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1 data above and beyond standard limits of the optical system.
2 ofabricated laminar-flow mixer to a confocal optical system.
3 a single wavelength and analyzed by a simple optical system.
4 try and stability, and low dispersion in the optical system.
5 ent points as well as the performance of the optical system.
6 imaging with no additional complexity in the optical system.
7 ncrease the telecommunication capacity of an optical system.
8 within the depth of focus (DOF) of the Raman optical system.
9 c range for sensitivity without altering the optical system.
10 nts were measured using a high-resolution 3D optical system.
11  achieved within 95 min using the integrated optical system.
12 evaluate the performance of the fluorescence optical system.
13  in this work is a ray trace analysis of the optical system.
14 e liquids tunes the characteristics of these optical systems.
15 le optical properties not present artificial optical systems.
16 rigid instruments that relied on rudimentary optical systems.
17 ancing the spatial resolution of traditional optical systems.
18 ar components enables the miniaturization of optical systems.
19 nsmission and reflection spectra of resonant optical systems.
20 ith the same accuracy as standard microscopy optical systems.
21  the effects of loss are major challenges in optical systems.
22 ed with a measuring tape and then by the two optical systems.
23 egration and scale-up of solid-state quantum optical systems.
24 tromagnetic metamaterials and reconfigurable optical systems.
25 d specificity potentially rivaling bench-top optical systems.
26 e control is a fundamental building block of optical systems.
27            In contrast, traditional man-made optical systems achieve focusing by physical displacemen
28 es of experiments to develop and validate an optical system and image analysis algorithm based upon a
29  development of the photoelectric absorption optical system and the incorporation of the Rayleigh int
30                                          The optical system and the source of aberrations in a confoc
31    Photonic nanostructures are used for many optical systems and applications.
32 based detection technique requires expensive optical systems and complex bioinformatics tools.
33 are challenging because they require complex optical systems and diagnostics.
34 ological potential in drug delivery, 'smart' optical systems and microelectromechanical systems.
35  Each replica was scanned 10 times with a 3D optical system, and 3D datasets representing the compute
36 zation control is therefore pivotal for many optical systems, and achieved using bulk devices such as
37 aging optical fibres and lasers in nonlinear optical systems, and gravitational singularities associa
38 hR2) or halorhodopsin (eNpHR3.0), via an all-optical system applied to monolayers of neonatal rat ven
39                    Resolution limitations of optical systems are major obstacles for determining whet
40                               Except for the optical system, as in the calcified lenses of trilobite
41 el methods to increase light transmission in optical systems, as well as to eliminate unwanted reflec
42 n the optical properties of Bragg mirrors in optical systems at temperatures above 700 degrees C beca
43  numerical digits monocularly within a Badal optical system (at both 0.0 and -3.0 D) while performing
44  refractive power was measured with a custom optical system based on the Scheiner principle.
45 h a modified commercial lensmeter or with an optical system based on the Scheiner principle.
46  report the observation of rogue waves in an optical system, based on a microstructured optical fibre
47 uclear magnetic resonance, cold ion trap and optical systems, but a solid-state realization has remai
48 tchable direction of light propagation in an optical system by steering it to an exceptional point (E
49 llustrates how transient nonlinearity in the optical system can be exploited to tackle complex optimi
50 ng traditional absorbance or an interference optical system can be used for protein-protein interacti
51                               Disorder-based optical systems can be implemented in one-dimensional st
52 5 nm laser excitation with a linear-scanning optical system capable of multichannel real-time fluores
53   A new, in situ sensing system, Channelized Optical System (CHANOS), was recently developed to make
54                                     A simple optical system, comprising a diode laser (405 nm), an op
55          Here we describe measurements of an optical system consisting of a pair of specially pattern
56  In this study, we employed a hybrid diffuse optical system consisting of diffuse correlation spectro
57 the microarray substrate at the focus of the optical system delivering the light and which can be con
58 with a protein, and a plasmonic surface, the optical system described here selectively amplifies a si
59 o advances in materials science and creative optical system designs.
