ライフサイエンスコーパス: resonant

1 toluminescence (PL) emission from tBLG after resonant 2-photon excitation, which tunes with the inter

2 Individual scales act as resonant (5) unit cells that are linked via a shared win

3 change in a multilayer VO(2) thin film based resonant absorber.

4 This new processing technique employed resonant acoustic mixing to coat an equiatomic NiCoCr po

5 we report a systematic study employing a 1D resonant acoustic trapping device to evaluate the cell v

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

7 Potential for resonant amplification was greatest in injured adult-siz

8 exchange qubit and a transmon qubit in both resonant and dispersive regimes, where the interaction i

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

10 ts from the temperature difference between a resonant antenna locally heated by infrared radiation an

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

12 nol contains an exchangeable hydroxyl proton resonant at 4.8 ppm from the resonance frequency of wate

13 r signal is dominated by a vibrationally non-resonant background, obscuring the Raman lineshape.

14 on pulses, suppressing the vibrationally non-resonant background.

15 ity also induces a spatially variant locally resonant band gap that progressively slow down the group

16 Consistent with previous work, a resonant behavior is observed in the resistively detecte

17 Meanwhile, resonant bonding in the PbTe-like sublattice and soft Tl

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

19 high-overtone bulk acoustic resonances(18), resonant build-up of bulk acoustic energy allows a 14-fo

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

21 ext] of molecular transitions couple to each resonant cavity mode, yielding two hybrid light-matter (

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

23 Here, we study resonant charge transport through graphene-based zinc-po

24 Off-resonant charge transport through molecular junctions ha

25 voltage across an inductor, L, of an LC tank resonant circuit to actuate the MEMS/NEMS resonator.

26 network analyzer, inductively coupled to the resonant circuit, measures the resonance frequency, agai

27 for them to subsequently be detected via the resonant circuit.

28 sleeve and connected to a coil, which form a resonant circuit.

29 These devices consist of inductively coupled resonant circuits that change their properties in respon

30 loits simple circuit descriptions of coupled resonant circuits, combined with standard radiation form

31 ic layer lithography, we create mid-infrared-resonant coaxial apertures with gap sizes as small as 1

32 We demonstrate that the vibrationally resonant coherent anti-Stokes Raman Scattering peak can

33 enhancing metamaterials typically consist of resonant components, which means that the transmitted ra

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

35 bands through Floquet engineering that under resonant conditions interacts strongly with the preexist

36 scopy using the laser wavelengths of 442 nm (resonant conditions) and 633 nm (non-resonant conditions

37 442 nm (resonant conditions) and 633 nm (non-resonant conditions).

38 ayers its effects are enhanced by interlayer resonant conditions, resulting in a superconductor-insul

39 itance method is able to cleanly resolve the resonant conductance characteristics of an electrode-con

40 he lower energy resonance peak in this multi-resonant construct is found to be highly tunable from vi

41 ted wirelessly from the transmit coil to the resonant-coupled receiver coil with an efficiency of 73%

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

43 signal amplification and generate plasmonic resonant coupling between NPs and chip surface.

44 Resonant coupling of plasmons between the gold grating a

45 satellite imagery, and the results suggest a resonant coupling with a larger-scale mode-4 internal ti

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

47 Diffraction methods, synchrotron resonant diffraction, and multiple-wavelength anomalous

48 tigative techniques that include synchrotron resonant diffraction, X-ray multiwavelength anomalous di

49 ltracold chemical reaction rates by inducing resonant dipolar interactions by means of an external el

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

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

52 We combine analytical understanding of resonant dynamics in two-planet systems with machine-lea

53 nt is attributed to the coherent polaritonic resonant effect, hence, was found to be stronger at lowe

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

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

56 Second, by performing circular dichroism in resonant elastic X-ray scattering, it is demonstrated th

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

58 dwidth is naturally narrow due to the highly resonant electro-optic modulator, it is not fundamentall

59 biaryl bond exhibited similar influences as resonant electron donors.

