particles, through

260 Triply resonant sum frequency (TRSF) and doubly vibrationally e

261 w that the interaction between an engineered resonant surface and a low-power infrared laser can caus

262 vailing paradigms for linear, time-invariant resonant systems, challenging the doctrine that high-qua

263 e we overcome the diffraction limit by using resonant tip-enhanced Raman scattering (TERS) of few-lay

264 enhancement in an optimized subnanometre-gap resonant tip-substrate configuration.

265 e review recent experimental observations of resonant toroidal dipole excitations in metamaterials an

266 Resonant transmission across the p-n junction provides a

267 It has proven difficult to tune resonant transmission in disordered diamond-like carbon

268 tal and theoretical analysis which addresses resonant transmission in DLC superlattices.

269 Whilst resonant transmission is well understood and can be full

270 w type of Zener tunnelling that involves the resonant transmission of electrons through zero-dimensio

271 he mechanism of enhancing or suppressing the resonant transmission of polychromatic light and the eff

272 ed for this interference to occur allows for resonant transmission to be highly sensitive to changes

273 n efficiently block the coupling channel for resonant transmission, leading to a suppression of trans

274 suppresses the localized mode along with the resonant transmission.

275 opagation properties and the features of the resonant transmissions.

276 try applications by comparing electronically resonant TRSF and DOVE spectra with each other and with

277 ture devices--such as tunneling transistors, resonant tunneling diodes, and light-emitting diodes--ar

278 the current spikes due to radiation-induced resonant tunneling of fluctuation Cooper pairs between t

279 In this work, we propose using resonant tunnelling diodes as practical true random numb

280 They are the resonant vibrations of a bridge demonstrating simultaneo

281 Our approach is based on resonant wave-wave interaction theory; i.e., we assume t

282 Various colors can be developed as the resonant wavelength dictated by nanosphere diameter.

283 The resonant wavelength for arbitrary OAM state is demonstra

284 ed out and detected through the shift in the resonant wavelength.

285 ance of a few atoms separated by hundreds of resonant wavelengths.

286 zed surface plasmon resonances (LSPR) can be resonant with molecular vibrations.

287 We show that X-ray pulses resonant with selected core transitions can manipulate e

288 onic system, leaving the absorption strongly resonant with the antenna's enhanced EM fields.

289 is enhanced when the laser photon energy is resonant with the energy separation of the van Hove sing

290 The emission, if resonant with the plasmonic system, re-radiates to the f

291 By using linearly polarized resonant X-ray absorption spectroscopy and magnetic circ

292 and investigated its electronic structure by resonant X-ray absorption spectroscopy combined with X-r

293 the domain of x-ray standing wave methods to resonant x-ray emission spectroscopy and provides means

294 effect has a significantly larger impact on resonant x-ray emission than is observable in x-ray abso

295 Using a synchrotron-based non-resonant X-ray magnetic diffraction technique, we reveal

296 This effect, revealed by resonant X-ray photoemission, arises from interfacial hy

297 In this regard resonant x-ray reflectivity (RXR) provides a unique expe

298 Here, we employ resonant x-ray scattering in stripe-ordered superconduct

299 number of the spin texture and the polarized resonant X-ray scattering process.

300 he cuprate YBa2Cu3Oy was obtained by NMR and resonant X-ray scattering.