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1 driven by the electric field of the incident electromagnetic wave.
2 , space-variant phase changes on an incident electromagnetic wave.
3 metamaterials upon which is incident a plane electromagnetic wave.
4  opposite propagation directions of the same electromagnetic wave.
5  to the power and the momentum carried by an electromagnetic wave.
6 olecular interactions can be captured by THz electromagnetic wave.
7 for two different directions of the incident electromagnetic wave.
8 tance for controlling their interaction with electromagnetic waves.
9 ity with pure rotation of linearly polarized electromagnetic waves.
10  7-50 nm were used as absorber materials for electromagnetic waves.
11 s (FSSs) have been used to control and shape electromagnetic waves.
12 h as tunability, switching and modulation of electromagnetic waves.
13 ct that it can achieve unity absorptivity of electromagnetic waves.
14 fficient devices to manipulate the terahertz electromagnetic waves.
15 by enabling precise control over the flow of electromagnetic waves.
16 st because of their unusual interaction with electromagnetic waves.
17  more energy efficient than communicating by electromagnetic waves.
18 ination of the data channels available using electromagnetic waves.
19 s cavity may be unstable to superradiance of electromagnetic waves.
20  In contrast, a dielectric is transparent to electromagnetic waves.
21 rong and tunable interaction with free-space electromagnetic waves.
22 ield-driven electron tunneling under intense electromagnetic waves.
23 the generation, manipulation, and storage of electromagnetic waves.
24 their ability to precisely control and steer electromagnetic waves.
25 omplex interference of fluidic, acoustic, or electromagnetic waves.
26 ndgaps shared by both surface and free-space electromagnetic waves.
27 alog complex mathematical computations using electromagnetic waves.
28 as intensity and polarization modulators for electromagnetic waves.
29  transmission, absorption, and scattering of electromagnetic waves.
30 lar resonances, at normal incidence of plane electromagnetic waves.
31  a handpiece that emitted infrared light and electromagnetic waves.
32 thin film, which results in the radiation of electromagnetic waves.
33 e potential for application in absorption of electromagnetic waves.
34 ing the bidirectional polarization states of electromagnetic waves.
35 ulation and switching of broadband terahertz electromagnetic waves.
36 m systems in analogy to cloaking devices for electromagnetic waves.
37 t periodic arrays can change the behavior of electromagnetic waves.
38 s an additional degree of freedom to control electromagnetic waves.
39  emission, propagation and scattering of the electromagnetic waves.
40 ve been demonstrated for electronic systems, electromagnetic waves(1-5), cold atoms(6,7), acoustics(8
41 ayer assembled film offers ~20% shielding of electromagnetic waves, a 24-layer film of ~55 nm thickne
42                                          The electromagnetic wave absorbing composite films were prep
43  The experimental results indicated that the electromagnetic wave absorbing properties of ACNTs are s
44  microscope and X-ray diffraction, and their electromagnetic wave absorbing properties were measured
45  electron gases, collectively accelerated by electromagnetic waves according to Newton's second law o
46 the ability of LN to generate and manipulate electromagnetic waves across a broad spectrum, from micr
47 found evidence for global contributions from electromagnetic waves (Alfven waves).
48 ally to distribute and route the propagating electromagnetic wave, allowing for simultaneous transmis
49                   These results suggest that electromagnetic waves alter the conformation of Spike, t
50  device's response increases with increasing electromagnetic wave amplitude and exhibits prominent br
51 urface, demanding to absorb all the incident electromagnetic wave and remit it as greater wavelengths
52 mentum as a sum of that propagating with the electromagnetic wave and that deposited locally in the m
53 ovide an unprecedented ability to manipulate electromagnetic waves and are an enabling technology for
54 , which studies the resonant interactions of electromagnetic waves and free electrons in solid-state
55 on are insensitive to the incident angles of electromagnetic waves and permittivity of dielectric sub
56 mplex micromachines that are controlled with electromagnetic waves and require custom external instru
57                   Thus, the effective use of electromagnetic waves and warmth localization at the sur
58 y an interaction between the material and an electromagnetic wave, and visualizes the heat source dis
59  the way the metamaterial will interact with electromagnetic waves, and accordingly, how it will tran
60 ositive signal gain, spontaneous emission of electromagnetic waves, and runaway amplification have no
61                                The resultant electromagnetic waves appear as monochromatic signals wi
62 ensional (2D) optical microcavities in which electromagnetic waves are confined in either metallic or
63                                              Electromagnetic waves are ideal candidates for transmitt
64                                              Electromagnetic waves are known to exert optical forces
65                              Planetary-scale electromagnetic waves are observed to modulate electroma
66 s the length scale of the cross section when electromagnetic waves are scattered by an electrically s
67 crystal and near 100 percent transmission of electromagnetic waves around sharp 90 degree corners wer
68 ally the topologically robust propagation of electromagnetic waves around sharp corners without backs
69 observations of the exponential decay of the electromagnetic wave as it propagates through the disord
70 oring changes in non-ionizing radiofrequency electromagnetic waves as they traverse the brain can det
71 sity regulation of reflected and transmitted electromagnetic waves, as well as their wavelength and p
72 y to determine the magnitude and phase of an electromagnetic wave at every point in space, as well as
73  electromagnetic radiation source to deflect electromagnetic waves at a desired frequency, ranging fr
74 iate the interference of slowly decompressed electromagnetic waves at far field to form images.
