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1 tection on a liquid-solid interface based on evanescent wave.
2 ng refraction, total internal reflection and evanescent wave.
3 es the metal layer and illuminates muscle by evanescent wave.
4 the distance-dependent intensity decay of an evanescent wave.
5 g angle with the depth of penetration of the evanescent wave.
6  of light propagated on the fiber surface is evanescent waves.
7 undamental mechanisms of such kinetics using evanescent waves.
8 instead of diverging, because of the role of evanescent waves.
9 resolved images by restoring propagative and evanescent waves.
10 ontact of soft objects and the scattering of evanescent waves.
11 ting light, but extraordinary confinement of evanescent waves.
12 e salt, which was measured as an increase in evanescent wave absorbance at 435 nm.
13 anescent-wave sensors to detect the mid-(IR) evanescent-wave absorbance spectra of small areas of bio
14 luorophore is monitored as a function of the evanescent wave absorption of an analyte-sensitive indic
15 er to enhance the phase matching between the evanescent wave and the lossy mode to realize dual-reson
16  Si (n(Si) = 3.4), which leads to a stronger evanescent wave and therefore higher sensitivity, as con
17 TIRF-FOB are (i) fluorescence is excited via evanescent waves and amplified via liposomes; (ii) the u
18 gs illuminate the unusual transverse spin in evanescent waves and explain recent experiments that hav
19 o forms of light energy (refracted light and evanescent waves) and surface-coated photocatalysts.
20                This study reports a reusable evanescent wave aptamer-based biosensor for rapid, sensi
21                         24% of the generated evanescent waves are not absorbed by nano-TiO(2) and ret
22 propagating waves are focused and, moreover, evanescent waves are reconstructed in the image plane.
23                                              Evanescent waves are ubiquitous at interfaces with optic
24 dy the lateral and vertical distributions of evanescent waves around the image plane of such a lens,
25 ial variations of the wave field (carried by evanescent waves), as the one created by edges or small
26                             The depth of the evanescent wave at different layers was altered by tunin
27 ng analyte-containing medium by means of the evanescent wave at the fiber boundary.
28 paves the way for the establishment of novel evanescent wave-based systems.
29  The concentration detection limit of the MB evanescent wave biosensor is 1.1 nM.
30 zed in a polymer matrix, as detected with an evanescent wave biosensor, was investigated.
31                                              Evanescent wave biosensors have found a wide array appli
32                           The application of evanescent wave cavity ring-down spectroscopy (EW-CRDS)
33                                              Evanescent wave cavity ringdown spectroscopy (EW-CRDS) i
34                     In this study, we employ evanescent wave cavity ringdown spectroscopy to probe Gd
35 ically active solid-liquid interface for the evanescent-wave cavity-ring-down spectroscopic (EW-CRDS)
36 sociation kinetics and diffusion through the evanescent wave contribute to the fluorescence fluctuati
37 sociation kinetics and diffusion through the evanescent wave contribute to the fluorescence fluctuati
38 al sound steering, showcasing unidirectional evanescent wave conversion and nonreciprocal upconversio
39 ed a precise optical cavity-based method, an evanescent-wave coupled cavity ring-down spectroscopy (E
40 ee orders of magnitude over the conventional evanescent-wave coupling.
41 offers important advantages over traditional evanescent-wave detection strategies which rely on recor
42       We have prepared a novel optical fiber evanescent wave DNA biosensor using a newly developed mo
43 linear optical cavity-based system combining evanescent wave (EW) with high-sensitive cavity ring-dow
44                Azimuthal beam scanning makes evanescent-wave (EW) excitation isotropic, thereby produ
45 duct of two near-field factors: the depth of evanescent wave excitation and a distance-dependent coup
46 ends on two near-field factors: the depth of evanescent wave excitation and a distance-dependent coup
47  liter with an automated array biosensor and evanescent wave excitation for fluorescence measurements
48                                  The limited evanescent wave excitation volume makes it possible to m
49 n analysis, and fluorescence assays based on evanescent wave excitation.
50 s fit to a model describing diffusion in the evanescent wave excitation.
51        An automated array biosensor based on evanescent-wave excitation has been developed for the de
52  One unknown hampering the interpretation of evanescent-wave excited fluorescence intensities is the
53                                              Evanescent-wave excited fluorescence technology has been
54 g require the quantitative interpretation of evanescent-wave-excited images.
55                  Combining the advantages of evanescent wave fiber optic sensor and microfluidic tech
56               We have developed a disposable evanescent wave fiber optic sensor by coating a molecula
57                                           An evanescent wave fiber optic sensor for detection of Esch
58 g diode based sensor and the other one is an evanescent wave fiber optic sensor.
59                                  A "turn-on" evanescent-wave fiber biosensor based on functional nucl
60                              The subfield of evanescent wave fluorescence biosensors has also matured
61                           We used multicolor evanescent wave fluorescence microscopy imaging to follo
62                                      We used evanescent wave fluorescence microscopy to observe assem
63  Fluorescence in the film was excited by the evanescent wave from attenuated total reflection spectro
64 s based on the excitation confinement of the evanescent wave generated at the glass/cell interface.
