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1 a pattern of light formed as a doughnut or a standing wave.
2 nce of a high frequency (500 kHz) ultrasonic standing wave.
3           In the orientation domain, it is a standing wave.
4 condensate in an amplitude-modulated optical standing wave.
5 lid and fluid, and arbitrary reflectivity of standing waves.
6 lts via direct detection of phonon-polariton standing waves.
7 e to generate "trapping nodes" in ultrasonic standing waves.
8 strong luminescence and formation of optical standing waves.
9 , gentle particle manipulation by ultrasonic standing waves.
10 ms as a result of the establishment of X-ray standing waves.
11  the pressure nodes or antinodes of acoustic standing waves.
12 oated particle-agglutination assays occur in standing waves.
13 ons from a travelling wave is probabilistic, standing wave absorption can be observed deterministical
14                                              Standing-wave ambient-pressure photoemission spectroscop
15 tates, the real-space distribution of phonon standing wave amplitudes, the scattering phase shifts, a
16                       The field replicates a standing wave and aligns polyethylene microspheres in wa
17 ustly trap along the pressure antinodes of a standing wave and separate from blood components in unde
18  were located in the antinodes of an optical standing wave and were loaded from a Bose-Einstein conde
19 , this effect can be seen as the collapse of standing waves and transition to travelling waves within
20 , particle focusing using multinode acoustic standing waves, and a spatially arrayed detector, can in
21 J ambush foraging associated behaviors (tail standing, waving, and jumping) were unaffected by the ab
22  acoustic field suggest that reflections and standing waves appear when the focus is placed near the
23    Here, we present a resonator nanophotonic standing-wave array trap (resonator-nSWAT) that demonstr
24                                In situ X-ray standing-wave atomic images relative to the hematite lat
25 honon-electron interactions in bulk acoustic standing wave (BAW) resonators made from piezoelectric s
26 e the incident and diffracted electric field standing wave becomes localized in regions of small CCA
27 breaking, is replaced by vertically jetting 'standing-wave breaking' (II).
28                      In between, 'travelling-standing-wave breaking' (III) is characterized by the fo
29 monstrated via direct imaging of polaritonic standing waves by means of infrared nano-optics.
30  multiplanar excitation of fluorescence by a standing wave can be produced in a single-spot laser sca
31         This design makes optimum use of the standing wave cavity to improve the energy efficiency of
32  flicker-induced cortical patterns displayed standing-wave characteristics and matched linear wave eq
33 megahertz-frequency noncavitating ultrasonic standing waves concentrate at submillimetre distances an
34 digitated bar electrode array energized in a standing-wave configuration.
35 lection coefficient, phase lag and period of standing waves, depth of water, permeability, degree of
36                                     Acoustic standing wave devices offer excellent potential applicat
37 m chains along the direction of the acoustic standing wave due to radiation interaction forces exhibi
38 n of energy deposition and the corresponding standing-wave electric-field intensities within the laye
39 eling-wave body undulations (compared with a standing wave) emerges when the dominant thrust-generati
40                               The visualized standing wave enables subwavelength distance measurement
41 and MinD division regulatory proteins form a standing wave enabling MinC, which binds MinD, to inhibi
42 ptical traps is formed at the antinodes of a standing-wave evanescent field on a nanophotonic wavegui
43 ms are rare, but have been shown to resemble standing waves, except that they lack a characteristic w
44 e of dyes specific for the cell membrane how standing-wave excitation can be exploited to generate pr
45                                              Standing-wave excitation of fluorescence is highly desir
46 terning utilizes forces within an ultrasound standing wave field (USWF) to organize cells or micropar
47                                Forces from a standing wave field align microscale particles along the
48 and tuned carefully to maximise the acoustic standing wave field at the cavity resonance.
49 ically caught in the nodal planes of a quasi-standing wave field formed in an acoustic resonator in f
50                                  An acoustic standing wave field is generated in the microchannel, an
51                               In an acoustic standing wave field the cells will be rotated until the
52           Acoustophoresis uses an ultrasonic standing wave field to separate cells based on biomechan
53 ensitive acoustophoresis using an ultrasonic standing wave field, followed by size-insensitive, acous
54 rmined by an applied high-amplitude acoustic standing wave field, in which particles move swiftly to
55 can only be acoustically levitated in simple standing-wave fields.
56 ces was investigated using long-period X-ray standing wave-florescence yield spectroscopy.
57 scence resonance energy transfer and optical standing wave fluorescence interferometry, we characteri
58 ed nuclei is investigated using a two-photon standing wave fluorescence photobleaching experiment wit
59 hickness in living cells (176 +/- 14 nm), by standing-wave fluorescence microscopy, and its F-actin d
60 tterns, which mathematical models explain as standing-wave formations emerging from periodic forcing
61 absorber to control its interaction with the standing wave formed by the incident wave and its reflec
62  by exploring real-space profiles of plasmon standing waves formed between the tip of our nano-probe
63           We experimentally demonstrate that standing waves formed by two coherent counter-propagatin
64 nsive electromagnetic wave simulations to be standing-waves formed between the tip and the edge-up as
65                               Two orthogonal standing waves generate surface flows of counter-rotatin
66  be stably trapped in a surface plasmon (SP) standing wave generated by the constructive interference
67                                     However, standing wave generation requires more than one transduc
68           It is found that the reflection of standing wave has a significant effect on the dynamic re
69                         We further show that standing waves have a strong modulatory effect on activi
70 familiar energy standing waves, polarization standing waves have constant electric and magnetic energ
71 , which are able to promote the formation of standing waves if patterned on a reflective material, ha
72                    By creating an ultrasonic standing wave in the liquid sample, placed on a low-cost
73 ces coupled with the sensitivity provided by standing waves in an optical cavity and detection via im
74  an interaction of the cyclotron motion with standing waves in the trap cavity containing the electro
75  empirical evidence for such flicker-induced standing waves in the visual cortex was missing.
