ライフサイエンスコーパス: electromagnetic

1 ey enablers for such applications in applied electromagnetics.

2 flexibility in engineering the properties of electromagnetic absorption.

3 stly considered in dynamic systems involving electromagnetic, acoustic and mechanical wave propagatio

4 in air at room temperature without external electromagnetic action, by impinging a high-speed microj

5 By measuring the brain's electromagnetic activity, we show that it also generates

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

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

8 ure of these cataclysmic events by combining electromagnetic and GW observations.

9 electric field, develops a coupling between electromagnetic and lattice-wave and this coupling gover

10 fects in optomechanical systems in different electromagnetic and mechanical frequency regimes, includ

11 e metadevices with simultaneously customized electromagnetic and mechanical properties.

12 As a fundamental phenomenon in electromagnetics and optics, material absorption has bee

13 Only a few electromagnetic brain imaging studies have examined neur

14 due to their exclusive responses to not only electromagnetic, but also to acoustic and thermal waves

15 c metamaterial able to switch on and off its electromagnetic chiral response is experimentally demons

16 ein the synthesis of a novel nest structured electromagnetic composite through in-situ chemical polym

17 We establish the physical association of an electromagnetic counterpart (EM170817) with gravitationa

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

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

20 Based on the lack of an electromagnetic counterpart, upper limits of 2,060 and 4

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

22 ry mergers involving neutron stars and their electromagnetic counterparts, as well as continuous-wave

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

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

25 ith the images and redshifts observed in the electromagnetic domain.

26 Recently explored electromagnetic double zero index metamaterials consist

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

28 the exciting prospect of integrating exotic electromagnetic effects in practical photonic devices, t

29 resent a broad outline of the whole range of electromagnetic effects observed using all-dielectric me

30 An electromagnetic-elastic metamaterial able to switch on a

31 A three-dimensional unified electromagnetic-electronic model is developed in conjunc

32 rgers, however, requires the detection of an electromagnetic (EM) counterpart.

33 active moieties are localized in areas where electromagnetic (EM) fields are confined.

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

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

36 Electromagnetic (EM) waves propagating through an inhomo

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

38 ill be difficult due to the expected lack of electromagnetic emission and limited localization accura

39 Here we report models that predict the electromagnetic emission of kilonovae in detail and enab

40 sounds must be associated with some form of electromagnetic energy generated by the meteor, propagat

41 PMPs) that selectively harvest the impinging electromagnetic energy in design-defined spectral bands

42 ypical schemes employed to probe the trapped electromagnetic energy of the near-field are with consid

43 tion of plasma waves1, which can concentrate electromagnetic energy on sub-wavelength length scales.

44 The toroidal dipole is a localized electromagnetic excitation, distinct from the magnetic a

45 , these methods can fail at identifying weak electromagnetic excitations masked by stronger neighbori

46 ve end exhibited optical and radio-frequency electromagnetic features expected for negative cloud-to-

47 ombination with a low frequency (150 kHz) AC electromagnetic field (AC EMF) to effectively remove tri

48 monic nanostructures to confine the incident electromagnetic field and increase it by many orders of

49 ible without the complications of driving an electromagnetic field but rather by using spin-polarized

50 etween the magnetic dipole of a spin and the electromagnetic field can be enhanced up to the point at

51 we demonstrate that the naturally occurring electromagnetic field chirality that arises in nanobeam

52 n improved capability to efficiently use the electromagnetic field compared to other structures.

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

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

55 f the nanoparticles while also mapping local electromagnetic field enhancements and reactivity patter

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

57 The highly enhanced electromagnetic field generated by the plasmon coupling

58 f the closely attached AuNPs, and the strong electromagnetic field in the cavity of the AuNP shell or

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

60 the limit set by quantum fluctuations of the electromagnetic field instead of thermal or technical no

61 as a resonator that accumulates an intensive electromagnetic field into a spiral capacitive gap (arou

62 h 15 nm resolution as a function of time and electromagnetic field polarization for different plasmon

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

64 -dimensional (3D) optical lens structure for electromagnetic field shaping based on spatial light tra

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

66 influenced the coupling of the LSPR-enhanced electromagnetic field with FM materials.

