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1 within 100 nm of the plasma membrane (in the evanescent field).
2 nt over the Si waveguide due to its stronger evanescent field.
3  field extends beyond the cavity, forming an evanescent field.
4 both electric and magnetic components of the evanescent field.
5 in push and twist a probe Mie particle in an evanescent field.
6 resence of the gold nanoparticles within the evanescent field.
7 yond the conventional monotonic decay of the evanescent field.
8 en the sample surface and the UME within the evanescent field.
9 orescence microscopy utilizing the generated evanescent field.
10 e rate of diffusion through the depth of the evanescent field.
11 e to the enhanced intensity of the resonance evanescent field.
12  diffusion coefficient, and the depth of the evanescent field.
13 cting with the external medium through their evanescent fields.
14 ample surface, we observe a maximum of these evanescent fields.
15 ell, through the porous membrane, and to the evanescent field above the biosensor's top layer, genera
16 l calculations it is also predicted that the evanescent field above the nickel films penetrates deepe
17 des serve as optical transducer for tailored evanescent field absorption analysis.
18  spectroscopy for simultaneous spectroscopic evanescent field absorption and scanning probe measureme
19 concept, the detection of acetone in D2O via evanescent field absorption is demonstrated achieving a
20                                              Evanescent field absorption measurements indicate a sign
21 s for plasma membranes were investigated via evanescent field absorption spectroscopy of a model anal
22 nts of oil in water using mid-infrared (MIR) evanescent field absorption spectroscopy via fiberoptic
23 taxy (MBE) as waveguide enabling sensing via evanescent field absorption spectroscopy, as demonstrate
24 duced processes at IR waveguide surfaces via evanescent field absorption spectroscopy.
25 elated bulk spectral changes by mid-infrared evanescent field absorption spectroscopy.
26  for liquid-phase chemical sensing utilizing evanescent field absorption spectroscopy.
27 e constant and rate of diffusion through the evanescent field agree with previous results, and all me
28 to deeply subdiffractional scales, while the evanescent field allows for interactions with substrates
29 romolecule such as DNA can extend beyond the evanescent field and analyte interaction results in a la
30                            Using alternating evanescent field and epifluorescence illumination, we sh
31 ulates both the accumulation of GLUT4 in the evanescent field and the fraction of this GLUT4 that is
32 obe as an overlap integral of the nanowire's evanescent field and the probe's response function.
33 , it is possible to confine even further the evanescent field, and by varying the angle of incidence,
34 f the two chemical species, the depth of the evanescent field, and the size of the observed area on t
35 eview existing techniques for characterizing evanescent fields, and we provide a roadmap for comparin
36 ear surface region of a sensor area with the evanescent field, any change of the refractive index of
37 in which a bright flash of strongly decaying evanescent field ( approximately 64 nm exponential decay
38 solated molecules excited either through the evanescent field at the quartz-liquid interface or as a
39 his work demonstrates the feasibility of new evanescent field-based biosensors that can specifically
40                                              Evanescent field-based fluorescence detection enabled mo
41  of label-free nanophotonic biosensors using evanescent-field-based sensing with plasmon resonances i
42 ogenerated ferricyanide within the resulting evanescent field, beyond the optical interface, was dete
43  static, moving vertically in and out of the evanescent field but with little lateral motion.
44 in solution diffuse through the depth of the evanescent field, but do not bind to the surface of inte
45 d is illustrated for the example of infrared evanescent field chemical sensors.
46 heres containing gold nanoparticles in their evanescent field combine the light guiding properties of
47 r-mode profiles and to preferentially select evanescent field concentrations such as the axial hotspo
48 iented membrane probe excited by a polarized evanescent field created by total internal reflection (T
49 ments demonstrated that diffusion out of the evanescent field determined the track lifetimes.
50 spectrum within the penetration depth of the evanescent field due to displacement of water molecules
51 e fluorophore was excited directly or by the evanescent field due to the surface plasmon resonance.
52 ction (TIR) has been applied to generate the evanescent field (EF), exploring aggregation kinetics ne
53 interrogating oil-in-water emulsions via the evanescent field emanating from the waveguide surface, a
54 ybridization assay sensor that relies on the evanescent field excitation of fluorescence from surface
55 With total internal reflection fluorescence, evanescent field excitation, supercritical angle fluores
56                               The WGM has an evanescent field extending into the capillary core and r
57                                          The evanescent field extends into the core and is sensitive
58  single, FM1-43-stained synaptic vesicles by evanescent field fluorescence microscopy, and tracked th
59 h high temporal and spatial resolution using evanescent field fluorescence microscopy.
60 s(3,4)P(2)/PtdIns(3,4,5)P(3), as measured by evanescent field fluorescence microscopy.
61 abeling experiments and when visualized with evanescent-field fluorescence microscopy.
62 ly developed magnetically assisted transport evanescent field fluoroassays (MATEFFs), takes advantage
63 IA approach, Magnetically-Assisted Transport Evanescent Field Fluoroimmunoassays (MATEFFs), which see
64 s involved granules that were present in the evanescent field for at least 12 s.
