ライフサイエンスコーパス: excitation wavelength

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 ss the entire visible spectrum by tuning the excitation wavelength.

4 t and its formation is dependent on the pump excitation wavelength.

5 rformance strongly varied in function of the excitation wavelength.

6 es of different origins and do not vary with excitation wavelength.

7 s greatly between samples and decreases with excitation wavelength.

8 ple spectral windows to be accessed with one excitation wavelength.

9 ximately 80 fs time scale independent of the excitation wavelength.

10 ssion shifted toward the red with increasing excitation wavelength.

11 eporter molecule and its corresponding laser excitation wavelength.

12 he compounds to be analyzed by adjusting the excitation wavelength.

13 h depend on quencher gas pressure but not on excitation wavelength.

14 bstrate at the surface plasmon angle for the excitation wavelength.

15 ously detected two cellular targets with one excitation wavelength.

16 variation of the absorber thickness and the excitation wavelength.

17 The emission spectra were independent of excitation wavelength.

18 nced light absorption in the graphene at the excitation wavelength.

19 strong and consistent fluorescence under an excitation wavelength.

20 , with the NLO absorption insensitive to the excitation wavelength.

21 ing the near-field enhancement at a specific excitation wavelength.

22 intermediate chain), surface coverage, laser excitation wavelength.

23 unusual mixed emission that is dependent on excitation wavelength.

24 and composition of the nanostructure and the excitation wavelength.

25 ith SERS microspectroscopy at a single laser excitation wavelength.

26 of the solar cell may likewise depend on the excitation wavelength.

27 Raman spectra as a function of tunable laser excitation wavelength.

28 its emission maximum strongly depends on the excitation wavelength.

29 eased, and 15 were variable depending on the excitation wavelength.

30 road range of emission colors using a single excitation wavelength.

31 y of the nanostructures to absorb a specific excitation wavelength.

32 uded in the optimization process three laser excitation wavelengths.

33 line, to be established over a wide range of excitation wavelengths.

34 emissions by tuning the doping levels and UV excitation wavelengths.

35 ximum emission, depending on temperature and excitation wavelengths.

36 hanges in the coherence spectra at different excitation wavelengths.

37 om the red to greenish-blue as a function of excitation wavelengths.

38 s as high as 0.31 were achieved using 532-nm excitation wavelengths.

39 to temperature, solvent, concentration, and excitation wavelengths.

40 er (CO-bound or NH-bound) with different SEP excitation wavelengths.

41 spectra of cofactors NAD(P)H and FAD at all excitation wavelengths.

42 ansfer was observed by a proper selection of excitation wavelengths.

43 r resonance Raman (rR) spectra at particular excitation wavelengths.

44 ulatus have been obtained using a variety of excitation wavelengths.

45 diffusive scattering techniques with varying excitation wavelengths.

46 ectral profile of the sensors toward desired excitation wavelengths.

47 revealed a flecked fundus AF pattern at both excitation wavelengths.

48 calculation of penetration depth at various excitation wavelengths.

49 The excitation wavelength (250 nm) and emission wavelength (

50 hy coupled to a fluorescence detector at the excitation wavelength 335 nm and the emission wavelength

51 the use of different, potentially orthogonal excitation wavelengths (365, 405, and 760 nm) for the se

52 e present study, kinetic measurements at two excitation wavelengths (395 nm and 460 nm) on either sid

53 Data have been obtained for two distinct excitation wavelengths, 400 nm at the edge of the UV gam

54 rat liver mitochondria were examined with an excitation wavelength (413.1 nm) in resonance with the S

55 triarylamine) helicene molecules by using an excitation wavelength (457 nanometers) in the vicinity o

56 Using a single excitation wavelength (488 nm) we acquired images from t

57 airs between the donor and acceptor, and the excitation wavelength (488 or 514 nm).

58 tudinally with fundus autofluorescence (FAF; excitation wavelength, 488 nm; emission wavelength, >500

59 tical imaging (emission wavelength = 600 nm, excitation wavelength = 500 nm) revealed that the fluore

60 f 19 ns and a high initial anisotropy at two excitation wavelengths, 505 and 690 nm.

61 pectral quality is evaluated using two Raman excitation wavelengths (532 and 785 nm) as these are cri

62 successfully balanced by using two different excitation wavelengths: 550 nm for high quantum-yield fl

63 pool agents optimized for two nonoverlapping excitation wavelengths (680 and 750 nm).

