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1 ration 4lambda0 (with lambda0 the free-space excitation wavelength).
2 ence of 0.54 J/cm(2) of 653 nm (PpIX optimal excitation wavelength).
3 Raman spectra as a function of tunable laser excitation wavelength.
4 its emission maximum strongly depends on the excitation wavelength.
5 eased, and 15 were variable depending on the excitation wavelength.
6 road range of emission colors using a single excitation wavelength.
7 y of the nanostructures to absorb a specific excitation wavelength.
8 t and its formation is dependent on the pump excitation wavelength.
9 rformance strongly varied in function of the excitation wavelength.
10 es of different origins and do not vary with excitation wavelength.
11 s greatly between samples and decreases with excitation wavelength.
12 ple spectral windows to be accessed with one excitation wavelength.
13 ximately 80 fs time scale independent of the excitation wavelength.
14 ssion shifted toward the red with increasing excitation wavelength.
15 eporter molecule and its corresponding laser excitation wavelength.
16            Thus, the processes depend on the excitation wavelength.
17 h depend on quencher gas pressure but not on excitation wavelength.
18 bstrate at the surface plasmon angle for the excitation wavelength.
19 al confinement of dimerization with a single excitation wavelength.
20 ously detected two cellular targets with one excitation wavelength.
21 ss the entire visible spectrum by tuning the excitation wavelength.
22     The emission spectra were independent of excitation wavelength.
23  strong and consistent fluorescence under an excitation wavelength.
24 ing with 4-20 ps lifetimes, independently of excitation wavelength.
25 between these pathways are influenced by the excitation wavelength.
26 a sufficiently high sample absorption at the excitation wavelength.
27 -RC is Phe, rather than P(D1), regardless of excitation wavelength.
28 alyzed using Raman spectroscopy with 1064 nm excitation wavelength.
29 orescence sensing using a single ultraviolet excitation wavelength.
30 te to the observed emission even at a single excitation wavelength.
31 parent quantum efficiency of 8.9 % at 420 nm excitation wavelength.
32 he compounds to be analyzed by adjusting the excitation wavelength.
33  variation of the absorber thickness and the excitation wavelength.
34 nced light absorption in the graphene at the excitation wavelength.
35 ssions could be generated by controlling the excitation wavelength.
36 , with the NLO absorption insensitive to the excitation wavelength.
37 ing the near-field enhancement at a specific excitation wavelength.
38 intermediate chain), surface coverage, laser excitation wavelength.
39  unusual mixed emission that is dependent on excitation wavelength.
40 and composition of the nanostructure and the excitation wavelength.
41 ith SERS microspectroscopy at a single laser excitation wavelength.
42 of the solar cell may likewise depend on the excitation wavelength.
43 revealed a flecked fundus AF pattern at both excitation wavelengths.
44  calculation of penetration depth at various excitation wavelengths.
45 uded in the optimization process three laser excitation wavelengths.
46 line, to be established over a wide range of excitation wavelengths.
47 emissions by tuning the doping levels and UV excitation wavelengths.
48 hanges in the coherence spectra at different excitation wavelengths.
49 om the red to greenish-blue as a function of excitation wavelengths.
50 s as high as 0.31 were achieved using 532-nm excitation wavelengths.
51  to temperature, solvent, concentration, and excitation wavelengths.
52 er (CO-bound or NH-bound) with different SEP excitation wavelengths.
53  spectra of cofactors NAD(P)H and FAD at all excitation wavelengths.
54 ansfer was observed by a proper selection of excitation wavelengths.
55 r resonance Raman (rR) spectra at particular excitation wavelengths.
56 ulatus have been obtained using a variety of excitation wavelengths.
57 e-photon imaging typically requires multiple excitation wavelengths.
58  fluorescence emission across UV and visible excitation wavelengths.
59 pectra with a single combination of discrete excitation wavelengths.
60 ues compared to SRNOM and other pyDOM at all excitation wavelengths.
61 re determined by the evaluation of different excitation wavelengths.
62 ximum emission, depending on temperature and excitation wavelengths.
63 diffusive scattering techniques with varying excitation wavelengths.
64 ectral profile of the sensors toward desired excitation wavelengths.
