戻る
「早戻しボタン」を押すと検索画面に戻ります。

今後説明を表示しない

[OK]

コーパス検索結果 (1語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1 driven by the electric field of the incident electromagnetic wave.
2 , space-variant phase changes on an incident electromagnetic wave.
3 olecular interactions can be captured by THz electromagnetic wave.
4 by enabling precise control over the flow of electromagnetic waves.
5 st because of their unusual interaction with electromagnetic waves.
6  more energy efficient than communicating by electromagnetic waves.
7 ination of the data channels available using electromagnetic waves.
8 s cavity may be unstable to superradiance of electromagnetic waves.
9 thin film, which results in the radiation of electromagnetic waves.
10 e potential for application in absorption of electromagnetic waves.
11 ing the bidirectional polarization states of electromagnetic waves.
12 ulation and switching of broadband terahertz electromagnetic waves.
13 m systems in analogy to cloaking devices for electromagnetic waves.
14  transmission, absorption, and scattering of electromagnetic waves.
15 lar resonances, at normal incidence of plane electromagnetic waves.
16 s an additional degree of freedom to control electromagnetic waves.
17  emission, propagation and scattering of the electromagnetic waves.
18  a handpiece that emitted infrared light and electromagnetic waves.
19 tance for controlling their interaction with electromagnetic waves.
20 ity with pure rotation of linearly polarized electromagnetic waves.
21  7-50 nm were used as absorber materials for electromagnetic waves.
22 h as tunability, switching and modulation of electromagnetic waves.
23 ct that it can achieve unity absorptivity of electromagnetic waves.
24 fficient devices to manipulate the terahertz electromagnetic waves.
25                                          The electromagnetic wave absorbing composite films were prep
26  The experimental results indicated that the electromagnetic wave absorbing properties of ACNTs are s
27  microscope and X-ray diffraction, and their electromagnetic wave absorbing properties were measured
28  electron gases, collectively accelerated by electromagnetic waves according to Newton's second law o
29 found evidence for global contributions from electromagnetic waves (Alfven waves).
30 ally to distribute and route the propagating electromagnetic wave, allowing for simultaneous transmis
31 mentum as a sum of that propagating with the electromagnetic wave and that deposited locally in the m
32 ovide an unprecedented ability to manipulate electromagnetic waves and are an enabling technology for
33 on are insensitive to the incident angles of electromagnetic waves and permittivity of dielectric sub
34 y an interaction between the material and an electromagnetic wave, and visualizes the heat source dis
35                                              Electromagnetic waves are ideal candidates for transmitt
36                                              Electromagnetic waves are known to exert optical forces
37 s the length scale of the cross section when electromagnetic waves are scattered by an electrically s
38 crystal and near 100 percent transmission of electromagnetic waves around sharp 90 degree corners wer
39 ally the topologically robust propagation of electromagnetic waves around sharp corners without backs
40 observations of the exponential decay of the electromagnetic wave as it propagates through the disord
41 oring changes in non-ionizing radiofrequency electromagnetic waves as they traverse the brain can det
42  electromagnetic radiation source to deflect electromagnetic waves at a desired frequency, ranging fr
43 iate the interference of slowly decompressed electromagnetic waves at far field to form images.
44 lectrons are accelerated more effectively by electromagnetic waves at frequencies of a few kilohertz.
45 vice that directly converts free-propagating electromagnetic waves at optical frequencies to direct c
46 ction), which originates from retardation of electromagnetic waves at the distances comparable to a w
47 roperty to be transparent or absorbing of an electromagnetic wave based on tunable electronic propert
48 l realization of a topological insulator for electromagnetic waves based on engineered bianisotropic
49 re, we propose a general method to transform electromagnetic waves between two arbitrary surfaces.
50              These results are described for electromagnetic waves, but are directly relevant to othe
51 etasurfaces enable a new paradigm to control electromagnetic waves by manipulating subwavelength arti
52 fferent type of control of the scattering of electromagnetic waves by means of the graphene layers.
53 are lost due to the reflection/absorption of electromagnetic waves by the sheath of plasma created by
54                                              Electromagnetic waves carrying orbital angular momentum
55 larization is one of the basic properties of electromagnetic waves conveying valuable information in
56                Surface polaritons, which are electromagnetic waves coupled to material charge oscilla
57 urface in the phase space of the propagating electromagnetic waves, determines the optical properties
58  resulting in the unidirectional behavior of electromagnetic waves (directional emitter) without any
59 e camera can capture quantitatively accurate electromagnetic wave distribution in the diffraction lim
60 accordance with the frequency of an incoming electromagnetic wave due to the frequency dispersion or
61 imated amplitude of radiofrequency-modulated electromagnetic waves emitted by the cell phone.
62 tic fields when the specimen is subjected to electromagnetic wave excitation.
63              Plasmaspheric hiss is a type of electromagnetic wave found ubiquitously in the dense pla
64 mass, e is the electron charge, and f is the electromagnetic-wave frequency.