64 In this study, we use a broad range of excitation wavelengths (730-880 nm) to demonstrate that

65 (3+), Tm(3+), and Ho(3+)) at a biocompatible excitation wavelength (795 nm) and also significantly mi

66 for measurements on pigmented skin lesions (excitation wavelength 976 nm and a wavelength range of t

67 nd downshifted luminescence across different excitation wavelengths (980, 800, and 658 nm), with negl

68 The range of one-photon excitation wavelengths afforded by these new VSDs spans

69 The optimization of solution parameters and excitation wavelengths allows SNAFR-1 to display red, gr

70 arriers is not significantly affected by the excitation wavelength, although this changes the fractio

71 f (1)O2 production as a function of incident excitation wavelength, analysis of X-ray diffraction dat

72 the MC strategy allows modifications in the excitation wavelength and absorptivity through the appro

73 exhibiting significant polarization near the excitation wavelength and becoming mostly depolarized ov

74 NEP-chromophore styryl dyes as a function of excitation wavelength and dye structure.

75 signal and signal-to-noise ratio at various excitation wavelength and emission filter combinations u

76 signed to provide optical resonances for the excitation wavelength and emission wavelength of Cy5, wa

77 signed to provide optical resonances for the excitation wavelength and emission wavelength of Cyanine

78 nanostructures cannot cover both fundamental excitation wavelength and harmonic generation wavelength

79 nd photocurrent experiments as a function of excitation wavelength and temperature for two low-band-g

80 t supports Bloch surface waves (BSWs) at the excitation wavelength and the bottom segment serves as a

81 The combination of the long excitation wavelength and the higher order nonlinear exc

82 fetime images obtained with FLIM at a single excitation wavelength and using a single broad band emis

83 Fluorescence spectra at 11 excitation wavelengths and a reflectance spectrum were a

84 By using multiple excitation wavelengths and by carefully examining the be

85 spectrally uniform enhancement for multiple excitation wavelengths and for different shifts enables

86 ichment and the prerequisite use of multiple excitation wavelengths and similar flocculation or depos

87 rect excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the

88 We demonstrate this principle by using two excitation wavelengths and three fluidic channels to imp

89 population of the states is dictated by the excitation wavelength (and not primarily by temperature)

90 roscopy in full spectral (60 emission and 34 excitation wavelengths) and chromatographic resolution (

91 of nanoparticle material, nanoparticle size, excitation wavelength, and capping agents on the perform

92 an internal standard requiring only a single excitation wavelength, and is much reduced in size (<20

93 distance between QDs and silver resonators, excitation wavelength, and QD film thickness.

94 The effects of sample morphology, excitation wavelength, and temperature are examined.

95 absorption spectra, fluorescence anisotropy, excitation wavelength, and temperature dependence of the

96 uding the nature of the SERRS substrate, the excitation wavelength, and the dye chosen.

97 f incident angle was measured using a 785-nm excitation wavelength, and was compared to the Raman pea

98 ffective Stokes shift (115-260 nm), multiple excitation wavelengths, and narrow, tunable deep-red/nea

99 ne set of Raman measurements at one specific excitation wavelength are effective for correcting fluor

100 a fluorescent probe, and the broad range of excitation wavelengths are advantageous over other genet

101 Two different excitation wavelengths are used to distinguish the super

102 proteins are the brightest and what the best excitation wavelengths are.

103 Raman spectra were acquired, using a 532 nm excitation wavelength as the protein samples were heated

104 easured in the range of 400-600 nm using the excitation wavelength at 375 nm.

105 ity of 3 x 10(11) cm Hz(1/2) W(-1) at 514-nm excitation wavelength at a modulation frequency of 90 Hz

106 onship; i.e., the fluorescence emission with excitation wavelength at either 350 or 504 nm decreased

107 pH 7.5 and 10.5 has been investigated using excitation wavelengths between 406 and 676 nm, and vibra

108 GTA, and azid-1, are studied in the range of excitation wavelengths between 700 and 800 nm.

109 r o-phthaldialdehyde-labeled glutamate using excitation wavelengths between 965 and 1012 nm.

110 For each excitation wavelength, between 250 and 400 nm (4.9-3.1 e

111 hrome c obtained by resonance SIRM at 532 nm excitation wavelength can be successfully complemented b

112 nitoring oxidation at both 396 and 510 nm of excitation wavelengths can facilitate the more selective

113 ing sensorFRET, fail at specific fluorophore-excitation wavelength combinations.

114 We performed an emission scan at 9 excitation wavelengths common to fluorescent microscopy

115 design of biocompatible systems operating at excitation wavelengths compatible for biomedical applica

116 ied by rate constants, and may depend on the excitation wavelength contrary to slower photochemical p

117 y decrease as the reentry stabilizes and the excitation wavelength decreases.