65 1 muM was detected, whereas the pre-resonant excitation wavelength 244 nm provides an LoD of 6.9 muM.
66                                          The excitation wavelength (250 nm) and emission wavelength (
67  of virgin and irradiated sample recorded at excitation wavelength 270 to 310 nm.
68 hy coupled to a fluorescence detector at the excitation wavelength 335 nm and the emission wavelength
69 the use of different, potentially orthogonal excitation wavelengths (365, 405, and 760 nm) for the se
70 e present study, kinetic measurements at two excitation wavelengths (395 nm and 460 nm) on either sid
71     Data have been obtained for two distinct excitation wavelengths, 400 nm at the edge of the UV gam
72              Furthermore, the impact of four excitation wavelengths 405, 532, 633, and 785 nm is inve
73 ses a custom-built flow cytometer with three excitation wavelengths (405 nm, 488 nm, and 633 nm) and
74 rat liver mitochondria were examined with an excitation wavelength (413.1 nm) in resonance with the S
75 triarylamine) helicene molecules by using an excitation wavelength (457 nanometers) in the vicinity o
76                               Using a single excitation wavelength (488 nm) we acquired images from t
77 -AF; 200 degrees : ultrawide-field, UWF-AF), excitation wavelength (488 nm, blue/SW-AF; 532 nm, UWF-A
78 airs between the donor and acceptor, and the excitation wavelength (488 or 514 nm).
79 tudinally with fundus autofluorescence (FAF; excitation wavelength, 488 nm; emission wavelength, >500
80 tical imaging (emission wavelength = 600 nm, excitation wavelength = 500 nm) revealed that the fluore
81 f 19 ns and a high initial anisotropy at two excitation wavelengths, 505 and 690 nm.
82 pectral quality is evaluated using two Raman excitation wavelengths (532 and 785 nm) as these are cri
83 successfully balanced by using two different excitation wavelengths: 550 nm for high quantum-yield fl
84 pool agents optimized for two nonoverlapping excitation wavelengths (680 and 750 nm).
85       In this study, we use a broad range of excitation wavelengths (730-880 nm) to demonstrate that
86 (3+), Tm(3+), and Ho(3+)) at a biocompatible excitation wavelength (795 nm) and also significantly mi
87  for measurements on pigmented skin lesions (excitation wavelength 976 nm and a wavelength range of t
88 nd downshifted luminescence across different excitation wavelengths (980, 800, and 658 nm), with negl
89                           Independent of the excitation wavelength, a long-lived (>450 mus) photoprod
90  outperforms its parent in mice and flies at excitation wavelengths above 1,000 nm and enables improv
91 years that would efficiently transform using excitation wavelengths above 350 nm remains a challenge
92                      The range of one-photon excitation wavelengths afforded by these new VSDs spans
93        Multiple series of Pdots with varying excitation wavelengths allow for fast (<1 minute) and si
94  The optimization of solution parameters and excitation wavelengths allows SNAFR-1 to display red, gr
95 arriers is not significantly affected by the excitation wavelength, although this changes the fractio
96 f (1)O2 production as a function of incident excitation wavelength, analysis of X-ray diffraction dat
97  the MC strategy allows modifications in the excitation wavelength and absorptivity through the appro
98 exhibiting significant polarization near the excitation wavelength and becoming mostly depolarized ov
99 NEP-chromophore styryl dyes as a function of excitation wavelength and dye structure.
100  signal and signal-to-noise ratio at various excitation wavelength and emission filter combinations u
101             Prepared S,N-GQDs showed maximum excitation wavelength and emission wavelength at 400 and
102 signed to provide optical resonances for the excitation wavelength and emission wavelength of Cy5, wa
103 signed to provide optical resonances for the excitation wavelength and emission wavelength of Cyanine
104 nanostructures cannot cover both fundamental excitation wavelength and harmonic generation wavelength
105 llular four-color multiplexing with a single excitation wavelength and in situ assembly and FRET to m
106 dene)benzohydrazide (BHN) exhibited stimuli (excitation wavelength and pH) induced changes in fluores
107 nd photocurrent experiments as a function of excitation wavelength and temperature for two low-band-g
108 t supports Bloch surface waves (BSWs) at the excitation wavelength and the bottom segment serves as a
109  for deep-tissue imaging because of the long excitation wavelength and the high nonlinear confinement
110                  The combination of the long excitation wavelength and the higher order nonlinear exc
111 fetime images obtained with FLIM at a single excitation wavelength and using a single broad band emis
112                   Fluorescence spectra at 11 excitation wavelengths and a reflectance spectrum were a
113                            By using multiple excitation wavelengths and by carefully examining the be
114  spectrally uniform enhancement for multiple excitation wavelengths and for different shifts enables
115      The line scans performed with different excitation wavelengths and hence different information d
116 t the scores of fluorescence EEMs with seven excitation wavelengths and over 1000 emission wavelength
117 ichment and the prerequisite use of multiple excitation wavelengths and similar flocculation or depos
