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1  miniature synchrotron X-ray source (Compact Light Source).
2 1.95 A, from data collected at a synchrotron light source.
3 l cation and the influence of oxygen and the light source.
4 onizing, short-wavelength ultraviolet (UV-C) light source.
5 der transmission spectra using an incoherent light source.
6 rcularity, brightness, and stability of this light source.
7 gnitude higher than that of a LED or thermal light source.
8 objects and the spectrum of the illuminating light source.
9  the excitation wavelength or the excitation light source.
10 ible light irradiation with an artificial Xe light source.
11 g diffraction upon illumination with a white light source.
12  twin electron bunches at the Linac Coherent Light Source.
13 plane array (FPA) detector and a synchrotron light source.
14 ume of brain tissue from a small, point-like light source.
15 th band during illumination with a broadband light source.
16 ed optical elements, including an integrated light source.
17 s bright yellow light when excited by a blue light source.
18 y transverse deflector at the Linac Coherent Light Source.
19 pled to the high brightness of a synchrotron light source.
20 owth toward a noncoherent, uniform intensity light source.
21 y machine, a laser called the Linac Coherent Light Source.
22 e vinyl acetate (EVA) film, and exposed to a light source.
23 ee electron laser, namely the Linac Coherent Light Source.
24  produced by a xenon flash or nitrogen laser light source.
25 ter than when they were exposed to a control light source.
26 d in Maxwellian view using a broadband xenon light source.
27 is, an ability to move in the direction of a light source.
28 Mn were obtained at the National Synchrotron Light Source.
29 rientations, collected at the Linac Coherent Light Source.
30  imaging resolution above 100 nm for a white-light source.
31 d by a smartphone camera under a portable UV light source.
32 coherence tomography with a 200-nm bandwidth light source.
33  phototaxis, i.e. actively orients towards a light source.
34 brightness for a speckle-free and narrowband light source.
35 ectly and accurately sense the position of a light source.
36 order transmission using an incoherent white light source.
37 le wavelength (Se-SAD) at the Linac Coherent Light Source.
38 act accelerator building blocks and advanced light sources.
39 ng an alternative to large-scale synchrotron light sources.
40 echniques enabled by modern short-wavelength light sources.
41 maging methods to harness new coherent x-ray light sources.
42 higher X-ray dose rates expected with future light sources.
43 e of high-brightness xenon and mercury vapor light sources.
44 and simulated and natural solar radiation as light sources.
45 ntities of molecules using widely accessible light sources.
46 ures, as well as compact extreme ultraviolet light sources.
47 tive materials for applications as nanoscale light sources.
48 ges that exploit the unique aspects of these light sources.
49 ly high-powered, faster and smaller coherent light sources.
50 ells, photodetectors, optical modulators and light sources.
51 t X-ray fluxes available on third-generation light sources.
52 icals (NO3) in the presence of the different light sources.
53 properties for future solid-state attosecond light sources.
54 e at depths difficult to reach with external light sources.
55 thod that enables low-repetition-rate pulsed light sources.
56 vanced through the discovery of new, tunable light sources.
57 ience, compact plasma-based accelerators and light sources.
58 ats used to discriminate among infrared (IR) light sources.
59  conditions in combination with intense blue light sources.
60 locks for highly efficient broadband visible lighting sources.
61 onomers) and a low energy visible LED as the light source (1-4.8 W, lambda(max) = 435 nm).
62                         We thus mated an LED light source, a dark-field condenser and a 20x objective
63 d fashion instead of in the direction of the light source, a global force on the system.
64       The integrated system includes a laser light source, a temperature-regulated flow cell encasing
65 oratories is its reliance on high peak-power light sources, a requirement that typically has been met
66 ch lamellar stripes grew toward the incident light source, adopted an orientation parallel to the lig
67  a neutral cue, predicting the location of a light source, affected the direction of plant growth.
68 ridge along with using a camera flash as the light source allows on-site halocarbon detection in seco
69 nt of robust and compact extreme ultraviolet light sources.Although higher harmonic generation from s
70 y transfer as the basis for flexible on-chip light sources, amplifiers, nonreciprocal devices and sig
71 anoribbon that serves both as an unpolarized light source and a dielectric waveguide.
72  integrated with a magnifying lens, a simple light source and a miniaturised immunoassay platform, th
73 r-infrared 860 nm light emitting diode (LED) light source and a wedge depolarizer to create a phase g
74          The CRET platform needs no external light source and avoids autofluorescence and photobleach
75 CRI) of 73 which is similar to a fluorescent light source and correlated color temperature (CCT) of 7
76 e compared with data obtained using the same light source and detector, but a conventional bend-coupl
77             LEDs provide a compact, low cost light source and have been incorporated directly into th
78 ical microlenses, allowing the cell to see a light source and move towards it.