60 Resonant electron transfer into TPP molecules occurs at

61 ained by patterning the slab with additional resonant elements, e.g. high index dielectric spheres.

62 eement, so long as we restrict ourselves to 'resonant' encounters(10) (the roughly 50 per cent of sca

63 cleus, the cytoplasmic gel, and fluorescence resonant energy transfer (FRET) biosensors as osmometers

64 as optical probes for bioimaging and Forster resonant energy transfer (FRET) due to their high signal

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

66 oth the plasmon-induced hot electron and the resonant energy transfer processes can occur on a time s

67 rted plasmonic effects are outlined, such as resonant energy transfer, scattering, hot electron injec

68 In a high-throughput Forster resonant energy transfer-based binding assay, we found t

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

70 xcitonic bands can hybridize, resulting in a resonant enhancement of moire superlattice effects.

71 lly observe coherent interaction between the resonant exchange qubit and a transmon qubit in both res

72 The spin qubit is a resonant exchange qubit hosted in a GaAs triple quantum

73 In combination with multi-step resonant excitation to Rydberg states using pulsed laser

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

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

76 Using the resonant features, we shielded the molecules from loss a

77 by pumping an argon-filled hollow-core anti-resonant fiber at a mid-IR wavelength of 2.45 mum.

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

79 letter is to introduce the concept of a non-resonant fractional random laser.

80 in terms of their separation, difference in resonant frequencies and pumping rate under conditions o

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

82 airflow, and is influenced by the whisker's resonant frequencies.

83 lowered R(in) and produced higher electrical resonant frequencies.

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

85 Using the resonant frequency as a readout for photodetection, we a

86 t frequencies above lung corner frequency or resonant frequency despite reduced tidal volumes, especi

87 ustic waves with frequency equal to marker's resonant frequency escape this confinement; the marker b

88 ion, we also showcase comb dynamics mediated resonant frequency modulation which indirectly points to

89 yclodextrin cavity leads to the reduction of resonant frequency of the cantilevers, whereas an increa

90 By tuning the resonant frequency of the metamaterial through an applie

91 dy, avoiding large deformations close to the resonant frequency of the vibration plate and vibration

92 It is found that a linear model with the resonant frequency peaks as predictors cannot be used to

93 easurements of DC conductance and mechanical resonant frequency shifts show the expected oscillations

94 Measurements of corner frequency and resonant frequency should be considered during high-freq

95 nsional transverse modes is reflected in the resonant frequency, thereby revealing Aharonov-Bohm osci

96 rs exhibit high sensitivities (~10% shift in resonant frequency-corresponding to 50 MHz-per 150 mg/dL

97 he largest value right at the (75)As nuclear resonant frequency.

98 ded graphene resonator, thereby shifting its resonant frequency.

99 lator to dynamically track variations in the resonant frequency.

100 two microwave parameters; quality factor and resonant frequency.

101 ng frequency above lung corner frequency and resonant frequency.

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

103 e the path for integrated SiC resonators and resonant gyroscopes with Q-factors beyond the reach of S

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

105 amplitude of precession indicates efficient resonant heat transfer from the lattice to coherent magn

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

107 r carboxyfluorescein are tethered to plasmon-resonant hollow gold nanoshells (HGN) tuned to absorb li

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

109 e systems, their compatibility with magnetic resonant imaging and computed tomography and the ability

110 A molecular ferroelectric architecture with resonant inclusions then exhibits adaptive mitigation of

111 Resonant inelastic light-scattering spectra reveal low-l

112 sualize independently-occurs nonlocally upon resonant inelastic scattering from single atomic defects

113 Operando nuclear resonant inelastic X-ray scattering (NRIXS) and X-ray ab

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

115 Time-resolved resonant inelastic X-ray scattering (RIXS) is one of the

116 the feasibility of indirect K -edge bimagnon resonant inelastic X-ray scattering (RIXS) spectrum as a

117 X-ray absorption spectroscopy (XAS) and 1s2p resonant inelastic X-ray scattering (RIXS) to study oxyh

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

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

120 te, by a combination of x-ray absorption and resonant inelastic x-ray scattering spectroscopy, how th

121 g temperature-dependent X-ray absorption and resonant inelastic X-ray scattering techniques.

