ライフサイエンスコーパス: electromagnetic

1 l components that require high stiffness and electromagnetic absorption; heat sinks for central proce

2 m that can propagate coherent waves, such as electromagnetic, acoustic, plasmonic, mechanical, or qua

3 a novel needle steering method empowered by electromagnetic actuation that overcomes all of the afor

4 We introduce the optical ruler, an electromagnetic analog of a physical ruler, for nanoscal

5 nd selective spatial frequency separation of electromagnetic and acoustic waves using graded metasurf

6 bow trapping effect has been demonstrated in electromagnetic and acoustic waves.

7 deriving accurate formulas for the effective electromagnetic and elastodynamic properties that depend

8 Landau levels in curved space-through local electromagnetic and gravitational responses of the bulk

9 ere the strength of the coupling between the electromagnetic and mechanical modes is controlled by th

10 In applications to electromagnetic and photonic metamaterials, some success

11 s enabled the creation of robust electronic, electromagnetic, and mechanical transport properties acr

12 Tongue postures were measured using electromagnetic articulography.

13 sented different types of meta-materials and electromagnetic bandgap (EBG) structures to improve the

14 pfions are of fundamental importance for the electromagnetic behavior of the nanocomposits and can re

15 The macroscopic electromagnetic boundary conditions, which have been est

16 l sensing framework based on the concepts of electromagnetic canyons and non-resonance amplification,

17 cs, optical holography, compressive imaging, electromagnetic communication, and so on.

18 e of the densest clusters with no detectable electromagnetic counterpart suggests that the black hole

19 r merger GW170817 remains the only confirmed electromagnetic counterpart to a gravitational-wave even

20 The discovery of an electromagnetic counterpart to the gravitational-wave so

21 e gravitational-wave event GW170817 with its electromagnetic counterparts AT2017gfo and GRB170817A, a

22 uble compact binaries, especially those with electromagnetic counterparts providing redshifts.

23 been designed in this field, emulating their electromagnetic counterparts.

24 effect mainly arises from distance-dependent electromagnetic coupling between neighboring coated fibe

25 linear polarization converter exhibit strong electromagnetic coupling, which increases the number of

26 ency (RF) electronics, which combine passive electromagnetic devices and active transistors to genera

27 ace disinfection, water purification, active electromagnetic devices based on artificial microplasma

28 etic convection, residual magnetization, and electromagnetic drift.

29 e a concept of valley photonic crystals with electromagnetic duality symmetry but broken inversion sy

30 thermal effect, ultraviolet irradiation, and electromagnetic effect have been regarded as ignorable f

31 ons are predominantly mediated by collective electromagnetic effects of the resulting currents and ch

32 onic antenna is enhanced due to strong local electromagnetic (EM) fields.

33 The lens system based on electromagnetic (EM) quadrupoles has been built as a par

34 Nowadays, intense electromagnetic (EM) radiation in the far-infrared (FIR)

35 To prevent the electromagnetic (EM) wakefields excitation, protect dete

36 Polarization is an important property of electromagnetic (EM) wave and different polarization man

37 , and strongly interact with light and other electromagnetic (EM) waves.

38 proposed for ultra-wideband manipulation of electromagnetic (EM) waves.

39 Observations of the late-time electromagnetic emission, however, do not agree with the

40 Chorus waves, among the most intense electromagnetic emissions in the Earth's magnetosphere,

41 la: see text]tenth of a micron) gaps of zero electromagnetic energy density in the modulated reflecte

42 or traveling mode, changed the conversion of electromagnetic energy into heat when 2.45 GHz microwave

43 The antennas are excited by coupling electromagnetic energy through the gaps of the concentri

44 ite the array via slot-lines that couple the electromagnetic energy to the patches.

45 ves to create perfect absorption of incident electromagnetic energy using relatively simple elemental

46 y, how it will transmit, reflect, and absorb electromagnetic energy.

47 We demonstrate that modifying the electromagnetic environment around the ion can increase

48 Increasingly, the local electromagnetic environment used by electro- and magneto

49 of an atom, but is instead dependent on the electromagnetic environment(1) and, in the case of ensem

50 verall peripheral techniques (electrical and electromagnetic) (ES = - 0.58, 95% CI = - 1.23 to 0.07).