79 optimized sensor head equipped with a UV-LED light source and optical fiber bundles for efficient flu
80 e demonstrate a silicon waveguide-integrated light source and photodetector based on a p-n junction o
81 coherence can be affected by the size of the light source and propagation distance in use.
82 acteria into the focus of the Linac Coherent Light Source and record diffraction patterns from indivi
83 -producible parts, including a semiconductor light source and sensor.
84 lated to the intensity and wavelength of the light source and that oxygen is essential for an efficie
85 rmance was evaluated through a simulated LED light source and the bioluminescence produced by the gen
86 cessing allows reducing the influence of the light source and the positioning of the microfluidic dev
87 ly test these approaches using a synchrotron light source and two commercially available X-ray instru
88  central organic light-emitting diode (OLED) light source and two opposed organic photovoltaic (OPV)
89 In this article, we introduce a standardized light source and validate its usability for PIT applicat
90 were integrated for filtering the excitation light source and, thereby, increasing the contrast of th
91 an extensive range of discrete monochromatic light sources and allows for an examination of the retin
92  applications for example as efficient white light sources and biolabels are reviewed.
93 sma-based accelerators envisioned for future light sources and colliders.
94 olines and enones using convenient household light sources and commercially available Ru(bpy)3Cl2 as
95 ttractive through the use of inexpensive LED light sources and common UV-vis spectrometers, as well a
96 gly popular because of technical advances in light sources and detectors.
97     Implementation typically requires remote light sources and fiber-optic delivery schemes that impo
98 n order to enable future generations of both light sources and high-energy physics experiments.
99            Coherence properties of different light sources and how they affect the image quality of h
100  structure opens for new experiments tunable light sources and LECs with added electronic functionali
101 ternating-current-powered electroluminescent light sources and light-emitting sensing devices.
102  of light propagation, dynamic access to the light sources and material parameters of the system, as
103 lfamethoxazole were irradiated under various light sources and pH conditions.
104                                     Suitable light sources and photo detectors have been selected, an
105                                     However, light sources and photodetectors present ongoing challen
106  Lastly, acne therapies involving the use of light sources and photosensitizers are currently being d
107 The first network, intended for solar cells, light sources and similar devices, has a quasi-fractal s
108  dynamics of both cells' accumulation toward light sources and their dispersion upon light cessation.
109 nstructed from a cell phone camera, a planar light source, and a cardboard box), demonstrate the conc
110  while harvesting its evaporation to power a light source, and a miniature car (weighing 0.1 kg) that
111      The reaction is promoted by any visible light source, and efficient, gram-scale cycloadditions c
112 ted to the awareness of the orientation of a light source, and hence any information presented on a w
113          Using a miniature spectrometer, LED light source, and optical fibers on a rotating benchtop
114 ganic or organic light emitting diode as the light source, and polythiophene: fullerene type bulk-het
115 tions exist even in 'classical'-like thermal light sources, and appear relevant for the implementatio
116 xperiments and measurements of low intensity light sources, and are extensively employed in biologica
117  integration in next-generation electronics, light sources, and biosensors.
118 ovel sensor designs with cheaper and smaller light sources, and consequently increases accessibility
119 onic devices, compact and wavelength-tunable light sources, and micro total analysis systems.
120 s State Park, PA) with minimal anthropogenic light sources, and one city location (Philadelphia, PA).
121 icularly bright mid-infrared (MIR; 3-20 mum) light sources are available offering high spectral brigh
122                           As next-generation light sources are developed, using extreme ultraviolet l
123 e passive optical components, but integrated light sources are limited by silicon's indirect band-gap
124                        At present, entangled-light sources are optically driven with lasers, which ar
125 ticularly at the high brightness synchrotron light sources, are making SXS an important tool for the
126                 Integration of nanostructure lighting source arrays with well-defined emission wavele
127 oscope available at the National Synchrotron Light Source as a high throughput imaging instrument, we
128 y ground hyperspectral imaging of artificial light sources as a complementary method for retrieving f
129 biological laboratories have a wide range of light sources as standard equipment.
130 n fluorescence microscopy, regardless of the light source, as the light power measured can be transla
131 results of a PI-TOF-MS study at the Advanced Light Source at Lawrence Berkeley National Laboratory.
