ライフサイエンスコーパス: femtosecond

1 for photosynthetic experiments (few hundred femtoseconds).

2 reversible with a recovery time of about 360 femtoseconds.

3 h coordinate with a resolution down to a few femtoseconds.

4 e scale of this process is a few hundreds of femtoseconds.

5 durations and time resolutions of only a few femtoseconds.

6 limit on the lifetime of this complex of 480 femtoseconds.

7 temperatures of approximately keV in tens of femtoseconds.

8 ehave like a bulk and relaxes in hundreds of femtoseconds.

9 use it typically decays within a few tens of femtoseconds.

10 he molecular structure of acetylene (C2H2) 9 femtoseconds after ionization.

11 These results are promising for ultrafast femtosecond and broadband photodetector applications.

12 al imaging with PINEM, paves the way for the femtosecond and nanometre visualization and control of p

13 absorption and emission spectroscopies, and femtosecond and nanosecond time-resolved transient absor

14 ctures possessing 2-to-4 tetrads by means of femtosecond and nanosecond transient absorption spectros

15 le to measure a correlation function for the femtosecond and picosecond fluctuations in the local ele

16 ing approach to attain the resolution of few femtoseconds and attoseconds in UEM.

17 he pulse duration (typically on the order of femtoseconds) and the size of the focused spot.

18 ng of components with periods as short as 15 femtoseconds, as well as more rapid changes, which have

19 Femtosecond-assisted 120-mum thickness and 9-mm diameter

20 4 patients the recellularized lamina into a femtosecond-assisted 9.5-mm diameter lamellar pocket und

21 carbon-deuterium bonds or propagation of the femtosecond bond motions into slower (nanoseconds to mil

22 The ability to probe femtosecond carrier dynamics in individual flakes can th

23 ly this nonlinear nanoprobe to image the few-femtosecond coherent dynamics of plasmonic hotspots on a

24 X-ray diffraction tracks the light-induced femtosecond coherent lattice motion at a single phonon f

25 visible and nearby spectral ranges allow sub-femtosecond control and metrology of bound-electron dyna

26 We demonstrate a coherent femtosecond control of spin-polarization for electronic

27 Time-resolved serial femtosecond crystallography (SFX) can potentially shine

28 Serial femtosecond crystallography (SFX) using X-ray free-elect

29 us sphaericus BinAB solved de novo by serial-femtosecond crystallography at an X-ray free-electron la

30 ying the recently developed method of serial femtosecond crystallography at an X-ray free-electron la

31 size fractions as desired for future serial femtosecond crystallography experiments.

32 In serial femtosecond crystallography of biological objects-an app

33 ce were used to conduct time-resolved serial femtosecond crystallography on photoactive yellow protei

34 Serial femtosecond crystallography overcomes this problem by ex

35 Serial femtosecond crystallography requires reliable and effici

36 herefore broaden the applicability of serial femtosecond crystallography to challenging projects for

37 r side of the receptor, determined by serial femtosecond crystallography with an X-ray free-electron

38 he structures of complex proteins via serial femtosecond crystallography.

39 oEM method MicroED and potentially by serial femtosecond crystallography.

40 ed on a network of time-division-multiplexed femtosecond degenerate optical parametric oscillators.

41 of extreme-ultraviolet optical vortices with femtosecond duration carrying a controllable amount of O

42 in a signal manipulation cycle of only a few femtoseconds duration (by measurement and ab initio calc

43 mJ-level two-colour hard X-ray pulses of few femtoseconds duration with an XFEL driven by twin electr

44 t can generate pulses of sufficiently short (femtosecond) duration in this wavelength range.

45 Intense femtosecond-duration pulses from X-ray free-electron las

46 2 orders of magnitude, an indication of the femtosecond dynamic contributions to catalysis.

47 h-sampling (TPS) calculations have predicted femtosecond dynamic coupling at the catalytic site of hu

48 paves the way for investigating few- to sub-femtosecond dynamics of both holes and electrons in comp

49 pen in organic molecules and involve coupled femtosecond dynamics of nuclei and electrons.