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

123 In addition, resonant inelastic X-ray scattering with unprecedented e

124 er, the magnetic excitation gap, measured by resonant inelastic x-ray scattering, is quite different

125 We combine three spectroscopic tools-resonant inelastic X-ray scattering, photoluminescence a

126 ich were determined previously using nuclear resonant inelastic X-ray scattering, were used to calcul

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

128 mass-spectrometry-based technique exploiting resonant infrared multiple photon dissociation (IRMPD),

129 Resonant injection and resulting charge storage were exa

130 The field of plasmonics, which studies the resonant interactions of electromagnetic waves and free

131 wever, the spatial evolution of the electron resonant interactions with electromagnetic waves remains

132 tic electrons in the plasma universe through resonant interactions with electrons.

133 nd, Earth's aurora becomes a display for the resonant interactions.

134 n a Bose-Einstein condensate (BEC) with near-resonant interactions.

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

136 c spectrum with origin at 21792 cm(-1) using resonant ionization and laser-induced fluorescence spect

137 ement of atomic parameters over previous non-resonant laser ionization methods.

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

139 d fashion with picosecond resolution using a resonant level as a detector.

140 tructural parameters play a key role such as resonant light trapping.

141 les both in the presence and absence of near-resonant light.

142 transfer function, near-field intensity and resonant line shape can all be rationally designed, prov

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

144 of skyrmion tubes in a lamella of FeGe using resonant magnetic x-ray imaging and comparative micromag

145 Here, we use a resonant magnetic X-ray scattering nanoprobe with sub-10

146 The dipole magnetic fields of the NV-resonant magnons couple to and relax nearby NV spins.

147 here the dissipated heat in a sample excites resonant magnons in a thin ferromagnetic metal layer.

148 ity despite the absence of any individual NV-resonant magnons, suggesting that multiple magnons parti

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

150 gratings, bilayer wire-grid polarizers, and resonant metal mesh long-pass filters are imprinted on C

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

152 ation of the analyte, we used an array of IR resonant metallic nanoantennas tuned to a specific IR ab

153 change with the sky can eliminate the use of resonant microstructures and noble metal mirrors in conv

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

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

156 Here we demonstrate resonant microwave-mediated coupling between two electro

157 -like system with artificial atoms acting as resonant mirrors in the otherwise open waveguide.

158 hich the monolayer pairs are nearly aligned, resonant mixing of the electron states leads to pronounc

159 ning of light scattering at the higher-order resonant mode under a low incident light intensity is de

160 ial resolution and depth response of PTIR in resonant mode while systematically varying the pulsing p

161 They can also spawn new resonant modes and quench existing ones.

162 s are reduced to subwavelength scales, their resonant modes begin to scatter light into many spatial

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

164 A sensor designed to exhibit resonant modes closely placed in frequency, enhancing th

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

166 The coupling between these resonant modes has drawn growing interest in recent year

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

168 normalization, producing strong higher-order resonant modes in single NPs with Q factors up to ~100 i

169 ight manipulations via controlling the local-resonant modes in the microstructures.

170 of the difference between the two mechanical resonant modes of the AFM cantilever.

171 according to a superposition of its two main resonant modes, rocking and bending.

172 a state flip, a sharp transition between the resonant modes.

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

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

175 Strong resonant modulation of the incident electromagnetic fiel

176 rging Raman scattering cross-sections of non-resonant molecules via chemical coupling reactions; (2)

177 in molecules is studied theoretically by off-resonant multiple X-ray diffraction events.