132 l, highly intense, single-particle, coherent light sources at subwavelength scale.
133 on of OCT system, which is a function of the light source bandwidth, is sufficient to resolve retinal
134 e potential for providing tabletop broadband light sources but so far are limited by their low conver
135 hnology not only resulted in efficient white light sources, but continues to enable a host of applica
136 nistic spatiospectral control of a broadband light source by means of wavefront shaping.
137 attered x ray light from a fourth generation light source can be used to detect the modification of t
138                 First, these III-V plasmonic light sources can be directly grown on Si substrates fre
139 demonstrating that existing third generation light sources can significantly enhance the brightness a
140 on of radiation, is recognized as a coherent light source capable of confining optical fields at subw
141 role that molecular oxygen (O2), solvent and light-source (CF lamp or blue LED) play in a variety of
142 e closed by laser-driven compact synchrotron light sources (CLS), which use an infrared (IR) laser ca
143 theoretically possible) opsin properties and light source configurations that would maximise therapeu
144 ters whose interrogation is carried out with light sources, detectors and fibre components readily av
145 enetics in particular, the ability to insert light sources, detectors, sensors, and other components
146  resolution for both incoherent and coherent light sources, different types and sizes of beads, and d
147  (LEDs) are gradually replacing conventional lighting sources due to their advantages in energy savin
148 bursts or continuous waveforms with only the light source, electrical drives/controls and detectors b
149 tion developed for use at the Linac Coherent Light Source enabled efficient and flexible FX experimen
150 ation of optomechanical systems with on-chip light sources feasible.
151 ges and a defined alignment of the observer, light source/fixation target, and subject eye, the subje
152  the tips are illuminated by a monochromatic light source for concurrent spectroscopic detection of t
153 adband radiations as an all-purpose tabletop light source for general applications in science and tec
154  Optical frequency combs are a revolutionary light source for high-precision spectroscopy because of
155 riton laser an attractive low-power coherent light source for medical and biomedical applications or
156 ht-emitting diode (LED) is investigated as a light source for optical detection in chemical analysis.
157 -field optical microscope is utilized as the light source for photolithography, it is possible to fab
158 The novel flower HOPS beams can act as a new light source for photonic applications.
159 is great need to characterize a standardized light source for PIT application.
160 ernment (0.64 microM), using a halogen white light source for the stimulation of algal photosynthetic
161  and medical therapy, university-scale X-ray light sources for biological and materials research, and
162 ue light-emitting diodes are important white light sources for our daily life.
163  light emitting diodes (OLEDs) as excitation light sources for quantum dot-based fluorescent lateral
164 racterize frequency-multiplexed nonclassical light sources for quantum info-communications technology
165 intense X-ray pulses from the Linac Coherent Light Source free-electron laser and compare it with the
166 oherent X-ray pulses from the Linac Coherent Light Source free-electron laser.
167 eated and diagnosed using the Linac Coherent light Source free-electron X-ray laser, tuned to specifi
168 ng up novel opportunities for designs of the light sources, free electron lasers, and high energy col
169  high harmonics as useful broadband tabletop light sources from the extreme ultraviolet to the X-rays
170                            Using appropriate light sources guided by fiber optics, we determined a de
171 d activity upon irradiation with an external light source has provided new tools to target cells for
172                                       Modern light sources have advanced many fields by providing ext
173                                  So far, the light sources have been limited to continuous wave or hi
174 addition to O2, the effects that solvent and light-source have on the dual-catalyzed decarboxylative
175 y the potential of using deep UV-LEDs as the light source in photometric detection for even lower-wav
176 rward, sensitive visualization with a simple light source in resource-limited situations.
177 an epidermal keratinocytes (NHEK) to an FS20 light source in vitro can induce the formation of mitoch
178 emiconductor lasers are widely used, compact light sources in optical communications.
179  are the most powerful and versatile compact light sources in the mid-infrared range, yet achieving t
180 esults suggest a design strategy for quantum light sources in the mid-IR/terahertz: ones that prefer
181 far-field, and behave as arrays of nanoscale light sources in the near-field.
182 ied avian responses to powerful ground-based light sources in urban areas.
183                        Common approaches for light sources include one or few off-chip or wafer-bonde
184 on fluxes and distance dependences of indoor light sources including halogen, incandescent, and compa
185 n the near future as general bright tabletop light sources, including intense attosecond pulses.
186                                  This single light source induced significant behavioral alterations
187 a, a retinal bleaching flash, and a Ganzfeld light source inside a pair of light-obscuring goggles.
188  live cells and function as highly localized light sources inside the cell.