67 Atoms interact with each other through the electromagnetic field, creating collective states that c

68 d dramatically increase the intensity of the electromagnetic field, functioning as high performance p

69 Possibly confined through its self-induced electromagnetic field, this plasmoid is shown to emit st

70 signal due to the effective coupling of the electromagnetic field.

71 nted level of confinement and enhancement of electromagnetic field.

72 coupling between the magnetic dipole and the electromagnetic field.

73 dielectric environment for manipulating the electromagnetic field.

74 Electromagnetic fields (EMF) are physical energy fields

75 Electromagnetic fields (EMFs) are present throughout the

76 led and perceived exposure to radiofrequency electromagnetic fields (RF-EMF) from mobile-phone base s

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

78 mechanism for the transfer of energy between electromagnetic fields and charged particles.

79 due to their ability to confine and enhance electromagnetic fields and strong, inherent nonlinearity

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

81 The risks of extremely-low frequency (ELF) electromagnetic fields are particularly poorly understoo

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

83 Dynamic control with pulsed electromagnetic fields can overcome energetic barriers,

84 Electromagnetic fields generated by neuronal activity in

85 ive response of positive-energy electrons to electromagnetic fields has been explored through ionizat

86 Plasmon-enhanced electromagnetic fields in an array of gold nanodots prov

87 is ultrafast charge transport and control by electromagnetic fields in semiconductors.

88 These structures allow for concentration of electromagnetic fields in the desired locations between

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

90 Nanoscale localization of electromagnetic fields near metallic nanostructures unde

91 is due to the increase in the confinement of electromagnetic fields on the location of the SLG that r

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

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

94 serious damage to instruments due to strong electromagnetic fields or arcing.

95 d by measuring the polarisation state of the electromagnetic fields produced by a microstrip waveguid

96 The forward and backward propagating electromagnetic fields produced by the waveguide, in a s

97 Electromagnetic fields produced by thermal fluctuation c

98 ydrogen-like bismuth (209)Bi(82+) experience electromagnetic fields that are a million times stronger

99 Through measurement of charged particles and electromagnetic fields with NASA's Magnetospheric Multis

100 ield-effect transistors (including realistic electromagnetic fields) to show that wavelength tunabili

101 c devices at extreme temperatures, intensive electromagnetic fields, and radiation found in space exp

102 The ability to control electromagnetic fields, heat currents, electric currents

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

104 ly inaccessible due to the large TMS-induced electromagnetic fields.

105 al mechanism through real-time processing of electromagnetic fields.

106 excitations of free charges (plasmons) with electromagnetic fields.

107 ting the phase, amplitude or polarization of electromagnetic fields.

108 citation is fully described by the Helmholtz electromagnetic force density.

109 it takes a bound electron to respond to the electromagnetic force of light sets a fundamental speed

110 ibes how electrons are bound in atoms by the electromagnetic force, mediated by the exchange of photo

111 This electromagnetic forming approach lays the groundwork for

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

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

114 eterostructures, we discuss the potential of electromagnetic hybrids--materials incorporating mixture

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

116 This should mirror in phenomena such as electromagnetic-induced transparency and harmonic genera

117 conductive and transducing its motion using electromagnetic induction, we demonstrate a miniature, d

118 rectly tune a magnetic sensor that relies on electromagnetic induction.

119 d to a Vector Network Analyzer (VNA) and the electromagnetic interaction between the samples and sens

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

121 ility and high conductivity that can provide electromagnetic interference (EMI) shielding with minima

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

123 s numerous other advantages like immunity to electromagnetic interference, fast response, low cost an

124 s additional advantages such as, immunity to electromagnetic interference, low cost, capability of on

125 rials with an ultralow density and ultrahigh electromagnetic-interference (EMI)-shielding performance

126 It has been long recognized that Electromagnetic Ion Cyclotron (EMIC) waves may play a cr

127 icles show very clear telltale signatures of electromagnetic ion cyclotron wave-induced loss.