65 e technique uses the unique polarizations of evanescent waves generated by total internal reflection
66 er, a wavelength-dependent PA/PT generation, evanescent wave-generated PA, and a back-propagated acou
67 se component of the spin angular momentum of evanescent waves gives rise to lateral optical forces on
68 stigations into the near-field properties of evanescent waves have revealed polarization states with
69 ver, the effective path length, d(e), of the evanescent wave in an ATR measurement, i.e., the equival
70 spectra were measured by excitation with the evanescent wave in total internal reflection, in order t
71   This superlens would allow the recovery of evanescent waves in an image via the excitation of surfa
72 rse-spin angular-momentum-density shifts for evanescent waves in magneto-optic waveguide media.
73 r momentum conversion in magneto-optic media evanescent waves in opposite propagation-directions.
74 imit of light, which is causd by the loss of evanescent waves in the far field that carry high spatia
75 sociation kinetics and diffusion through the evanescent wave, in solution, contribute to the fluoresc
76  of contributions from diffusion through the evanescent wave, in solution, has been published previou
77 ctively detected by following changes in the evanescent-wave-induced fluorescence anisotropy of the i
78 lished optical fiber, providing an efficient evanescent wave interaction.
79 t for sensor coating, a waveguide to provide evanescent wave interrogation, and it can be easily exte
80 length objects by transforming the scattered evanescent waves into propagating waves in an anisotropi
81                    The metamaterial converts evanescent waves into propagative waves exciting trapped
82                                           An evanescent wave is generated by total internal reflectio
83  total reflection setup where the developing evanescent wave is responsible for photothermal excitati
84 impedance analysis and optical sensing using evanescent waves like SPR.
85 cal spots can actually be formed without any evanescent waves, making far-field, label-free super-res
86 emblies in bacteria lacking MCP complexes by evanescent wave microscopy [6].
87                                        Using evanescent wave microscopy and green fluorescent protein
88 ugh a single molecular contact is tracked by evanescent wave microscopy as a force is exerted through
89               Here we developed a dual-color evanescent wave microscopy method to simultaneously meas
90     Direct observation of actin filaments by evanescent wave microscopy showed that cofilins from fis
91                               Using in vitro evanescent wave microscopy, we demonstrated that GMF pot
92 d neuropeptidergic vesicles by wide-field or evanescent-wave microscopy shows that a separate immobil
93 us to fully characterize all propagating and evanescent wave modes from the MetaSurfaces.
94 ssion is due to the enhanced propagating and evanescent wave modes inside the ADNZ medium thanks to t
95 ion spectra obtained in the transmission and evanescent-wave modes are discussed.
96  nanoplasmonic absorption of the fiber optic evanescent wave occurs.
97 ch or exceed the distance encompassed by the evanescent wave of the surface plasmon.
98                                           An evanescent wave optical fiber biosensor based on titania
99  of excitation; that is, it does not require evanescent wave or surface-plasmon excitation.
100 mbdaSH/4 (or lambdapump/8) without involving evanescent waves or subwavelength apertures.
101 ation), the detection volume is a product of evanescent wave penetration depth and distance-dependent
102 ated with the maximum overlap between the IR evanescent wave penetration depth and the analyte diffus
103 ticles synthesized beforehand, or in-situ by evanescent-wave photopolymerization on the fiber.
104                                     A single evanescent wave possesses a spin component, which is ind
105 mats has subsections on planar, fiber optic, evanescent wave, refractive index, surface plasmon reson
106 ercome the diffraction limit by transforming evanescent waves responsible for imaging subwavelength f
107 compared to previous sizes and geometries of evanescent-wave sensors (e.g., commercially available in
108                 Fiber-optic near-ultraviolet evanescent-wave sensors have been constructed, and their
109  strips 30-50 microm thick and 2 mm wide, as evanescent-wave sensors to detect the mid-(IR) evanescen
110         In this research, mid-infrared Fiber Evanescent Wave Spectroscopy (FEWS) supported by statist
111                                  Fiber-optic evanescent wave spectroscopy (FEWS)-FTIR with endoscope-
112 easured by infrared reflection-absorption or evanescent wave spectroscopy) during increase in protein
113 tives, nonlinear methods, fluorescence dyes, evanescent wave tailoring, and point-spread function eng
114                              These modes are evanescent waves that form, for example, surface plasmon
115  a conventional biosensor waveguide based on evanescent waves, the ARROW structure is designed to all
116 on, d(p), to estimate the path length of the evanescent wave through the sample.
117 ect on the propagation and penetration of IR evanescent waves through the film.
118     We demonstrate the use of the calibrated evanescent wave to resolve the 20.1 +/- 0.5-nm step incr
119                        Therefore, maximizing evanescent waves to activate photocatalysts by controlli
120                                 The measured evanescent wave transfer function was then used to conve
121 r a broad visible spectrum and the waveguide evanescent wave was used to excite the Raman signals of
122              It is demonstrated that the ATR evanescent wave, which primarily probes the fluid within
123 ature information of an object is carried by evanescent waves, which exponentially decays in space an
124 enerated LSPR through the interaction of the evanescent wave with AuNPs deposited at the tapered wais

 
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