189 stem enables the use of a low-cost broadband light source instead of a bulky and expensive tunable la
190 mental conditions including ultraviolet (UV) light sources, intensity, solution pH, and Cl(2,T) conce
191                                     When the light source is a pulsed laser, water splitting is accom
192                                       Such a light source is also ideal for space communications, bot
193  employing GaN or InGaN chips as the primary light source is explored.
194               A high-resolution image of the light source is focused on the edge of the cell opposite
195 interferometric method means that a coherent light source is not required, making the monolithic inte
196                                     When the light source is removed, and the sample is slowly heated
197 axis tomography scheme is adopted, where the light source is rotated along two orthogonal axes.
198 y, the modulation bandwidth of the plasmonic light-sources is enhanced to significantly higher than c
199 followed by exposure to a laser or broadband light source, is a promising modality for treatment of m
200 The bowel was illuminated with an incoherent light source laparoscope (D-light-P, KarlStorz).
201 e using the full power of the Linac Coherent Light Source (LCLS) and a dose up to 1.3 GGy per crystal
202 sults from experiments at the Linac Coherent Light Source (LCLS) demonstrating that serial femtosecon
203                           The Linac Coherent Light Source (LCLS) is an X-ray source of unmatched bril
204  x-ray pulses produced at the Linac Coherent Light Source (LCLS) were used for simultaneous x-ray dif
205        With the advent of the Linac Coherent Light Source (LCLS) X-ray laser, high-intensity radiatio
206 cond (fs) X-ray pulses of the Linac Coherent Light Source (LCLS), the Ni center electronic configurat
207 -ray free-electron laser, the Linac Coherent Light Source (LCLS).
208 20-Hz repetition rate of the Linear Coherent Light Source (LCLS).
209 a obtained with the Stanford Linear Coherent Light Source (LCLS).
210 e of a complex set-up that involves multiple light sources, lenses or mirrors.
211                              Compact on-chip light sources lie at the heart of practical nanophotonic
212   This technique was evaluated using various light sources, lighting angles, imaging backgrounds, and
213 d with bright, economical, nanosecond-pulsed light sources like flashlamps and nitrogen lasers are an
214 thers the experimental animal to an external light source, limiting the range of possible experiments
215 units conveyed significant information about light-source location, whereas, over a corresponding reg
216                                High harmonic light sources make it possible to access attosecond time
217 tion between those designing new indicators, light sources, microscopes, and computational analyses w
218 ed on a trapezoidal prism for the disposable light source module.
219  domain and Fourier domain devices, and with light sources of different wavelengths.
220 oherence properties are measured for various light sources of diode-pumped solid-state (DPSS) laser,
221                                Non-classical light sources offer a myriad of possibilities in both fu
222 II-V nanolasers as monolithically integrated light source on Si chips due to many advantages.
223 figurable, and low lasing threshold coherent light sources on a chip.
224 s, rendering individually identifiable point light sources on compliant substrates.
225 ues for developing monolithically integrated light-sources on conventional microchips.
226 assive photonic devices for on-chip coherent light sources, optical signal processing, and the invest
227 ed by means of external factors, such as the light source or filters.
228 , there is no need for a pulsed or modulated light source or for additional time-resolved detection.
229 es not use any mechanical elements, external light sources, or reflectarrays, creating, for the first
230 ped at the Materials Science beamline (Swiss Light Source, Paul Scherrer Institute, Switzerland).
231 bedded flash in the cell phone camera as the light source, piped the light with an optical fiber from
232                         A partially coherent light source placed approximately 70 mm away from the se
233                                    Broadband light sources play essential roles in diverse fields, su
234 tages for the use of many directly modulated light sources positioned at the transmitter location.
235 e semiconductor laser (SCL) is the principal light source powering the worldwide optical fiber networ
236  (CO formation); however, conventional (LED) light sources produce water splitting exclusively.
237 f the technique is parallel to that of laser light sources, recent advances have spurred a resurgence
238                       The usage of the SoLux light source represents a new method which enables a con
239  channels with dense arrays of implanted red light sources resulted in successful defibrillation.
240       Because each single fluorophore acts a light source roughly 1 nm in size, microscopic observati
241                                With suitable light sources, s-SNOM is instrumental in numerous discov
242 ence instruments by replacing the excitation light source (short duty cycle rectangular signal instea
243 hat the silica products excited by different light sources show different luminescence properties.