128 the electron flux and pitch angle show that electromagnetic ion cyclotron waves provide the dominant

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

130 Electromagnetic mechanism of Joule heating and thermal c

131 Artificial electromagnetic media, or metamaterials, based on metall

132 might provide a new pathway for engineering electromagnetic metamaterials and reconfigurable optical

133 effect analogous to the optical rainbow for electromagnetic metasurfaces.

134 ing drift-diffusion transport model with the electromagnetic model which rigorously characterizes the

135 Furthermore, we adopt an electromagnetic model with the finite element method to

136 ackage, we show for the first time that such electromagnetic modeling techniques (typically applied t

137 ricated structures are assisted by numerical electromagnetic modeling, which supplies predictive simu

138 Bulk electromagnetic modes of continuum materials have Chern

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

140 and modelled the influence of the FEL mixed electromagnetic modes, also present in externally seeded

141 Advanced bronchoscopy techniques such as electromagnetic navigation (EMN) have been studied in cl

142 e diagnostic yield and complication rates of electromagnetic navigational bronchoscopic (ENB)-guided

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

144 localization of these hot carriers, akin to electromagnetic near-field maps, has been elusive.

145 mit, requires sensors that interact with the electromagnetic near-field of those features.

146 We accomplish this by enhancing the electromagnetic near-fields in the vicinity of the slits

147 octupole moments are topologically quantized electromagnetic observables.

148 with the merger of two compact objects, the electromagnetic observations provide independent constra

149 lasmas are induced from artificially created electromagnetic or electrostatic fields.

150 d by top-down fabrication, relatively larger electromagnetic passives are within the reach of printin

151 rfaces have mainly been investigated from an electromagnetic perspective, their ultrathin nature may

152 Detection relies on the electromagnetic piezoelectric acoustic sensor (EMPAS) pl

153 ctroscopy (XPS) and the ultra-high frequency electromagnetic piezoelectric acoustic sensor (EMPAS).

154 The coupling of an electromagnetic plane wave to a thin conductor depends o

155 ates has revolutionized our understanding of electromagnetic propagation and scattering.

156 re generally scattered whenever the medium's electromagnetic properties change on the scale of a sing

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

158 Conventional materials vary their electromagnetic properties in response to the frequency

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

160 ractical way to characterize the thermal and electromagnetic properties of materials and devices unde

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

162 ces driven by electric current determine key electromagnetic properties of superconductors.

163 tution of Ce not only enhances the microwave electromagnetic properties of the YIG, but also modulate

164 ere is considerable freedom to prescribe the electromagnetic properties through the judicious design

165 re artificial media that sustain transformed electromagnetic properties without persistent external s

166 Owing to their electromagnetic properties, tunability and biocompatibil

167 cing protected surface states with anomalous electromagnetic properties.

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

169 frequencies (</=20 THz) and increase of the electromagnetic pulse energy in the high-frequency range

170 This paper proposed electromagnetic pulsed thermography for fast and compreh

171 s remote possibility when intense, few-cycle electromagnetic pulses are used in a computational exper

172 ng module, which, by employing laser-excited electromagnetic pulses directed along a helical path sur

173 surement of the electric-field components of electromagnetic pulses from high-intensity laser-matter

174 Ultra-intense, narrow-bandwidth, electromagnetic pulses have become important tools for e

175 space as spatially and temporally localized electromagnetic pulses propagating at the speed of light

176 force is a universal interaction induced by electromagnetic quantum fluctuations between any types o

177 tracer using pulses of both radio-frequency electromagnetic radiation and magnetic-field gradients,

178 The emitted electromagnetic radiation can be explained with an eject

179 It describes electromagnetic radiation from a charged particle moving

180 The detection of electromagnetic radiation from the same source has shown

181 excitation and control of lattice motion by electromagnetic radiation in optical frequency range has

182 ransmission shows more advantages than other electromagnetic radiation in reacting with biological ti

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

184 bi oscillations describe the process whereby electromagnetic radiation interacts coherently with spin

185 of thermal heating from any other effect of electromagnetic radiation is completely impossible.