178 These sensors use a resonant nanoantenna to couple the IR energy to a nanosc

179 ctra, taking into account the electronically resonant nature of both.

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

181 This pulse is followed by a second non-resonant near-infrared pulse (lambda = 1064 nm) for ener

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

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

184 , hyperuniform-clad, electrically controlled resonant optical modulator suitable for fabrication in t

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

186 With a resonant optical response that can be spectrally tuned b

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

188 X-ray diffraction techniques with resonant or polarized variations of the experimental set

189 yrometer based on spatial modulation using a resonant oscillating mirror, which enables a sensitivity

190 gnal detection between cantilever mechanical resonant oscillations and the photoinduced force from th

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

192 ns for precision measurement employing other resonant-output MEMS devices such as gyroscopes and magn

193 ce intensity, together with the ground-state resonant peak of quantum dots appearing in the photolumi

194 ee-dimensional (3D) nearly-periodic, locally resonant phononic crystal (PnC).

195 a(-) and tKAN3H8b(-) yield tautomer-specific resonant photoelectron spectra.

196 formation dynamics of excitons following non-resonant photoexcitation of free electron-hole pairs hav

197 y is reported for the engineering of tunable resonant photonic media with thickness exceeding the pla

198 te general principles and a case study: a bi-resonant piezo electric harvester.

199 oupling strength helps explain both the weak resonant PL and the slower 1 ps(-1) exciton relaxation r

200 ins at room-temperature and show a five-fold resonant PL-enhancement over the background hot-electron

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

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

203 We embedded resonant polar dielectric microspheres randomly in a pol

204 a deviation from thermal equilibrium in the resonant polariton population, which we ascribe to non-M

205 laser ignition method based on a dual-pulse resonant pre-ionization scheme.

206 rm a difference in signal generation between resonant PTIR and other photothermal techniques that we

207 We excite phonons with resonant pulses and probe the resulting excitation spect

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

209 couple a silicon nitride membrane to an off resonant radio-frequency cavity formed by a lumped eleme

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

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

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

213 r and stimulate the engineering of novel non-resonant random lasers with significantly reduced footpr

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

215 The resonant removal mechanism is driven by both recoil mome

216 efficiently converted to large shifts in the resonant response of interlayer-RF sensors.

217 At the optimal frequency of 8 kHz, near the resonant response of the melt pool, the drilling efficie

218 w cavity quality factor (Q(E) ~ 7.4) and off resonant, room temperature operation, we are able to par

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

220 Wavelength-dependent diffraction and resonant scattering effects usually limit their working

221 toresistance oscillations that are caused by resonant scattering of Landau-quantised Dirac electrons

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

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

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

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

226 electromechanical system to detect light via resonant sensing.

227 Conventionally, the operation of these resonant sensors is implemented using a feedback oscilla

228 our pedestal microelectromechanical systems resonant sensors, we have developed a non-contact interf

229 hancements in optical chirality density near resonant silicon nanodisks boost CD.

230 omain sizes as evidenced by PL quenching and resonant soft X-ray scattering (R-SoXS) analyses.

231 ded X-ray absorption fine structure (EXAFS); resonant soft X-ray scattering (R-SoXS); ultraviolet pho

232 microscopic and nanoscopic properties using resonant soft X-ray scattering and a number of other exp

233 Here, using resonant soft X-ray scattering, we study the archetypal

234 on bubbles have a skyrmion number of +1, and resonant soft-X-ray diffraction experiments show circula

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

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

237 We have theoretically studied how resonant spin wave modes in an elliptical nanomagnet are

238 ies, and the power and phase profiles of the resonant spin wave modes.

239 Electronic pre-resonant SRS allows detection of sub-micromolar chromoph

240 duced pseudo-localized phonon modes-that is, resonant states resulting from the hybridization of the

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

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

243 diabatically through weakly coupled but near-resonant states.

244 Individual phonons in a resonant structure can be controlled and detected by sup

245 ce upon electronic excitation of these multi-resonant structures.