60 the current study is to report an innovative optical system for dual oxyphor phosphorescence lifetime
61         Here we report an achromatic Fresnel optical system for EUV or X-ray radiation that combines
62 m dot (QD)-based immunosensor using a simple optical system for human serum albumin (HSA) detection i
63                       Here we describe a new optical system for rapid uncaging in arbitrary patterns
64 ial of this technology in the development of optical systems for microscopy, photography, and compute
65 ns can be found in linking optical qubits to optical systems for which coupling is best described in
66  molecule to the point spread function of an optical system greatly improves the precision with which
67 emonstrating blind quantum computation in an optical system has raised new challenges regarding the s
68                    Compared to near-infrared optical systems, however, mid-infrared component technol
69                             We employed this optical system in the setting of ventricular tachycardia
70                                          The optical system is able to provide a clean, high-flux X-r
71                                          The optical system is completed by a low-numerical-aperture
72                                          Our optical system is conceptualized to provide optimal perf
73                                           An optical system is described for simultaneous video imagi
74 monstration of chaotic communication with an optical system is described.
75 copy, the signal-to-noise ratio (SNR) of the optical system is directly linked to the numerical apert
76 ing is employed to encrypt a 3-D object, the optical system is incoherent, resulting in negligible am
77                                     A simple optical system is used to generate a polarization-varian
78 ailable temporal and spatial channels of the optical system, making it difficult to represent informa
79 ectrode arrays, video microscopy, and an all-optical system measuring calcium transients.
80                             The move towards optical system miniaturization therefore motivates the d
81                           Improvement of the optical system of minilaparoscopes may allow reliable be
82                                         This optical system opens possibilities for rapid, inexpensiv
83 holds promise for integration within compact optical systems operating at visible frequencies.
84                 Vision, which consists of an optical system, receptors and image-processing capacity,
85 llent in many ways, scaling to large quantum optical systems remains challenging.
86                               Most practical optical systems require that the device properties be ti
87 his approach presents a path to creating the optical systems required for large-scale trapped-ion qua
88 s enhancement can be achieved using resonant optical systems such as plasmonic particles or nanoanten
89                             An image-forming optical system that is based on a mirror with an unconve
90                           Here we present an optical system that, under appropriate conditions, ident
91 nd readout, experiments so far have employed optical systems that are cumbersome to scale to even a f
92 escent coupling scheme works well for planar optical systems that are naturally waveguide based, many
93 ic properties in nanomaterials and designing optical systems that efficiently excite and collect ligh
94 es in miniaturization technology have led to optical systems that no longer require complicated mecha
95 al demonstrations have been implemented with optical systems that used both discrete and continuous v
96 ture of the objective, the efficiency of the optical system, the emission rate of the single molecule
97 ticular attention to the organization of the optical system, the retinular cells, the rhabdom, and of
98 oposed for the transport of light through an optical system; this involves photon-photon interactions
99     These results show the promise of an all-optical system to acquire action potentials with precise
100  flexible substrate was incorporated into an optical system to demonstrate high resolution imaging of
101 blue] and 623 [red] nm) were presented by an optical system to one eye after dilation, while the cons
102                  However, using conventional optical systems to generate, analyse and detect circular
103 ar field and near field, it allows far-field optical systems to project an image of the near-field fe
104                       The miniaturization of optical systems (to the micro and nanoscale) has resulte
105 tasurfaces are especially important, as most optical systems used in practice operate in transmission
106                               The customized optical system uses multiple fixed-wavelength lasers to
107  neural activity, we designed a needle-based optical system using gradient-index (GRIN) rod lens.
108 was measured with a custom-built, noncontact optical system, using a focus detection technique.
109                              A three-channel optical system was developed that simultaneously measure
110        A novel fluorescence microscope/laser optical system was developed to measure fast transients
111                                     A custom optical system was used for video recording of tear film
112                             An eight-channel optical system was used to generate lights that differed
113              Maxwellian-view and direct-view optical systems were used to obtain foveal and extrafove
114 ment or modification leads to reconfigurable optical systems, whereas the implementation of optics th
115 s on two critical challenges: the inertia of optical systems, which limits image speed, and aberratio
116 tes within the limited depth-of-focus of the optical system while maintaining the necessary reagent f
117                            A Maxwellian-view optical system with a xenon light source was used to pre
118 mages has been demonstrated in an incoherent optical system with biometric keys.
119                                           An optical system with shaping optics is used to direct a w
120 matic effect in a one-dimensional disordered optical system with spatial features a thousand times sm
121                      Although integration of optical systems with classical microfluidic analysis tec
122 very important class of dissipative (active) optical systems with cyclic gain and losses, such as las
123 e that the two modes can also be observed in optical systems with only a few (artificial) atoms insid
124            BB particles can be a complicated optical system, with scattering and absorption contribut
125 aluation of directly filtered data, using an optical system without extensive numerical spectral anal

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