118 rect excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the
119 ERS performance is strongly dependent on the excitation wavelengths and the molecule types.
120   We demonstrate this principle by using two excitation wavelengths and three fluidic channels to imp
121  population of the states is dictated by the excitation wavelength (and not primarily by temperature)
122 roscopy in full spectral (60 emission and 34 excitation wavelengths) and chromatographic resolution (
123 iplexing with a single measurement, a single excitation wavelength, and a single FRET pair allowed fo
124 of nanoparticle material, nanoparticle size, excitation wavelength, and capping agents on the perform
125 an internal standard requiring only a single excitation wavelength, and is much reduced in size (<20
126  distance between QDs and silver resonators, excitation wavelength, and QD film thickness.
127            The effects of sample morphology, excitation wavelength, and temperature are examined.
128 absorption spectra, fluorescence anisotropy, excitation wavelength, and temperature dependence of the
129 uding the nature of the SERRS substrate, the excitation wavelength, and the dye chosen.
130 f incident angle was measured using a 785-nm excitation wavelength, and was compared to the Raman pea
131 ffective Stokes shift (115-260 nm), multiple excitation wavelengths, and narrow, tunable deep-red/nea
132  and orthogonal responses to temperature and excitation wavelength are achieved by confining the stim
133 ne set of Raman measurements at one specific excitation wavelength are effective for correcting fluor
134  a fluorescent probe, and the broad range of excitation wavelengths are advantageous over other genet
135                                Two different excitation wavelengths are used to distinguish the super
136 proteins are the brightest and what the best excitation wavelengths are.
137  Raman spectra were acquired, using a 532 nm excitation wavelength as the protein samples were heated
138 easured in the range of 400-600 nm using the excitation wavelength at 375 nm.
139 ity of 3 x 10(11) cm Hz(1/2) W(-1) at 514-nm excitation wavelength at a modulation frequency of 90 Hz
140 onship; i.e., the fluorescence emission with excitation wavelength at either 350 or 504 nm decreased
141  vacuolic pH values was determined using DUV excitation wavelengths at 244 and 257 nm.
142                                              Excitation wavelengths at 244 and 532 nm were used to en
143  pH 7.5 and 10.5 has been investigated using excitation wavelengths between 406 and 676 nm, and vibra
144 GTA, and azid-1, are studied in the range of excitation wavelengths between 700 and 800 nm.
145 r o-phthaldialdehyde-labeled glutamate using excitation wavelengths between 965 and 1012 nm.
146                                     For each excitation wavelength, between 250 and 400 nm (4.9-3.1 e
147 hrome c obtained by resonance SIRM at 532 nm excitation wavelength can be successfully complemented b
148 nitoring oxidation at both 396 and 510 nm of excitation wavelengths can facilitate the more selective
149 ing sensorFRET, fail at specific fluorophore-excitation wavelength combinations.
150           We performed an emission scan at 9 excitation wavelengths common to fluorescent microscopy
151 design of biocompatible systems operating at excitation wavelengths compatible for biomedical applica
152 ied by rate constants, and may depend on the excitation wavelength contrary to slower photochemical p
153 y decrease as the reentry stabilizes and the excitation wavelength decreases.