76 ery or periphery-to-fovea traveling waves or standing waves in V1, in which ground truth cortical wav
77 n depth of seabed induced by fully-reflected standing waves increases 82.49% under certain conditions
78  vivo retina and propose that the control of standing waves is a new potential method to modulate the
79              A liquid surface established by standing waves is used as a dynamically reconfigurable t
80                             Here we employ a standing-wave laser field as a spatially resolving probe
81 s the near-field Talbot effect with a single standing-wave laser pulse as a phase grating.
82 -resolving atomic force microscopy and X-ray standing-wave measurements characterise the geometry, X-
83         Our work extends the domain of x-ray standing wave methods to resonant x-ray emission spectro
84 structure of multiparticle resonances at the standing-wave-mode frequencies of the cavity.
85 two pump waves, we can control the generated standing waves' movements and characterize the resonator
86 ervation that atoms could be diffracted by a standing wave of light.
87 f the pectoral and pelvic girdles creating a standing wave of the axial body.
88 of the two condensates causes formation of a standing wave of the condensate density and quantized vo
89 will help to better predict the influence of standing waves on breakwaters and seabed soil, and can p
90 n indicates the presence of a nodal line and standing waves on its surface.
91 the electrode array showing the influence of standing waves on the response.
92  optically driven thermo-optic modulation in standing wave optical fields, with titanium nano-antenna
93 ctures with a low laser power by combining a standing-wave optical trap with confocal Raman spectrosc
94 he dayside by the ionosphere, resulting in a standing wave or eigenmode of the magnetopause surface.
95 s direction compared to when the input was a standing wave, or a traveling wave in a different direct
96 those in vivo and failed to recapitulate the standing wave oscillations observed in vivo.
97 in vivo dynamics of the Min system including standing wave oscillations.
98 n from the cytoplasm drives a self-organized standing wave oscillator.
99                               Unlike current standing-wave parametric amplifiers, this traveling wave
100  the emergence of a distinct electromagnetic standing wave pattern in the cavity.
101                                          The standing wave pattern is generated through bidirectional
102 to avoid the formation of a nonphysiological standing wave pattern.
103 n conventional lasing systems, the resulting standing wave patterns exhibit only minimal overlap with
104 t camera-facilitated imaging and analysis of standing wave patterns in optical ring resonators.
105  typically use an array of sources to create standing wave patterns that can trap and move objects in
106 ser beams that create quasi-periodic optical standing-wave patterns.
107 We used a piezoelectric actuator to create a standing wave perpendicular to the crystal flow, which f
108                       In this method, we use standing-wave phase shifts to move particles or cells in
109 ressure X-ray photoelectron spectroscopy and standing-wave photoemission spectroscopy provides the sp
110               In contrast to familiar energy standing waves, polarization standing waves have constan
111 e vibrations and how they can excite surface standing waves possibly amplified under geometric condit
112 queous media by a combination of an acoustic standing wave pressure field and in situ complex coacerv
113 le argon atoms, traveling through an optical standing wave, produced a periodic array of localized me
114  phase can also be exploited to optimize the standing wave profile in planar devices to maximize ligh
115 pproaches such as coherent absorption from a standing wave promise total dissipation of energy.
116                             Here, we present standing-wave Raman tweezers for stable trapping and sen
117 ficient as low as -45 dB at 4 GHz, a voltage standing wave ratio (VSWR) consistently below 1.5, and a
118                                   Evanescent standing wave (SW) illumination is used to generate a si
119                                 Conventional standing-wave (SW) fluorescence microscopy uses a single
120 n normal visual responses, and both start as standing waves: synchronous elevated activity in the V1
121 In this study, we demonstrate that the X-ray standing wave technique allows the surface polarization
122                                    The X-ray standing wave technique provides the average Ti and Ba a
123 sing an application of the long-period x-ray standing wave technique.
124 oustophoretic device that uses an ultrasonic standing wave to align the blood cells, which exhibit po
125 coustic flow cytometer that uses an acoustic standing wave to focus particles into 16 parallel analys
126 he surface electrodes, confining an acoustic standing wave to the electrode region.
127        We report the first use of ultrasonic standing waves to achieve cell cycle phase synchronizati
128 hip for acoustophoresis utilizing ultrasonic standing waves to focus and orient red blood cells in tw
129 the sound source near the flame or have used standing waves to reach large enough acoustic amplitudes
130                Here we use long-period x-ray standing waves to study the adsorption of mercurated-pol
131 tion wide-field biological imaging by use of standing wave total internal reflection fluorescence (SW
132                                      In most standing-wave traps, however, particles interact via aco
133 eaky waveguide (MCLW) sensor with ultrasound standing waves (USW).
134 characteristics of the accompanying electron standing waves, we are able to distinguish the fluorine
135  controlled, for the application of acoustic standing waves when using live cells and for potential c
136 rces are comparable to those produced from a standing wave, which suggests opportunities for in vivo
137 cident and diffracted waves, which creates a standing wave with nodes at strongly absorbing atoms.
138  reflected from a metallic mirror produces a standing wave with reduced intensity near the reflective
139  of a poro-elastic seabed induced by partial standing waves with arbitrary reflectivity.
140  of pro-grade and retrograde flow rotations, standing waves with zero angular velocities can emerge.
141 terns appear stable, they are the product of standing waves, with auxin flowing through the tissue, m
142                                 Here, we use standing-wave X-ray fluorescence (SWXF) to localize chem
143                    The variable-period x-ray standing wave (XSW) technique is emerging as a powerful

 
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