51 the two platforms generates locally enhanced electromagnetic field 'hot spot', formed at the junction

52 er and the electro-sensitive Little skate to electromagnetic field (EMF) emissions of a subsea high v

53 While increasing frequency of electromagnetic field (EMF) exposure (up to <10 kHz) of

54 the transfer of energy between the turbulent electromagnetic field and electrons in the Earth's magne

55 iving a topological magnon insulator with an electromagnetic field and show that this causes edge mod

56 ht, its electrons can absorb energy from the electromagnetic field by rapidly rearranging their posit

57 rdles in plasmonics is the trade-off between electromagnetic field confinement and the coupling effic

58 Strong interactions, better electromagnetic field confinements, and less leakage int

59 bling tailoring of the damping processes and electromagnetic field couplings of the Fano resonances,

60 able to the decay length of the LSPR-induced electromagnetic field enhancement ( approximately 5-20 n

61 the conservative energy exchange between the electromagnetic field fluctuations and the charged parti

62 The highly enhanced electromagnetic field generated by the plasmon coupling

63 by modifying the vacuum fluctuations of the electromagnetic field in a cavity.

64 We proved the high confinement of the electromagnetic field in the holes both by theoretical m

65 eflection band due to evanescent coupling of electromagnetic field in the slab and the buffer layer.

66 The optical ruler is a complex electromagnetic field in which singularities serve as th

67 on path for applications where tailoring the electromagnetic field induced by Fano resonance can impr

68 neous yet powerful volumetric confinement of electromagnetic field inside an open-access nanotip.

69 he finite zero point energy of the quantized electromagnetic field inside an optical cavity.

70 gular grooves which effectively confines the electromagnetic field into a slow travelling wave.

71 Strong resonant modulation of the incident electromagnetic field is achieved thanks to the exceptio

72 surface design parameters based on a desired electromagnetic field outcome.

73 frames per second) video images and wideband electromagnetic field records of the attachment process

74 model consists of an accurate body model for electromagnetic field simulations, an atlas of periphera

75 We calculate the electromagnetic field tensor for general three dimension

76 We then compare the electromagnetic field tensors obtained by a direct boost

77 ticles resulting from strong coupling of the electromagnetic field with the lattice vibrations of pol

78 Each natural mode of the electromagnetic field within a parabolic mirror exhibits

79 tightly-confined and exponentially-decaying electromagnetic field.

80 tion is generated as a complex-valued output electromagnetic field.

81 dielectric environment for manipulating the electromagnetic field.

82 programmable frequency and force level in an electromagnetic field.

83 ng qubits(5), high-resolution and high-speed electromagnetic-field sensing(8) and high-accuracy curre

84 Exposure to electromagnetic fields (EMF) has been associated with th

85 and tissue cultures generated using induced electromagnetic fields (EMFs) in an air-core solenoid co

86 Brief exposure to low mT-range pulsing electromagnetic fields (PEMFs) was previously shown to a

87 Radio-frequency electromagnetic fields (RF-EMFs) can be absorbed in all

88 nteractions between electronic states, local electromagnetic fields (tip-induced plasmons), and molec

89 ctrons at low [Formula: see text] Spectra of electromagnetic fields and the ion distribution function

90 the amplitude, phase and polarization of the electromagnetic fields are accrued gradually along an op

91 Biological electromagnetic fields arise throughout all tissue depth

92 We find strong focusing of the electromagnetic fields at the contact edges over the sam

93 ns, (macro)molecules, hydrodynamic flows, or electromagnetic fields can be directly observed under th

94 , has predicted that quantum fluctuations of electromagnetic fields could induce phonon coupling acro

95 Electromagnetic fields generated by neuronal activity in

96 Most studies of current responses to electromagnetic fields have focused on optical intensity

97 e samples to an intense interaction with the electromagnetic fields highly concentrated around the se

98 Depending on the applied strength, electromagnetic fields in electronic materials can induc

99 the calculation of physical quantities like electromagnetic fields in the relativistic regime.