65 s involved granules that were present in the evanescent field for no more than 0.3 s, indicating that
66 y-coated membranes were illuminated with the evanescent field from a totally internally reflected las
67                          In this method, the evanescent field from an internally reflected excitation
68 ey feature of the present method is that the evanescent field generated by TIR illumination harnesses
69 laser at 644 nm and a right-angled prism for evanescent field generation on prism surface.
70 E penetrates into the exponentially decaying evanescent field in close vicinity (a few micrometer) to
71                                 The decay of evanescent field intensity beyond a dielectric interface
72 le angles, and corrected for angle-dependent evanescent field intensity using "reference" images acqu
73 on, owing to the exponential distribution of evanescent field intensity, the evanescent imaging syste
74 a thin layer of ZnO nanoparticles to enhance evanescent field interaction with the VOCs at the fiber
75 tes using total internal reflection where an evanescent field interacts with bound antibody immobiliz
76 opy experiments the penetration depth of the evanescent field into the stratum corneum is comparable
77 he measurement of key properties such as the evanescent field into the vacuum cladding with nanometer
78                                          The evanescent field is made accessible through the use of a
79 erformed at the SPR sensor surface where the evanescent field is the strongest.
80                                           An evanescent field is used to excite cleaved AMC and the r
81  single-molecule level by imaging within the evanescent field layer using total internal reflection f
82 erfaces were monitored by imaging within the evanescent field layer using total internal reflection f
83 t various pHs and ionic strengths within the evanescent-field layer (EFL) at a water/fused-silica int
84 nic strengths within the 180-nanometer-thick evanescent-field layer at a fused-silica surface.
85 wide range of incident angles with different evanescent-field layer thicknesses, the fluorescence int
86 wide range of incident angles with different evanescent-field layer thicknesses, the fluorescence int
87 te interface can be fluorescently excited by evanescent field light polarized either perpendicular or
88 r beam epitaxy for use in mid-infrared (MIR) evanescent field liquid sensing.
89                                              Evanescent field microscopy has shown that, during exocy
90                                 We have used evanescent field microscopy to image Annexin 2-GFP in li
91                              Using two-color evanescent field microscopy, we imaged the lipid probe F
92 single granules in live cells were imaged by evanescent field microscopy.
93               The cell surface was imaged by evanescent field microscopy.
94  proteins in different colors, and two-color evanescent-field microscopy was used to view single gran
95 ough quantitative analysis and modeling that evanescent fields must be precisely matched between FRET
96                In order to exploit the whole evanescent field of BSW, extended three-dimensional hydr
97 e to a change of its average position in the evanescent field of excitation and can be associated wit
98 anoscale object that subsequently enters the evanescent field of the cavity perturbs the system from
99 eled biological complexes are excited by the evanescent field of the guided light.
100  in the local refractive index probed by the evanescent field of the guided optical mode in the devic
101  the Belinfante momentum to particles in the evanescent field of waveguides depends in a non-trivial
102  measure the optical interaction between the evanescent fields of microfiber and ovarian cancer inter
103 s formed at the antinodes of a standing-wave evanescent field on a nanophotonic waveguide.
104 e-, orientation-, and polarization-dependent evanescent fields on the surfaces of A431 cancer cells a
105 nciple, efficiently load cold atoms into the evanescent-field optical trap generated by the suspended
106 recovery, bleach time, bleach intensity, and evanescent field penetration depth; the model included i
107 f plasmon waves in biological samples, these evanescent fields reflect the changes in EGFR kinase dom
108  300-nm region measurably illuminated by the evanescent field resulting from total internal reflectio
109 LMR) phenomenon by strengthening the fiber's evanescent field, resulting in improved sensitivity and
110  biosensors are advantageous combinations of evanescent field sensing and optical phase difference me
111  range reveal a substantial potential of MIR evanescent field sensing devices for on-line in situ env
112 nce of thin film optical waveguides used for evanescent field sensing of liquid chemical and biologic
113 he polymer coating is performed by utilizing evanescent field spectroscopy in the fingerprint range (
114 ses optical gradient forces generated in the evanescent field surrounding hybrid photonic-plasmonic s
115 rs from diffraction limit due to the loss of evanescent field that carries subwavelength information.
116 support a highly-penetrating surface plasmon evanescent field that extends well into the dielectric m
117 nternal reflection is employed to excite the evanescent field to enhance light-analyte interaction an
118 zing the enhanced sensitivity of superchiral evanescent fields to mesoscale chiral structure.
119  multilayer dielectric waveguides as well as evanescent fields to strongly confine light in low-index
120 IR) detector elements-serving as on-chip MIR evanescent field transducers in combination with tunable
121 single atoms falling through the resonator's evanescent field, we determine the coherent coupling rat
122 senting BCECF translational diffusion in the evanescent field, were in the range 2.2-4.8 ms (0.2-1 ms
123 y and tracked them in three dimensions in an evanescent field where the nanoparticles appeared bright
124  interaction of the propagating light in the evanescent field with glucose molecules.
125 Here we demonstrate a superlens for electric evanescent fields with low losses using perovskites in t
126 eviously derived models for diffusion in the evanescent field within the nanostructure, the diffusion

 
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