186 rescence, the absorption of short-wavelength electromagnetic radiation reemitted at longer wavelength

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

188 e, by measuring power consumption, timing or electromagnetic radiation).

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

190 order of magnitude larger than that seen in electromagnetic radiation, which, together with an absen

191 a new class of bright laboratory sources of electromagnetic radiation.

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

193 Different demonstrations of acoustic and electromagnetic rainbow devices have been performed, how

194 l doping and external gate voltage - and the electromagnetic resonance provided by intentionally engi

195 of deformation, resulting in a shift of its electromagnetic resonance, and in the structure transfor

196 velength is limited by designs which rely on electromagnetic resonances.

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

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

199 the conventional methods for analysis of the electromagnetic response, and provides a new route to de

200 ide large-amplitude, dynamic tuning of their electromagnetic response, which is potentially useful fo

201 olecule interactions leading to a collective electromagnetic response.

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

203 e an innovative way to tailor band-selective electromagnetic responses at the surface of a heavy ferm

204 ngineered structures can produce astonishing electromagnetic responses because of their constituents

205 Low-loss electromagnetic responses covering all four quadrants of

206 equires a comprehensive investigation of the electromagnetic responses of novel materials at subwavel

207 th dimensions for successful modification of electromagnetic responses point by point, with merits of

208 We applied Dynamic Causal Modeling of evoked electromagnetic responses recorded by EEG and MEG to an

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

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

211 d limit on the dynamic control of matter and electromagnetic signal processing.

212 heavy radioactive isotopes that can power an electromagnetic signal.

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

214 The electromagnetic signatures show that they are of negativ

215 The optimal device is studied with full-wave electromagnetic simulations to compare its behavior unde

216 eguides as well as seamless integration with electromagnetic solvers for optomechanical device design

217 tions indicates they might not be useful for electromagnetic sounding of the atmosphere from a high a

218 It was accompanied by radiation across the electromagnetic spectrum and localized to the galaxy NGC

219 mitted color across the visible range of the electromagnetic spectrum and switchable polarization pro

220 its band gap is in the visible range of the electromagnetic spectrum and the ionic type of bonding i

221 ng scenarios, including broad regions of the electromagnetic spectrum and through scattering media.

222 and shortwave infrared (SWIR) regions of the electromagnetic spectrum are essential for optical imagi

223 In order to realize the terahertz (THz) electromagnetic spectrum as a fully-functional bandwidth

224 its extension to the terahertz regime of the electromagnetic spectrum, where a rich variety of materi

225 -performance paradigm for imaging across the electromagnetic spectrum.

226 n rates has been found by studies across the electromagnetic spectrum.

227 erglow radiation that is detected across the electromagnetic spectrum.

228 extreme ultraviolet and soft x-ray region of electromagnetic spectrum.

229 visible into the near-infrared region of the electromagnetic spectrum.

230 iolet and extreme-ultraviolet regions of the electromagnetic spectrum.

231 We present a formulation of electromagnetic spin-orbit coupling in magneto-optic med

232 It shows that magnetization-induced electromagnetic spin-orbit coupling is possible, and tha

233 erbolic metamaterial domains, which from the electromagnetic standpoint behave as individual "Minkows

234 Remarkably, electromagnetic stimulation leads to a specific activati

235 Electromagnetic stimulation techniques such as transcran

236 Effects of multiple-day electromagnetic stimulation were assessed using an objec

237 the application of intense fields, impulsive electromagnetic stimulation, and nanostructuring or inte

238 Recent theoretical work indicates that electromagnetic structures collectively known as photoni

239 ics of Weyl points has also been explored in electromagnetic structures such as photonic crystals and

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

241 step towards realizing the deeper insight in electromagnetic thermography (EMT) and automatic defect

242 n eigenmode solvers ubiquitously employed in electromagnetics to find waveguide modes, and enables de

243 ERPs), and standardized low-resolution brain electromagnetic tomography (sLORETA).

244 adults with MDD, using Low-Resolution Brain Electromagnetic Tomography.