100 Little is known about how electromagnetic fields interact with this layer, particu

101 ility that weak, low-frequency anthropogenic electromagnetic fields may have biological consequences.

102 ions of electrons (plasmons), providing huge electromagnetic fields on the nanometer scale.

103 chnique to produce and then image evanescent electromagnetic fields on the surfaces of nanostructures

104 Detecting weak radio-frequency electromagnetic fields plays a crucial role in a wide ra

105 Electromagnetic fields produced by thermal fluctuation c

106 How living systems respond to weak electromagnetic fields represents one of the major unsol

107 thod captures atomic-scale variations of the electromagnetic fields while efficiently handling extrem

108 /2 particles undergoing Larmor precession in electromagnetic fields with small field non-uniformities

109 The interaction of static to high frequency electromagnetic fields with the cell constituents induce

110 obtaining strong coupling between motion and electromagnetic fields without adding additional decoher

111 uantum particles(1-11) and their coupling to electromagnetic fields(12-18).

112 Electrical stimulation (pulsed electromagnetic fields, direct current, and capacitive c

113 imodal nature of the interaction between the electromagnetic fields, such as phase noises and spontan

114 coherently manipulated by means of external electromagnetic fields.

115 lving integral equations using monochromatic electromagnetic fields.

116 is correlated with this rapid heating under electromagnetic fields.

117 oupled by interactions mediated by scattered electromagnetic fields.

118 ional hydraulic power generation mainly uses electromagnetic generators that are heavy, bulky, and be

119 Inspired by the historical development of electromagnetic generators, here, we propose and realize

120 Atlantic margin using new shallow water electromagnetic geophysical methods.

121 able to travelling waves of any nature (e.g. electromagnetic, gravitational or acoustic), BISER provi

122 trate that the formation of plasma is due to electromagnetic hotspots arising from the cooperative in

123 lor their plasmonic properties and intrinsic electromagnetic "hotspots".

124 provides general guidelines for engineering electromagnetic illusions but can be extended to shape t

125 Intense electromagnetic impulses induced by Jupiter's lightning

126 easurements of vineyard soils obtained by an electromagnetic induction (EMI) technique.

127 During BI-KPro surgery, an electromagnetic induction sensor ring enabling telemetri

128 dicts that animals detect magnetic fields by electromagnetic induction within the semicircular canals

129 opose that pigeons detect magnetic fields by electromagnetic induction within the semicircular canals

130 ovides a means of studying them by combining electromagnetic interaction with detection techniques th

131 Through direct programming of a continuous electromagnetic interface at deep subwavelength scales,

132 e critical for flexible electronics, such as electromagnetic interference (EMI) shielding coatings an

133 Lightweight, ultrathin, and flexible electromagnetic interference (EMI) shielding materials a

134 as mechanically flexible, easily processable electromagnetic interference (EMI) shielding materials.

135 Miniaturization of electronics demands electromagnetic interference (EMI) shielding of nanoscal

136 merous applications, such as energy storage, electromagnetic interference shielding, and catalysis.

137 demonstrated state-of-the-art performance in electromagnetic interference shielding, chemical sensing

138 h the tested devices, thus showing a lack of electromagnetic interference with data transmission in t

139 for thermal anchoring, and is also immune to electromagnetic interference, which allows routing of se

140 d presented by the axial theta E . B term in electromagnetic Lagrangian (E and B are the electric and

141 pectrum can be strongly modified through the electromagnetic local density of states (EM LDOS) in nan

142 will allow multimode entanglement involving electromagnetic, mechanical, and spin degrees of freedom

143 zation insensitive, wide-angle and broadband electromagnetic metamaterial absorber, which can cover e

144 ement forming the artificial structure of an electromagnetic metamaterial defines the way the metamat

145 pling, which is analogous to bianisotropy in electromagnetic metamaterials.

146 generated light has a high-order transverse electromagnetic mode structure in both the first and sec

147 Using a suite of electromagnetic modeling tools (Mie theory, T-matrix, su

148 oustic graphene plasmons are highly confined electromagnetic modes carrying large momentum and low lo

149 A laser is based on the electromagnetic modes of its resonator, which provides t

150 jects when compared to the wavelength of the electromagnetic modes with which they interact.