154 rboxylation reaction strongly depends on the excitation wavelength, decreasing in the order 254 nm >
155 ity, hopping radius and lifetime varies with excitation wavelength, decreasing with increasing energy
156                              By shifting the excitation wavelength deep into the NIR, both NIR one-ph
157                                          The excitation wavelength dependence (action spectrum) was m
158  polarity, number of linked CT entities, and excitation wavelength dependence in governing the lifeti
159                                          The excitation wavelength dependence of (1)O(2) generation f
160  a theoretical and experimental study of the excitation wavelength dependence of the entangled two-ph
161                              By studying the excitation wavelength dependence of the time-resolved EP
162  a few to hundreds of picoseconds and strong excitation-wavelength dependence of emission spectra, in
163 ide through a hydrothermal reaction displays excitation-wavelength dependence of PL.
164 egation behavior at higher concentration and excitation wavelength dependent multicolor emission prop
165 phosphorescence versus fluorescence that are excitation wavelength dependent.
166 n transfer (ESIPT) organic luminophores with excitation wavelength-dependent color tunability have dr
167                                              Excitation wavelength-dependent electron injection, intr
168 hibits a very high quantum yield (QY = 78%), excitation wavelength-dependent emission, and upconversi
169  The first two components represent strongly excitation wavelength-dependent energy equilibration pro
170 ajority of the current CDots to date exhibit excitation-wavelength-dependent emissions with their max
171                                          The excitation-wavelength-dependent localization of carriers
172                               Using a single excitation wavelength dual colour FLIM method we are abl
173   In addition to their commonly used visible excitation wavelengths, essentially all FPs can be excit
174 o choosing the right fluorescent protein and excitation wavelength for two-photon applications.
175 ical systems and provides for more favorable excitation wavelengths for fluorescence applications.
176 rganic frameworks (An-MOFs) as a function of excitation wavelength, for the first time.
177 f the Os-ligand complex to be used as a long excitation wavelength FPI probe for potential use in hom
178 red and green emissions, simply by adjusting excitation wavelength from 980 to 808 nm.
179 end the capabilities of FDS-SV with a single excitation wavelength from single-component to multi-com
180  readout of fluorescence evoked by different excitation wavelengths from a single photoreceiver signa
181  (p-FRET) uses a simultaneous combination of excitation wavelengths from two orthogonally polarized s
182 mer with identical constituents at different excitation wavelengths, from the near-infrared up to the
183 gh variations in concentration, solvent, and excitation wavelength, further accentuates the uniquenes
184 de probes labeled with such dyes by using an excitation wavelength has been used to simultaneously me
185 illumination intensity distributions for all excitation wavelengths have a maximum deviation approxim
186 the redshift takes place with respect to the excitation wavelength i.e., melanoma (18 nm), BCC (23 nm
187 ent absorption spectroscopy as a function of excitation wavelength in A. vinosum membranes.
188 using Raman scattering techniques with laser excitation wavelengths in the range from 514.5 to 1320 n
189  presented previously but was limited due to excitation wavelengths in the UV.
190 shifts in the resultant chromaticity with an excitation wavelength including the generation of white
191 ed from data on the 100 ps scale are largely excitation wavelength independent.
192 ta demonstrate that selecting an appropriate excitation wavelength is a key factor for extracting str
193 relative intensities on the binding site and excitation wavelength is found.
194 cy filtering (WIFF) whereby the fluorescence excitation wavelength is modulated across the absorption
195  C[double bond]C stretches) increases as the excitation wavelength is shifted from 570 to 450 nm wher
196 beled with CFP and YFP by choosing different excitation wavelengths is used to identify the compositi
197 igned by using fluorophores with the desired excitation wavelength lambda(ex).
198 according to hole periodicity, diameter, and excitation wavelength (lambda(SPR)).
199 ighly focused two-photon (2P) irradiation at excitation wavelength (lambdaex) 700 nm.
200                    By employing the resonant excitation wavelengths lambdaexc = 244 nm and lambdaexc
201         However, the limited tissue-depth of excitation wavelengths limits their clinical applicabili
202 otein is that our construct can be used when excitation wavelengths lower than 488nm are not availabl
203             Our results show that at shorter excitation wavelengths (&lt;800 nm), the signal emitted fro
204 ibitor containing a fluorescent moiety whose excitation wavelengths match the emission wavelengths of
205                                          The excitation wavelength maxima for 2-AP within these conte
206                             Hence, different excitation wavelengths may preferentially activate one c
207 rescent particles relative to their incident excitation wavelengths, Mie scatter conditions were obse
208 itation of this pair by a single multiphoton excitation wavelength (MPE, 850 nm) yields well-separabl
209 iments afford the ability to finely tune the excitation wavelength near the molecular resonance of R6
210 ilon-ADPR was detected by fluorescence at an excitation wavelength of 230 nm and an emission waveleng
211 mly on the Al nanoparticle arrays at a laser excitation wavelength of 257.2 nm.