245 s and physical modelling of a rapidly fading electromagnetic transient in the galaxy NGC 4993, which

246 Quantum fluctuations of the electromagnetic vacuum produce measurable physical effec

247 roperty to be transparent or absorbing of an electromagnetic wave based on tunable electronic propert

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

249 Penetration depth of electromagnetic wave into samples decreased with increas

250 tials for real-time, fast, and sophisticated electromagnetic wave manipulation such as dynamic hologr

251 Dynamic control of electromagnetic wave propagation direction through this

252 d characterized for suppressing the specular electromagnetic wave reflection or backward radar cross

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

254 ls and may lead to potential applications in electromagnetic wave related metrology.

255 State-of-the-art compact antennas rely on electromagnetic wave resonance, which leads to antenna s

256 s are supported by numerical as well as full electromagnetic wave simulations.

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

258 y an interaction between the material and an electromagnetic wave, and visualizes the heat source dis

259 mensions than the wavelength of the incident electromagnetic wave, hence behaving as artificial mater

260 e acoustic resonance of the antenna with the electromagnetic wave, reducing the antenna footprint by

261 olecular interactions can be captured by THz electromagnetic wave.

262 to antenna sizes that are comparable to the electromagnetic wavelength.

263 resulting in the unidirectional behavior of electromagnetic waves (directional emitter) without any

264 ine based on topologically protected surface electromagnetic waves (TPSWs) between two PTIs which are

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

266 Electromagnetic waves are known to exert optical forces

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

268 ally the topologically robust propagation of electromagnetic waves around sharp corners without backs

269 ction), which originates from retardation of electromagnetic waves at the distances comparable to a w

270 l realization of a topological insulator for electromagnetic waves based on engineered bianisotropic

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

272 Electromagnetic waves carrying orbital angular momentum

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

274 pens new degrees of freedom for manipulating electromagnetic waves in air.

275 figurable metasurfaces capable of deflecting electromagnetic waves in an electronically controllable

276 The sub-luminal phase velocity of electromagnetic waves in free space is generally unobtai

277 ual dispersion and attenuation of transverse electromagnetic waves in the few-THz regime on nanoscale

278 ating the spectral and spatial properties of electromagnetic waves in unconventional ways.

279 It was hypothesized previously that electromagnetic waves inside left-handed metamaterials p

280 (R), absorption (A), and transmission (T) of electromagnetic waves is a key objective in quantum opti

281 ntly manipulating the polarization states of electromagnetic waves is of great importance for communi

282 for achieving spin-selective transmission of electromagnetic waves is proposed.

283 have made the exotic control of the flow of electromagnetic waves possible, which is difficult to ac

284 at a normal angle only, although in reality electromagnetic waves scatter from various structures or

285 These ME antennas receive and transmit electromagnetic waves through the ME effect at their aco

286 tonics, where spin waves are used instead of electromagnetic waves to transmit and process informatio

287 Such media support propagating electromagnetic waves with extremely large wave vectors

288 an absorptive or emissive semiconductor for electromagnetic waves with orthogonal linear polarizatio

289 originate from strong resonances of incident electromagnetic waves with plasmonic and excitonic state

290 These results are described for electromagnetic waves, but are directly relevant to othe

291 these antennas sense the magnetic fields of electromagnetic waves, giving a piezoelectric voltage ou

292 ulation and switching of broadband terahertz electromagnetic waves.

293 m systems in analogy to cloaking devices for electromagnetic waves.

294 transmission, absorption, and scattering of electromagnetic waves.

295 s an additional degree of freedom to control electromagnetic waves.

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

297 a handpiece that emitted infrared light and electromagnetic waves.

298 thin film, which results in the radiation of electromagnetic waves.

299 e potential for application in absorption of electromagnetic waves.

300 ing the bidirectional polarization states of electromagnetic waves.