75 lectrons are accelerated more effectively by electromagnetic waves at frequencies of a few kilohertz.
76 vice that directly converts free-propagating electromagnetic waves at optical frequencies to direct c
77  anomalous propagation properties of surface electromagnetic waves at resonance result in extremely l
78 ction), which originates from retardation of electromagnetic waves at the distances comparable to a w
79 nce and manipulate terahertz (THz) frequency electromagnetic waves at the nanoscale.
80 tons offers numerous possibilities to tailor electromagnetic waves at the nanoscale.
81  can change the local phase and intensity of electromagnetic waves at the subwavelength unit level an
82 artificial surfaces engineered to manipulate electromagnetic waves at will - represent highly promisi
83 e theorem, the gravitational force inside an electromagnetic wave ball results in a point energy that
84 roperty to be transparent or absorbing of an electromagnetic wave based on tunable electronic propert
85 l realization of a topological insulator for electromagnetic waves based on engineered bianisotropic
86                                              Electromagnetic wave-based analogue computing has become
87 re, we propose a general method to transform electromagnetic waves between two arbitrary surfaces.
88 vely study the general case of refraction of electromagnetic waves between two strongly anisotropic (
89              These results are described for electromagnetic waves, but are directly relevant to othe
90 etasurfaces enable a new paradigm to control electromagnetic waves by manipulating subwavelength arti
91 fferent type of control of the scattering of electromagnetic waves by means of the graphene layers.
92 e a mechanism that can both hold and amplify electromagnetic waves by rapidly changing the permittivi
93 are lost due to the reflection/absorption of electromagnetic waves by the sheath of plasma created by
94  measure the subsequent coherent emission of electromagnetic waves by water molecules.
95 orthogonal to the magnetic field of incident electromagnetic wave can be generated.
96                   Scattering of particles by electromagnetic waves can lower the plasma conductivity.
97                                              Electromagnetic waves carrying orbital angular momentum
98 posite media that link effective elastic and electromagnetic wave characteristics to one another, inc
99 ems-level symmetry breaking to enable active electromagnetic wave control.
100 larization is one of the basic properties of electromagnetic waves conveying valuable information in
101                Surface polaritons, which are electromagnetic waves coupled to material charge oscilla
102 hod for achieving root canal disinfection by electromagnetic waves, creating a synergistic reaction v
103 urface in the phase space of the propagating electromagnetic waves, determines the optical properties
104  resulting in the unidirectional behavior of electromagnetic waves (directional emitter) without any
105 e camera can capture quantitatively accurate electromagnetic wave distribution in the diffraction lim
106 accordance with the frequency of an incoming electromagnetic wave due to the frequency dispersion or
107  significant interaction cross-sections with electromagnetic waves due to their large surface area-to
108 imated amplitude of radiofrequency-modulated electromagnetic waves emitted by the cell phone.
109     This work successfully reports that weak electromagnetic waves (EMWs) could cohere the microparti
110 ng devices exploit fundamental properties of electromagnetic waves, enabling parallel signal processi
111 tic fields when the specimen is subjected to electromagnetic wave excitation.
112 dal light pulses, as space-time nonseparable electromagnetic waves, exhibit unique topological proper
113 e coupling between the Weyl fermions and the electromagnetic wave for further study of novel light-ma
114   A metal is a material highly reflective to electromagnetic waves for frequencies up to the optical
115 heses predominantly use wired connections or electromagnetic waves for powering and data telemetry, w
116 this data provides proof-of-concept in using electromagnetic waves for sanitation and prevention effo
117              Plasmaspheric hiss is a type of electromagnetic wave found ubiquitously in the dense pla
118 ly occurring chorus emissions are a class of electromagnetic waves found in the space environments of
119 mass, e is the electron charge, and f is the electromagnetic-wave frequency.
120 ption, allowing detection of a wide range of electromagnetic waves from ultraviolet and visible, to t
121 impact in optics due to its interaction with electromagnetic waves gave rise to a multitude of effect
122 which diffusion is inhibited and waves (also electromagnetic waves) get localized.