212                                           An excitation wavelength of 290 nm was selected and three d
213 nce emission was observed at ~380 nm with an excitation wavelength of 300 nm.
214 rving the increase in fluorescence, using an excitation wavelength of 360 nm, and measuring emission
215  The fluorometric assay is carried out at an excitation wavelength of 380 nm to eliminate the backgro
216  spores appeared as white-yellow ovals at an excitation wavelength of 395 to 415 nm used for viewing
217                                           An excitation wavelength of 405 nm was used to obtain emiss
218 scence emission intensity at 550 nm using an excitation wavelength of 470 nm.
219 resced bright yellow-green when viewed at an excitation wavelength of 470 to 490 nm, whereas live spo
220 tion (LOD) of ~247 pg mL(-1); however, at an excitation wavelength of 532 nm, it provided a LOD of ~6
221 ne Raman signal is resonantly enhanced at an excitation wavelength of 532 nm, providing a convenient,
222 and level of fluorescence polarization at an excitation wavelength of 595 nm and an emission waveleng
223  unsectioned tissue biopsies at a two-photon excitation wavelength of 780 nm.
224  spectral range of 3250-250 cm(-1), using an excitation wavelength of 785 nm, and several bands have
225 id fiber probe-based Raman technique with an excitation wavelength of 785 nm, which is applied to cla
226 fiber-probe-based Raman spectroscopy with an excitation wavelength of 785 nm, which was applied to in
227 e observed peak conversion efficiency at the excitation wavelength of approximately 780 nm indicates
228                                 However, the excitation wavelength of conPET systems mainly focused o
229 igned to provide an optical resonance at the excitation wavelength of cyanine-5 (Cy5), thus providing
230                                  Engineering excitation wavelength of photosensitizers (PSs) for enha
231 hape, fluorophore/particle distance, and the excitation wavelength of the coupling photosensitizer, w
232 let resonance Raman (UVRR) spectroscopy with excitation wavelengths of 257, 244, 238, and 229 nm.
233 UVRR) spectra of fd have been obtained using excitation wavelengths of 257, 244, 238, and 229 nm.
234 ast square discriminant analysis (PLS-DA) at excitation wavelengths of 270, 290, and 430 nm.
235 at grating periods of 925 nm and 1250 nm for excitation wavelengths of 633 nm and 850 nm, respectivel
236 /- 0.6) x 10(8) with maximum enhancement for excitation wavelengths of 785 nm and lower energy.
237 le, near-infrared Raman systems operating at excitation wavelengths of either 785 nm or 1064 nm, coll
238 on and with little apparent phototoxicity at excitation wavelengths of from 930 to 990 nm.
239 ress the influence of antenna morphology and excitation wavelength on polarization conversion efficie
240 erimental data on the effect of changing the excitation wavelength on the ROA spectra of a protein.
241 i3N4 nanowires can be changed along with the excitation wavelength or the excitation light source.
242 c VT activation and exhibited attenuation of excitation wavelength (P<0.001).
243  oxygen production is shown to depend on the excitation wavelength, particularly in a viscous medium.
244 cies of serotonin is identified using pH and excitation wavelength perturbation.
245                                     At given excitation wavelengths, photochemical homolysis rate con
246 green, distinct channels with well-separated excitation wavelengths provide non-invasive video-rate i
247 rgy transfer (ET) processes as a function of excitation wavelength, providing a novel pathway for ET
248  2D grid pattern algorithm to switch between excitation wavelengths quickly, we show volume rates as
249 on wavelength range of 485-580 nm and in the excitation wavelength range of 363-475 nm.