151 ly built from rigid, metallic components and electromagnetic motors, which make them heavy, expensive

152 The electromagnetic near field enables subwavelength applica

153 Far-field spectroscopy and mapping of electromagnetic near-field distribution are the two domi

154 ir energy to NaCl lattice vibrations via the electromagnetic near-field.

155 d the properties of black holes, and in 2017 electromagnetic observations of a double neutron star me

156 While many investigations have focused on electromagnetic, optical, and transport behaviors, nanos

157 d is generally applicable to tomography with electromagnetic or other types of radiation at all bands

158 Electromagnetic or ultrasound waves suffer from absorpti

159 In the past two decades, high-amplitude electromagnetic outbursts have been detected from dorman

160 Electromagnetic performance of the lens antenna was expe

161 new degrees of freedom and achieve enhanced electromagnetic performance.

162 evant length scales above about 1 nanometre) electromagnetic phenomena.

163 n several technological fields, ranging from electromagnetic pollution to integrated multi-physical r

164 d Bohm showed that electrons are affected by electromagnetic potentials in the absence of forces due

165 with strong self-biased behaviors have good electromagnetic properties in millimeter-wave range.

166 chieve simultaneous control over the various electromagnetic properties of dielectric waveguides, inc

167 ir distribution, are directly coupled to the electromagnetic properties of oxides and related emergen

168 We measure the electromagnetic properties of suspended DNA tweezer solu

169 detect extremely delicate variations in the electromagnetic properties that characterize the varying

170 rotated to each other to bestow the desired electromagnetic properties.

171 r cross section of an object is an important electromagnetic property that is often measured in anech

172 , based on coherent perfect absorption (CPA) electromagnetic protocols, by utilizing a network of cou

173 y germanium detectors is given by the strong electromagnetic pulse caused by the laser-matter interac

174 that were accompanied by quasi-simultaneous electromagnetic pulses (EMPs) detected by the GLD360 and

175 ns, with intensities much higher than common ElectroMagnetic Pulses (EMPs) generated by the same expe

176 Here we show that terahertz electromagnetic pulses allow coherent steering of spins

177 Here we report the discovery of electromagnetic pulses associated with Jovian lightning.

178 n models that describe synchrotron masers or electromagnetic pulses powered by magnetar bursts and gi

179 Biofluorescence is the absorption of electromagnetic radiation (light) at one wavelength foll

180 ger event GW170817 was detected through both electromagnetic radiation and gravitational waves.

181 simulations that show they spin up and emit electromagnetic radiation at ~ 10(4) to ~ 10(9) Hz after

182 The low propagation loss of electromagnetic radiation below 1 MHz offers significant

183 The emitted electromagnetic radiation can be explained with an eject

184 It describes electromagnetic radiation from a charged particle moving

185 Electromagnetic radiation from Wi-Fi systems operating a

186 that achieves wireless energy harvesting of electromagnetic radiation in the Wi-Fi band with zero ex

187 mospheric air is still highly transparent to electromagnetic radiation in this spectral region, makin

188 applications for detection of the echoes of electromagnetic radiation in turbid media.

189 In this study, we investigated the effect of electromagnetic radiation produced by a number of everyd

190 aterial enabled sensors, polymer fillers for electromagnetic radiation shields, and catalysts for var

191 Reversed Cherenkov radiation is the exotic electromagnetic radiation that is emitted in the opposit

192 to a magnetic field, they resonantly absorb electromagnetic radiation via electronic transitions bet

193 , powered chemically and/or by the energy of electromagnetic radiation, can give rise to the emergent

194 heir plasmonic responses, upon coupling with electromagnetic radiation, to research areas such as sen

195 he surface reflection and bulk absorption of electromagnetic radiation.

196 e use of natural oscillation sources such as electromagnetic radiation.

197 has anisotropic interactions with impingent electromagnetic radiation.