123  these antennas sense the magnetic fields of electromagnetic waves, giving a piezoelectric voltage ou
124 eration is determined by the interference of electromagnetic waves, giving rise to the resonance spec
125                          A broad spectrum of electromagnetic waves has been explored for wireless neu
126 lity of cloaking an object from detection by electromagnetic waves has recently become a topic of con
127 tions, to name but a few, where conventional electromagnetic waves have a number of limitations, most
128 e indices acts to prevent the propagation of electromagnetic waves having certain wavelengths.
129 mensions than the wavelength of the incident electromagnetic wave, hence behaving as artificial mater
130 of plasmaspheric hiss, a naturally occurring electromagnetic wave in the high-density plasmasphere (r
131 stration of enhanced broadband absorption of electromagnetic waves in a continuously modulated time-v
132 pens new degrees of freedom for manipulating electromagnetic waves in air.
133 ablation technique uses microwaves, applying electromagnetic waves in an approximate range of 900 MHz
134 figurable metasurfaces capable of deflecting electromagnetic waves in an electronically controllable
135 nsion topology to control the propagation of electromagnetic waves in artificially engineered photoni
136 ose connection between the two, showing that electromagnetic waves in both materials are governed by
137  Hamiltonians derived for the propagation of electromagnetic waves in dedicated spatial structures.
138            The sub-luminal phase velocity of electromagnetic waves in free space is generally unobtai
139 ributed to an anomalously high absorption of electromagnetic waves in its layered, metamaterial-like
140 ructures capable of dynamically manipulating electromagnetic waves in real-time.
141                  We demonstrate that surface electromagnetic waves in such materials may exhibit a "p
142 ual dispersion and attenuation of transverse electromagnetic waves in the few-THz regime on nanoscale
143 xion dark matter can resonantly convert into electromagnetic waves in the solar corona when their mas
144 ating the spectral and spatial properties of electromagnetic waves in unconventional ways.
145          Optical metasurfaces can manipulate electromagnetic waves in unprecedented ways at ultra-thi
146 h negative refractive indices can manipulate electromagnetic waves in unusual ways, and can be used t
147 ives us another degree of freedom to control electromagnetic waves in various fields including wirele
148 nce it allows for control over the traveling electromagnetic waves, in a way that goes far beyond ord
149          It was hypothesized previously that electromagnetic waves inside left-handed metamaterials p
150                         Penetration depth of electromagnetic wave into samples decreased with increas
151  a single photon, it nonetheless divides the electromagnetic wave into transmitted and reflected, wit
152                                   A coherent electromagnetic wave is expected to be induced by dark p
153 (R), absorption (A), and transmission (T) of electromagnetic waves is a key objective in quantum opti
154                       Resonant scattering of electromagnetic waves is a widely studied phenomenon wit
155                          This method to trap electromagnetic waves is also applicable to electronic a
156               Controlling the propagation of electromagnetic waves is important to a broad range of a
157 ntly manipulating the polarization states of electromagnetic waves is of great importance for communi
158 for achieving spin-selective transmission of electromagnetic waves is proposed.
159                           Dynamic control of electromagnetic wave jamming is a notable technological
160 in penetration capability compared to longer electromagnetic waves, leading to less obvious visuals o
161 e direct evidence that a naturally occurring electromagnetic wave, lower-band chorus, can drive pulsa
162 ionally allows for an infinite wavelength of electromagnetic waves, manifesting exotic spatially-stat
163 tform enables reconfigurable metasurface for electromagnetic wave manipulation and control for wirele
164 around obstacles, opening a new paradigm for electromagnetic wave manipulation in air.
165 tials for real-time, fast, and sophisticated electromagnetic wave manipulation such as dynamic hologr
166 implies the existence of a spacetime of pure electromagnetic waves of energies but without particles;
167 o their strong chiroptical interactions with electromagnetic waves of incident light.
168 ction (i.e., endfire radiation pattern) over electromagnetic waves of orthogonal electric components.
169 ve mode, obtaining the power supply from the electromagnetic waves of the RFID reader or from a small
170 es can manipulate the amplitude and phase of electromagnetic waves, offering applications from antenn
171 also be applied to escape detection by other electromagnetic waves or sound.
172 y thin layers capable of perfectly absorbing electromagnetic waves over a wide bandwidth.
173  and adaptive wireless links by manipulating electromagnetic waves over free space.