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

247 Any attempt to reduce the losses of the resonant system, and hence store a (mechanical, acoustic

248 xceeding the 'fundamental' limit of ordinary resonant systems by a factor of 30.

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

250 Most present-day resonant systems, throughout physics and engineering, ar

251 Our results open the path for designing resonant systems, ubiquitous in physics and engineering,

252 This resonant tracking approach may also have general applica

253 the Cu(111) surface involving a three-photon resonant transition from the Shockley surface band to th

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

255 g at the center wavelength of the first anti-resonant transmission window (2460 nm) with ~100 fs puls

256 opagation properties and the features of the resonant transmissions.

257 tative and quantitative understanding of the resonant transport regime has proven more elusive.

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

259 om being sharply localized so that efficient resonant tunneling across long distances becomes possibl

260 We conclude that resonant tunneling enables cost-effective ALD coatings t

261 electron field emission which is captured by resonant tunneling from the ZnO layer.

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

263 nd offsets of InAs/AlSb and a triple-barrier resonant tunnelling structure.

264 suggest a switching mechanism that relies on resonant tunnelling via the superatom molecular orbitals

265 quasi-guided photonic crystal modes known as resonant-type Wood's anomalies.

266 This paper investigates the use of resonant ultrasound measurements to predict the mechanic

267 Single-crystal X-ray diffraction and resonant ultrasound spectroscopy (RUS) revealed two dist

268 ompression testing, density measurements and resonant ultrasound spectroscopy.

269 material microstructures, between subsets of resonant unit cells forming the metasurface.

270 rds nonlinear radiation sources that combine resonant upconversion with broadband operation.

271 s coherent over time, close to the predicted resonant velocity, similar to that seen in kinetic Alfve

272 ] step is associated with a long-lived quasi-resonant vibrational coherence; and another vibrational

273 Deep, resonant vocalizations in particular may function in att

274 r accelerator can be utilized to control the resonant wavelength by adjusting the bunch sequence freq

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

276 ckbody limit by >8 times at lambda = 1.7 mum resonant wavelength in the far-field.

277 By matching the surface plasmon-resonant wavelength of the nanoparticle tag to the reson

278 nt wavelength of the nanoparticle tag to the resonant wavelength of the PC nanostructure, the reflect

279 ble transmission loss was -14.07 dB, and the resonant wavelength shift was 11.239 nm.

280 cific spatio-spectral signature, we tune the resonant wavelength within 200-300 nm by modification of

281 antennas utilizing strain-driven currents at resonant wavelengths up to five orders of magnitude smal

282 The reflected and resonant waves generated at the edges of the waveguide w

283 recipients are empowered, both in culturally resonant ways.

284 constrained to the case where the NV spin is resonant with a magnon mode in the sample meaning that t

285 polaritons to a single spatial mode that is resonant with an atomic transition.

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

287 such that the m = 1, 2, and 3 LSPR modes are resonant with the laser energy and the optically stimula

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

289 ultaneously generate spectral lines that are resonant with two chosen spatial modes of a non-degenera

290 port the onset of such a nonlinearity in the resonant X-ray absorption of magnetic Co/Pd multilayers

291 Resonant X-ray absorption, where an X-ray photon excites

292 phases, including the SkL, is determined by resonant x-ray diffraction as well as small angle neutro

293 Here we report a resonant X-ray diffraction study of ZrTe[Formula: see te

294 Using resonant X-ray reflectivity, a superlattice of SrFeO(3)

295 geometrically frustrated lattice by means of resonant X-ray scattering and Lorentz transmission elect

296 Simultaneous measurements of resonant X-ray scattering and transport reveal that this

297 In situ resonant X-ray scattering at the sulfur K-edge reveals t

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

299 Here, we report coherent resonant X-ray speckle correlation analysis, which direc

300 d scattering duration and proton dynamics in resonant X-ray-matter interaction are taken into account