198 These arrays of electromagnetic resonators (or meta-atoms) carrying shor

199 Dual-mode electromagnetic resonators are used in numerous systems

200 Shape symmetry in dual-mode planar electromagnetic resonators results in their ability to h

201 using origami patterns with strongly coupled electromagnetic resonators, we transform a single-band F

202 ols for analysis and characterization of the electromagnetic response in nanophotonics.

203 The metamaterial electromagnetic response is controlled via a low-frequen

204 Unique electromagnetic response of Weyl semimetals such as chir

205 dy reports origami-based metamaterials whose electromagnetic responses are dynamically controllable v

206 ic states leads to robust surface states and electromagnetic responses.

207 at non-zero frequencies, lead to new laws of electromagnetic scattering that allow cross sections to

208 ross a thickness less than the skin depth of electromagnetic screening.

209 Here we integrate controlled-source electromagnetic, seismic reflection and borehole data wi

210 heavy radioactive isotopes that can power an electromagnetic signal.

211 femtometre scale and the ability to convert electromagnetic signals at the single photon level.

212 essengers, including gravitational waves and electromagnetic signals, can be used to study the behavi

213 ated in ways that are impossible with purely electromagnetic signals, due to the 10(5) times slower m

214 The largest difference in electromagnetic signature was observed between NN F1 and

215 and supported with a quasi-static full-wave electromagnetic simulation model.

216 the spatial evolution of the vortex fields; electromagnetic simulations and analytic theory confirm

217 typically results in the designer performing electromagnetic simulations of a large number of correla

218 Full-wave electromagnetic simulations of light absorption indicate

219 Two-dimensional finite-element method electromagnetic simulations of the composite nanostructu

220 investigate the possibility of accelerating electromagnetic simulations using the data collected fro

221 Electromagnetic simulations were performed using 4- and

222 experimental nanoscale surface analysis, and electromagnetic simulations, we perform a comprehensive

223 the visible and infrared (IR) regions of the electromagnetic spectrum are desirable for applications

224 his powerful tool for coherently uniting the electromagnetic spectrum developed.

225 The terahertz region of the electromagnetic spectrum has been the least utilized owi

226 essing the near-infrared (NIR) region of the electromagnetic spectrum is exceedingly important for ph

227 optical waveguides over a broad range of the electromagnetic spectrum ranging from Terahertz to visib

228 ant mid-infrared and terahertz region of the electromagnetic spectrum(1,2).

229 rtz radiation encompasses a wide band of the electromagnetic spectrum, spanning from microwaves to in

230 or the visible and invisible segments of the electromagnetic spectrum.

231 ge from the UV to the infrared region of the electromagnetic spectrum.

232 kes place in the visible (green) part of the electromagnetic spectrum.

233 peptides and where they can be found in the electromagnetic spectrum.

234 -performance paradigm for imaging across the electromagnetic spectrum.

235 erglow radiation that is detected across the electromagnetic spectrum.

236 on bands reach into the NIR-II region of the electromagnetic spectrum.

237 e tuned within the visible and near-infrared electromagnetic spectrum.

238 es have been implemented to realize squeezed electromagnetic states, including microwave fields and o

239 wireless activation of enzyme function using electromagnetic stimuli.

240 the proposed FSS is a dynamic reconfigurable electromagnetic structure whereas traditional FSSs are s

241 Electromagnetic surface waves guided by the planar inter

242 Surface plasmon polaritons are electromagnetic surface waves, which, due to their nanos

243 we show for the first time that an airborne electromagnetic survey provides a 3D global resistivity

244 0.84, 95% CI = - 1.57 to - 0.11) compared to electromagnetic techniques (ES = 0.21; 95% CI = - 1.00 t

245 measured with non-destructive ultrasonic or electromagnetic techniques, on the basis that corrosion

246 -consistent multi-physics simulations of the electromagnetic, thermal and IV characteristics of the d

247 nerve, and standardized low-resolution brain electromagnetic tomography (sLORETA) was used to image t

248 Exact low-resolution electromagnetic tomography was used to compute activity

249 compared, and conditions of full and partial electromagnetic transparency are discussed.