174 velocity of information, which is carried by electromagnetic wave packets, to the speed of light in f
175                                              Electromagnetic waves pass exclusively through the nanog
176        Whistler-mode emissions are important electromagnetic waves pervasive in the Earth's magnetosp
177  have made the exotic control of the flow of electromagnetic waves possible, which is difficult to ac
178     Mergers that emit both gravitational and electromagnetic waves probe the formation of short gamma
179                 In order to determine how an electromagnetic wave propagates from a base station to a
180 d field enhancement of magnetic field for an electromagnetic wave propagating in Mie-resonance-based
181                           Dynamic control of electromagnetic wave propagation direction through this
182                          Here, the theory of electromagnetic wave propagation in diffusive media is c
183 om-built, multi-physics model to investigate electromagnetic wave propagation in human tissue and stu
184                                  Controlling electromagnetic wave propagation in multiple scattering
185                                              Electromagnetic wave propagation in three-dimensional (3
186               The a priori ability to design electromagnetic wave propagation is crucial for the deve
187 up to 1.5 GPa, and the attenuation degree of electromagnetic wave reaches 99.999999999% (110 dB) with
188                             However, whether electromagnetic waves reduce SARS-CoV-2 infectivity is u
189 e acoustic resonance of the antenna with the electromagnetic wave, reducing the antenna footprint by
190 d characterized for suppressing the specular electromagnetic wave reflection or backward radar cross
191 ery, 123 nonradioactive, infrared-activated, electromagnetic wave reflectors were percutaneously inse
192 bjects and may also have extensions to other electromagnetic wave regimes, including radio and sound.
193 ls and may lead to potential applications in electromagnetic wave related metrology.
194 n of the electron resonant interactions with electromagnetic waves remains poorly understood owing to
195                                        Using electromagnetic waves represents an alternative strategy
196    State-of-the-art compact antennas rely on electromagnetic wave resonance, which leads to antenna s
197  at a normal angle only, although in reality electromagnetic waves scatter from various structures or
198 ibits AT characteristics of linear polarized electromagnetic wave sensitive to both polarization dire
199 eries, supercapacitors, compression devices, electromagnetic wave shielding and sensors.
200 nciple is justified by scientific deduction, electromagnetic wave simulations and carefully designed
201 fringe patterns were confirmed via extensive electromagnetic wave simulations to be standing-waves fo
202 s are supported by numerical as well as full electromagnetic wave simulations.
203 cally reconfigurable system with an external electromagnetic wave source at radio frequencies (RF) in
204 a surface plasmon polariton (SPP)--a surface electromagnetic wave that is coupled to the free electro
205                         Surface plasmons are electromagnetic waves that can exist at metal interfaces
206                              One property of electromagnetic waves that has been recently explored is
207 nents is modeled using scalar diffraction of electromagnetic waves through a pixelated multi-level 3D
208 sed on the transmission-reflection theory of electromagnetic waves through a series of inhomogeneous
209 inear oscillators and the propagation of the electromagnetic waves through non-linear Bloch waves of
210       These ME antennas receive and transmit electromagnetic waves through the ME effect at their aco
211 gy harvesting, and the remarkable ability of electromagnetic wave to traverse obstacles and abrupt st
212 als have been discovered that can manipulate electromagnetic waves to create perfect absorption of in
213                         The rectification of electromagnetic waves to direct currents is a crucial pr
214  of a material to behave as a lens and focus electromagnetic waves to produce a real image.
215 tonics, where spin waves are used instead of electromagnetic waves to transmit and process informatio
216 ine based on topologically protected surface electromagnetic waves (TPSWs) between two PTIs which are
217 , non-local voltage generation and anomalous electromagnetic wave transmission.
218 orthern Norway, which has several high power electromagnetic wave transmitters and receivers in the r
219                    Transmission spectra show electromagnetic waves traverse the composite medium from
220 ng the reflection and absorption of incident electromagnetic waves using various submicrometre-thick
221                With the purpose to transform electromagnetic waves, we morph the shapes of FSS design
222 ot heat under RF fields due to reflection of electromagnetic waves, whereas composites with low condu
223 ivity to externally alternating current (AC) electromagnetic waves, which is attributed to the vortex
224 egative-index materials) can support surface electromagnetic waves, which now play crucial roles in p
225 fundamental mechanisms behind interaction of electromagnetic waves with 2D materials.
226 ntenna devices has been achieved by applying electromagnetic waves with different frequencies and amp
227               Such media support propagating electromagnetic waves with extremely large wave vectors
228 er occurs due to the resonant interaction of electromagnetic waves with fast electrons in the relativ
229 re that reveal strong, circularly polarized, electromagnetic waves with frequencies near 100 Hz.
230 ctively infinitely-long slit passes incident electromagnetic waves with no cutoff, enhances the elect
231  an absorptive or emissive semiconductor for electromagnetic waves with orthogonal linear polarizatio
232 originate from strong resonances of incident electromagnetic waves with plasmonic and excitonic state
233                           The interaction of electromagnetic waves with the designed structure is inv
234 olic dispersion, which allows propagation of electromagnetic waves with wave vectors much larger than

 
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