118 rboxylation reaction strongly depends on the excitation wavelength, decreasing in the order 254 nm >

119 ity, hopping radius and lifetime varies with excitation wavelength, decreasing with increasing energy

120 The excitation wavelength dependence (action spectrum) was m

121 By studying the excitation wavelength dependence of the time-resolved EP

122 a few to hundreds of picoseconds and strong excitation-wavelength dependence of emission spectra, in

123 ide through a hydrothermal reaction displays excitation-wavelength dependence of PL.

124 egation behavior at higher concentration and excitation wavelength dependent multicolor emission prop

125 phosphorescence versus fluorescence that are excitation wavelength dependent.

126 Excitation wavelength-dependent electron injection, intr

127 hibits a very high quantum yield (QY = 78%), excitation wavelength-dependent emission, and upconversi

128 The first two components represent strongly excitation wavelength-dependent energy equilibration pro

129 ajority of the current CDots to date exhibit excitation-wavelength-dependent emissions with their max

130 The excitation-wavelength-dependent localization of carriers

131 Using a single excitation wavelength dual colour FLIM method we are abl

132 In addition to their commonly used visible excitation wavelengths, essentially all FPs can be excit

133 o choosing the right fluorescent protein and excitation wavelength for two-photon applications.

134 ical systems and provides for more favorable excitation wavelengths for fluorescence applications.

135 f the Os-ligand complex to be used as a long excitation wavelength FPI probe for potential use in hom

136 end the capabilities of FDS-SV with a single excitation wavelength from single-component to multi-com

137 (p-FRET) uses a simultaneous combination of excitation wavelengths from two orthogonally polarized s

138 mer with identical constituents at different excitation wavelengths, from the near-infrared up to the

139 illumination intensity distributions for all excitation wavelengths have a maximum deviation approxim

140 ent absorption spectroscopy as a function of excitation wavelength in A. vinosum membranes.

141 using Raman scattering techniques with laser excitation wavelengths in the range from 514.5 to 1320 n

142 presented previously but was limited due to excitation wavelengths in the UV.

143 shifts in the resultant chromaticity with an excitation wavelength including the generation of white

144 ed from data on the 100 ps scale are largely excitation wavelength independent.

145 ta demonstrate that selecting an appropriate excitation wavelength is a key factor for extracting str

146 relative intensities on the binding site and excitation wavelength is found.

147 C[double bond]C stretches) increases as the excitation wavelength is shifted from 570 to 450 nm wher

148 beled with CFP and YFP by choosing different excitation wavelengths is used to identify the compositi

149 igned by using fluorophores with the desired excitation wavelength lambda(ex).

150 according to hole periodicity, diameter, and excitation wavelength (lambda(SPR)).

151 ighly focused two-photon (2P) irradiation at excitation wavelength (lambdaex) 700 nm.

152 By employing the resonant excitation wavelengths lambdaexc = 244 nm and lambdaexc

153 However, the limited tissue-depth of excitation wavelengths limits their clinical applicabili

154 otein is that our construct can be used when excitation wavelengths lower than 488nm are not availabl

155 Our results show that at shorter excitation wavelengths (<800 nm), the signal emitted fro

156 ibitor containing a fluorescent moiety whose excitation wavelengths match the emission wavelengths of

157 The excitation wavelength maxima for 2-AP within these conte

158 Hence, different excitation wavelengths may preferentially activate one c

159 rescent particles relative to their incident excitation wavelengths, Mie scatter conditions were obse

160 itation of this pair by a single multiphoton excitation wavelength (MPE, 850 nm) yields well-separabl

161 iments afford the ability to finely tune the excitation wavelength near the molecular resonance of R6

162 ilon-ADPR was detected by fluorescence at an excitation wavelength of 230 nm and an emission waveleng

163 mly on the Al nanoparticle arrays at a laser excitation wavelength of 257.2 nm.

164 nce emission was observed at ~380 nm with an excitation wavelength of 300 nm.

165 rving the increase in fluorescence, using an excitation wavelength of 360 nm, and measuring emission

166 The fluorometric assay is carried out at an excitation wavelength of 380 nm to eliminate the backgro

167 spores appeared as white-yellow ovals at an excitation wavelength of 395 to 415 nm used for viewing

168 scence emission intensity at 550 nm using an excitation wavelength of 470 nm.

169 resced bright yellow-green when viewed at an excitation wavelength of 470 to 490 nm, whereas live spo

170 tion (LOD) of ~247 pg mL(-1); however, at an excitation wavelength of 532 nm, it provided a LOD of ~6

171 and level of fluorescence polarization at an excitation wavelength of 595 nm and an emission waveleng

172 unsectioned tissue biopsies at a two-photon excitation wavelength of 780 nm.