250 L interaction, and the other half acts as an electromagnetic undulator to generate up to 13 keV X-ray

251 Quantum fluctuations of the electromagnetic vacuum produce measurable physical effec

252 ons, long-range wireless power transfer, and electromagnetic warfare.

253 device's response increases with increasing electromagnetic wave amplitude and exhibits prominent br

254 y to determine the magnitude and phase of an electromagnetic wave at every point in space, as well as

255 posite media that link effective elastic and electromagnetic wave characteristics to one another, inc

256 e camera can capture quantitatively accurate electromagnetic wave distribution in the diffraction lim

257 e coupling between the Weyl fermions and the electromagnetic wave for further study of novel light-ma

258 Penetration depth of electromagnetic wave into samples decreased with increas

259 In order to determine how an electromagnetic wave propagates from a base station to a

260 ery, 123 nonradioactive, infrared-activated, electromagnetic wave reflectors were percutaneously inse

261 eries, supercapacitors, compression devices, electromagnetic wave shielding and sensors.

262 , non-local voltage generation and anomalous electromagnetic wave transmission.

263 ally to distribute and route the propagating electromagnetic wave, allowing for simultaneous transmis

264 opposite propagation directions of the same electromagnetic wave.

265 to the power and the momentum carried by an electromagnetic wave.

266 olecular interactions can be captured by THz electromagnetic wave.

267 for two different directions of the incident electromagnetic wave.

268 , which studies the resonant interactions of electromagnetic waves and free electrons in solid-state

269 on are insensitive to the incident angles of electromagnetic waves and permittivity of dielectric sub

270 s the length scale of the cross section when electromagnetic waves are scattered by an electrically s

271 etasurfaces enable a new paradigm to control electromagnetic waves by manipulating subwavelength arti

272 measure the subsequent coherent emission of electromagnetic waves by water molecules.

273 significant interaction cross-sections with electromagnetic waves due to their large surface area-to

274 A metal is a material highly reflective to electromagnetic waves for frequencies up to the optical

275 ly occurring chorus emissions are a class of electromagnetic waves found in the space environments of

276 ption, allowing detection of a wide range of electromagnetic waves from ultraviolet and visible, to t

277 impact in optics due to its interaction with electromagnetic waves gave rise to a multitude of effect

278 Hamiltonians derived for the propagation of electromagnetic waves in dedicated spatial structures.

279 ributed to an anomalously high absorption of electromagnetic waves in its layered, metamaterial-like

280 n of the electron resonant interactions with electromagnetic waves remains poorly understood owing to

281 nents is modeled using scalar diffraction of electromagnetic waves through a pixelated multi-level 3D

282 inear oscillators and the propagation of the electromagnetic waves through non-linear Bloch waves of

283 als have been discovered that can manipulate electromagnetic waves to create perfect absorption of in

284 Transmission spectra show electromagnetic waves traverse the composite medium from

285 fundamental mechanisms behind interaction of electromagnetic waves with 2D materials.

286 ntenna devices has been achieved by applying electromagnetic waves with different frequencies and amp

287 ve been demonstrated for electronic systems, electromagnetic waves(1-5), cold atoms(6,7), acoustics(8

288 ayer assembled film offers ~20% shielding of electromagnetic waves, a 24-layer film of ~55 nm thickne

289 the way the metamaterial will interact with electromagnetic waves, and accordingly, how it will tran

290 With the purpose to transform electromagnetic waves, we morph the shapes of FSS design

291 ot heat under RF fields due to reflection of electromagnetic waves, whereas composites with low condu

292 ivity to externally alternating current (AC) electromagnetic waves, which is attributed to the vortex

293 egative-index materials) can support surface electromagnetic waves, which now play crucial roles in p

294 In contrast, a dielectric is transparent to electromagnetic waves.

295 as intensity and polarization modulators for electromagnetic waves.

296 transmission, absorption, and scattering of electromagnetic waves.

297 lar resonances, at normal incidence of plane electromagnetic waves.

298 a handpiece that emitted infrared light and electromagnetic waves.

299 t periodic arrays can change the behavior of electromagnetic waves.

300 s (FSSs) have been used to control and shape electromagnetic waves.