244     Experiments with different monochromatic light sources showed that rus1 phenotypes can be rescued
245 s been to develop an efficient silicon-based light source since indirect band-gap of silicon gives ri
246  essential components of the device like the light source, spectrometer, filters, microcontroller and
247 ation of the MERLIN beamline at the Advanced Light Source storage ring (Berkeley, USA).
248 with the increasing availability of advanced light sources such as quantum cascade lasers and the adv
249                Accordingly, chemiluminescent light sources such as those generated by luciferases hav
250                               In a classical light source, such as a laser, the photon number follows
251                   Modern tuneable high-power light sources, such as free-electron lasers and vacuum t
252          In contrast, traditional incoherent light sources, such as thermal sources or light emitting
253          To overcome this, we demonstrated a light source system having a wide tunability in the spat
254  of a psychophysics procedure with a quantum light source that can generate single-photon states of l
255 ystem with a 1.7 mum center wavelength swept light source that can readily penetrate deeper into the
256                  The development of a robust light source that emits one photon at a time will allow
257 equirements on the temporal coherence of the light source that no longer can be met by current SCLs.
258 ht for a wide range of angles could become a light source that reaches luminous efficiencies ( approx
259           Laser frequency combs are coherent light sources that simultaneously provide pristine frequ
260      Random lasers are a developing class of light sources that utilize a highly disordered gain medi
261 ight, using the flash of the smartphone as a light source, the image captured with the built-in camer
262 lopment of a new generation of compact x-ray light sources, the coherence of which depends directly o
263 y on rigid fiber optics tethered to external light sources, these novel devices carry wirelessly powe
264                         Testing revealed the light source to be safe, easy to use, and independent of
265  can potentially serve as a tunable coherent light source to enable on-chip signal processing for int
266  activity coefficients" (ELAC) for the white light source to generate calibration curves that relate
267 s capable of serving simultaneously as local light source to initiate photo(bio)electrochemical react
268 chnique has been extended from a synchrotron light source to utilise a lab-based microfocus X-ray sou
269 oncentrations of 1 and using a low-intensity light source, to activate the enzyme soluble guanylyl cy
270  high reflectivity mirrors and hence intense light sources (typically lasers) to have enough light tr
271                             The LSPR probing light source used a green light-emitting diode (LED; lam
272 point out shortcomings of the low-resolution light source used in their experiments.
273 igate the nature of correlations in Gaussian light sources used for ghost imaging.
274  driven by a blue (lambda(max) = 472 nm) LED light source using [Ru(bpy)(3)]Cl(2) (bpy = 2,2'-bipyrid
275 ion spectroscopy (XES) at the Linac Coherent Light Source using redox-active Mn complexes.
276 ectures, thus enabling easy manufacturing of light sources using printing tools.
277               Coherent and tunable nanoscale light sources utilizing optical nonlinearities are requi
278 o ligand coadditive) and a readily available light source (UVC compact fluorescent light bulb), a wid
279        To demonstrate utility beyond quantum light sources we show that nanocavity-coupled SWCNTs per
280 unable synchrotron radiation at the Advanced Light Source, we demonstrate the first evidence of nitro
281                                With a single light source, we stimulated channelrhodopsin-2-expressin
282 d x-ray pulses emitted by the Linac Coherent Light Source were used to conduct time-resolved serial f
283                                              Light sources were modelled as synchronously activating
284 termine the safety power level for different light sources when viewing the produced images by human
285 and a third sample was irradiated by a SoLux light source which closely models the solar emission pro
286 -cost laser to realize a compact inexpensive light source, which can ultimately impact many fields of
287 andom walk toward or away from a directional light source, which is sensed by intracellular photorece
288 n of electroluminescence emitters as quantum light sources, which can be studied with high time resol
289 d to the intrinsic spectrum bandwidth of the light source, while spatial coherence can be affected by
290                         We combine a thermal light source with a conventional thermal infrared camera
291  results could pave way to produce low- cost light source with high luminance, using TADF molecules.
292 se of random Raman lasing as a novel imaging light source with unprecedented brightness for a speckle
293 ts on the performances of self-powered PD to light sources with different wavelengths and indicates h
294                                        Other light sources with more intense UV output hold potential
295 tudy explores two approaches for integrating light sources with nuclear magnetic resonance (NMR) spec
296 t of densely integrated, electrically driven light sources with tailored emission properties.
297 tral properties of incoherent supercontinuum light sources with the advantages of cavity ring-down sp
298 nventional lithography, works under ordinary light source without complex optics system, giving rise
299                  The ultimate form of such a light source would be a monolithic white laser.
300 measurements performed at the Linac Coherent Light Source X-ray free-electron laser.

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