173 spectral range of 3250-250 cm(-1), using an excitation wavelength of 785 nm, and several bands have

174 e observed peak conversion efficiency at the excitation wavelength of approximately 780 nm indicates

175 igned to provide an optical resonance at the excitation wavelength of cyanine-5 (Cy5), thus providing

176 hape, fluorophore/particle distance, and the excitation wavelength of the coupling photosensitizer, w

177 let resonance Raman (UVRR) spectroscopy with excitation wavelengths of 257, 244, 238, and 229 nm.

178 UVRR) spectra of fd have been obtained using excitation wavelengths of 257, 244, 238, and 229 nm.

179 /- 0.6) x 10(8) with maximum enhancement for excitation wavelengths of 785 nm and lower energy.

180 on and with little apparent phototoxicity at excitation wavelengths of from 930 to 990 nm.

181 ress the influence of antenna morphology and excitation wavelength on polarization conversion efficie

182 erimental data on the effect of changing the excitation wavelength on the ROA spectra of a protein.

183 i3N4 nanowires can be changed along with the excitation wavelength or the excitation light source.

184 c VT activation and exhibited attenuation of excitation wavelength (P<0.001).

185 oxygen production is shown to depend on the excitation wavelength, particularly in a viscous medium.

186 cies of serotonin is identified using pH and excitation wavelength perturbation.

187 2D grid pattern algorithm to switch between excitation wavelengths quickly, we show volume rates as

188 on wavelength range of 485-580 nm and in the excitation wavelength range of 363-475 nm.

189 when the LSPR band is blue-shifted from the excitation wavelength rather than at the on-resonance po

190 hree probes were originally designed as dual excitation wavelength-ratiometric probes, with high phot

191 ) reveals strong photoactivated emission for excitation wavelengths shorter than 520 nanometers.

192 urements as a function of incident angle and excitation wavelength show the existence of both surface

193 The same excitation wavelength simultaneously populates a higher

194 Choosing excitation wavelengths so that excitation ratios were co

195 AMD eyes, however, both the 364- and 488-nm excitation wavelengths stimulated substantial blue-green

196 For a three-photon process, a longer excitation wavelength such as those common in optical co

197 , peak fluorescence occurs at 483 nm for all excitation wavelengths, suggesting a common emissive sta

198 upling strength shows a strong dependence on excitation wavelengths, suggesting the state-specific dy

199 find a dependence of voltage sensitivity on excitation wavelength that is consistent with a two-phot

200 ectrum, lifetimes, and quantum yield (QY) on excitation wavelength that is particularly pronounced in

201 erous multicolor applications using a single-excitation wavelength that was not possible before.

202 olycycle system, greatly extend the range of excitation wavelengths that can be used for fluorescence

203 HG and TPEF from collagen, whereas at longer excitation wavelengths the ECM signal is exclusively due

204 When tuning the excitation wavelength, the distribution changes in both

205 With increased excitation wavelength, the emission maximum shifted towa

206 d by affixing a fluorophore with the desired excitation wavelength to the Cbl-bioagent conjugate.

207 ogenated matrixes requires adjustment of the excitation wavelength to values below that of the standa

208 low values we used different combinations of excitation wavelengths to determine which could be used

209 ields must be precisely matched between FRET excitation wavelengths to isolate dynamic interactions b

210 in concentration, solvent, temperature, and excitation wavelength tune the luminescence energy of bo

211 Furthermore, we demonstrate single excitation wavelength two-colour Ca(2+) and glutamate im

212 tween the UV absorptivity of the tags at the excitation wavelengths typical for UV-MALDI and the magn

213 h an aspect ratio of 3.3 to match the 785 nm excitation wavelength used in the SERS studies.

214 ed with catalysis were very dependent on the excitation wavelength used to monitor the reaction.

215 spillover of di-8-ANEPPS fluorescence at the excitation wavelengths used for fura-2 (340 and 360 nm).

216 trix, we first investigated the influence of excitation wavelength, varied between 2.7 and 3.1 mum, a

217 cident light, while light scattering (at the excitation wavelength) was still present and behaved sim

218 Merely by changing the excitation wavelength, we could specifically excite eith

219 By using appropriate near-infrared excitation wavelengths, we detect strong transient absor

220 est that (3)DOM quantum yields decrease with excitation wavelength, which gives rise to the Phi(1O2)

221 and frequency mixing across a broad range of excitation wavelengths, which cannot be achieved with na

222 ng features comparable to or larger than the excitation wavelength, while E-CARS allows detection of

223 a mode that appears near 32-33 cm(-1) at all excitation wavelengths, with a phase that is consistent

224 d from deep blue to red, just by varying the excitation wavelength without changing its chemical comp