65 ption, allowing detection of a wide range of electromagnetic waves from ultraviolet and visible, to t
66 which diffusion is inhibited and waves (also electromagnetic waves) get localized.
67  these antennas sense the magnetic fields of electromagnetic waves, giving a piezoelectric voltage ou
68 lity of cloaking an object from detection by electromagnetic waves has recently become a topic of con
69 e indices acts to prevent the propagation of electromagnetic waves having certain wavelengths.
70 mensions than the wavelength of the incident electromagnetic wave, hence behaving as artificial mater
71 of plasmaspheric hiss, a naturally occurring electromagnetic wave in the high-density plasmasphere (r
72 pens new degrees of freedom for manipulating electromagnetic waves in air.
73 figurable metasurfaces capable of deflecting electromagnetic waves in an electronically controllable
74 ose connection between the two, showing that electromagnetic waves in both materials are governed by
75            The sub-luminal phase velocity of electromagnetic waves in free space is generally unobtai
76 ual dispersion and attenuation of transverse electromagnetic waves in the few-THz regime on nanoscale
77 ating the spectral and spatial properties of electromagnetic waves in unconventional ways.
78 h negative refractive indices can manipulate electromagnetic waves in unusual ways, and can be used t
79 ives us another degree of freedom to control electromagnetic waves in various fields including wirele
80          It was hypothesized previously that electromagnetic waves inside left-handed metamaterials p
81                         Penetration depth of electromagnetic wave into samples decreased with increas
82 (R), absorption (A), and transmission (T) of electromagnetic waves is a key objective in quantum opti
83                          This method to trap electromagnetic waves is also applicable to electronic a
84               Controlling the propagation of electromagnetic waves is important to a broad range of a
85 ntly manipulating the polarization states of electromagnetic waves is of great importance for communi
86 for achieving spin-selective transmission of electromagnetic waves is proposed.
87 e direct evidence that a naturally occurring electromagnetic wave, lower-band chorus, can drive pulsa
88 around obstacles, opening a new paradigm for electromagnetic wave manipulation in air.
89 tials for real-time, fast, and sophisticated electromagnetic wave manipulation such as dynamic hologr
90 ve mode, obtaining the power supply from the electromagnetic waves of the RFID reader or from a small
91 also be applied to escape detection by other electromagnetic waves or sound.
92 velocity of information, which is carried by electromagnetic wave packets, to the speed of light in f
93                                              Electromagnetic waves pass exclusively through the nanog
94        Whistler-mode emissions are important electromagnetic waves pervasive in the Earth's magnetosp
95  have made the exotic control of the flow of electromagnetic waves possible, which is difficult to ac
96 d field enhancement of magnetic field for an electromagnetic wave propagating in Mie-resonance-based
97                           Dynamic control of electromagnetic wave propagation direction through this
98                          Here, the theory of electromagnetic wave propagation in diffusive media is c
99               The a priori ability to design electromagnetic wave propagation is crucial for the deve
100 e acoustic resonance of the antenna with the electromagnetic wave, reducing the antenna footprint by
101 d characterized for suppressing the specular electromagnetic wave reflection or backward radar cross
102 ery, 123 nonradioactive, infrared-activated, electromagnetic wave reflectors were percutaneously inse
103 bjects and may also have extensions to other electromagnetic wave regimes, including radio and sound.
104 ls and may lead to potential applications in electromagnetic wave related metrology.
105    State-of-the-art compact antennas rely on electromagnetic wave resonance, which leads to antenna s
106  at a normal angle only, although in reality electromagnetic waves scatter from various structures or
107 s are supported by numerical as well as full electromagnetic wave simulations.
108 cally reconfigurable system with an external electromagnetic wave source at radio frequencies (RF) in
109 a surface plasmon polariton (SPP)--a surface electromagnetic wave that is coupled to the free electro
110                         Surface plasmons are electromagnetic waves that can exist at metal interfaces
111                              One property of electromagnetic waves that has been recently explored is
112       These ME antennas receive and transmit electromagnetic waves through the ME effect at their aco
113  of a material to behave as a lens and focus electromagnetic waves to produce a real image.
114 tonics, where spin waves are used instead of electromagnetic waves to transmit and process informatio
115 ine based on topologically protected surface electromagnetic waves (TPSWs) between two PTIs which are
116               Such media support propagating electromagnetic waves with extremely large wave vectors
117 re that reveal strong, circularly polarized, electromagnetic waves with frequencies near 100 Hz.
118 ctively infinitely-long slit passes incident electromagnetic waves with no cutoff, enhances the elect
119  an absorptive or emissive semiconductor for electromagnetic waves with orthogonal linear polarizatio
120 originate from strong resonances of incident electromagnetic waves with plasmonic and excitonic state
121 olic dispersion, which allows propagation of electromagnetic waves with wave vectors much larger than

WebLSDに未収録の専門用語(用法)は "新規対訳" から投稿できます。
 
Page Top