250  when the LSPR band is blue-shifted from the excitation wavelength rather than at the on-resonance po
251 hree probes were originally designed as dual excitation wavelength-ratiometric probes, with high phot
252 , or photoluminescence) as a function of the excitation wavelength resulted in photoswitch-directed t
253 e, the "filter" appears or disappears at the excitation wavelength resulting in the fluorescence turn
254 lysis to the emission spectra acquired after excitation wavelengths set at 270, 290, and 430 nm, a cl
255 ) reveals strong photoactivated emission for excitation wavelengths shorter than 520 nanometers.
256 urements as a function of incident angle and excitation wavelength show the existence of both surface
257                                     The same excitation wavelength simultaneously populates a higher
258                                     Choosing excitation wavelengths so that excitation ratios were co
259 aining brighter polymethine dyes with varied excitation wavelengths spaced throughout the near-infrar
260  AMD eyes, however, both the 364- and 488-nm excitation wavelengths stimulated substantial blue-green
261 mplications for deductions drawn from single-excitation-wavelength studies of the photochemistry of s
262         For a three-photon process, a longer excitation wavelength such as those common in optical co
263 tic behavior with emissions dependent on the excitation wavelengths suggesting anti-Kasha behavior.
264 , peak fluorescence occurs at 483 nm for all excitation wavelengths, suggesting a common emissive sta
265 upling strength shows a strong dependence on excitation wavelengths, suggesting the state-specific dy
266 ial or lateral resolution compared to single-excitation-wavelength SW microscopy.
267  find a dependence of voltage sensitivity on excitation wavelength that is consistent with a two-phot
268 ectrum, lifetimes, and quantum yield (QY) on excitation wavelength that is particularly pronounced in
269 erous multicolor applications using a single-excitation wavelength that was not possible before.
270 olycycle system, greatly extend the range of excitation wavelengths that can be used for fluorescence
271                  However, the specific solar excitation wavelengths that drive photodissolution remai
272 HG and TPEF from collagen, whereas at longer excitation wavelengths the ECM signal is exclusively due
273                              When tuning the excitation wavelength, the distribution changes in both
274                               With increased excitation wavelength, the emission maximum shifted towa
275  heavy-atom-free photosensitizers have short excitation wavelengths, thereby hampering their biomedic
276 d by affixing a fluorophore with the desired excitation wavelength to the Cbl-bioagent conjugate.
277 ogenated matrixes requires adjustment of the excitation wavelength to values below that of the standa
278 low values we used different combinations of excitation wavelengths to determine which could be used
279 ields must be precisely matched between FRET excitation wavelengths to isolate dynamic interactions b
280 s the light source, enabling a wide range of excitation wavelengths to support flexible development o
281  Gamma, decreases from unity (at the longest excitation wavelengths) to zero at short wavelengths.
282  in concentration, solvent, temperature, and excitation wavelength tune the luminescence energy of bo
283           Furthermore, we demonstrate single excitation wavelength two-colour Ca(2+) and glutamate im
284 tween the UV absorptivity of the tags at the excitation wavelengths typical for UV-MALDI and the magn
285 h an aspect ratio of 3.3 to match the 785 nm excitation wavelength used in the SERS studies.
286 ed with catalysis were very dependent on the excitation wavelength used to monitor the reaction.
287 spillover of di-8-ANEPPS fluorescence at the excitation wavelengths used for fura-2 (340 and 360 nm).
288 trix, we first investigated the influence of excitation wavelength, varied between 2.7 and 3.1 mum, a
289 d an approximate linear decrease with longer excitation wavelength was observed.
290                                   A range of excitation wavelengths was tested to detect the particip
291 cident light, while light scattering (at the excitation wavelength) was still present and behaved sim
292                       Merely by changing the excitation wavelength, we could specifically excite eith
293           By using appropriate near-infrared excitation wavelengths, we detect strong transient absor
294 the same field with multiple combinations of excitation wavelengths, we obtain data representing diff
295 ably strong resonance enhancement across the excitation wavelengths when the excitation polarization
296 est that (3)DOM quantum yields decrease with excitation wavelength, which gives rise to the Phi(1O2)
297 and frequency mixing across a broad range of excitation wavelengths, which cannot be achieved with na
298 ng features comparable to or larger than the excitation wavelength, while E-CARS allows detection of
299 a mode that appears near 32-33 cm(-1) at all excitation wavelengths, with a phase that is consistent
300 d from deep blue to red, just by varying the excitation wavelength without changing its chemical comp

 
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