50 Together with femtosecond early dynamics and computational simulation

51 dynamic description of electron plasma under femtosecond excitation, we numerically investigate harmo

52 thesis occur in organic molecules, but their femtosecond excited-state dynamics are difficult to trac

53 The femtosecond excited-state dynamics following resonant ph

54 xcitonic coherence that has been observed in femtosecond experiments.

55 Here, few-femtosecond extreme UV transient absorption spectroscopy

56 Here, transient femtosecond extreme-ultraviolet measurements suggest tha

57 we demonstrate a highly-efficient source of femtosecond extreme-ultraviolet pulses at 50-kHz repetit

58 standoff detection of uranium by the use of femtosecond filament-induced laser ablation molecular is

59 By inducing femtosecond filamentation with the modulated pulse, we c

60 nts, and no intermediates were observed from femtosecond fluorescence decays.

61 etonitrile, and tetrahydrofuran-by combining femtosecond fluorescence experiments, addressing the eff

62 t electron distribution within a few hundred femtoseconds, followed by a further relaxation via elect

63 modulation, we used pulses of an 800 nm, 60 femtosecond for pump and a MWIR tunable probe in the spe

64 composition into silica substrates through a femtosecond (fs) laser generated plasma assisted process

65 lica substrates based on temporal shaping of femtosecond (fs) laser pulses.

66 Femtosecond (fs) pulsed laser irradiation techniques hav

67 Here, we used femtosecond (fs) soft x-ray spectroscopy near the carbon

68 the second-harmonic frequency (2omega) of a femtosecond (fs) Ti:sapphire laser.

69 s protein promoting vibrations (PPVs) on the femtosecond (fs) to picosecond (ps) time scale to promot

70 Using the femtosecond (fs) X-ray pulses of the Linac Coherent Ligh

71 The highly collimated, energetic and femtosecond gamma-ray bursts that are produced in this w

72 Femtosecond hard x-ray pulses emitted by the Linac Coher

73 surements of ultrafast atomic dynamics using femtosecond HEX-ray pulses.

74 riments and show that the ultrafast (tens of femtoseconds) hot electron decay times observed experime

75 We populated the states through femtosecond illumination of rsEGFP2 in its non-fluoresce

76 is observed on the time scale of hundreds of femtoseconds in all molecules studied.

77 We confirm the upconversion rules of a femtosecond infrared helically phased beam into its high

78 The femtosecond ionization had a large air background not pr

79 The ultrafast dynamics in hundreds of femtoseconds is from the outer-layer, bulk-type mobile w

80 sma with a time resolution as small as a few femtoseconds is proposed.

81 mal incisions were created using the Catalys femtosecond laser (Abbott Medical Optics, Inc., Santa An

82 and flap thickness predictability of Visumax femtosecond laser (FSL) compared to Moria M2 microkerato

83 med in all eye specimens using manual CCC, a femtosecond laser (LenSx, Alcon, Fort Worth, TX), or an

84 The use of femtosecond laser ablation allows for precise removal of

85 Overall, we find that femtosecond laser ablation and ionization of aerosol par

86 d monolayer MoS2 QDs using temporally shaped femtosecond laser ablation of bulk MoS2 targets in water

87 ol to characterize nanoparticles produced by femtosecond Laser Ablation of pure copper are presented.

88 monstrate measurement of uranium isotopes in femtosecond laser ablation plumes using two-dimensional

89 ties for generation of tensile stress during femtosecond laser ablation to roll up the nanoflakes, wh

90 We thoroughly investigated femtosecond laser ablation-inductively coupled plasma-ma

91 Femtosecond laser ablation/ionization mass spectrometry

92 n-rate pulses with high-peak-powers, such as femtosecond laser amplifiers, to facilitate investigatio

93 tracheal epithelium (1 to 12 cells) using a femtosecond laser and followed wound closure up to 6 hou

94 by ocular dominance to flap creation with a femtosecond laser and the other eye to flap creation wit

95 idic devices have recently been proposed for femtosecond laser axotomy in the nematode C. elegans for

96 Femtosecond laser cataract surgery has a low complicatio

97 experiments, suggesting that the fiber-based femtosecond laser desorption mechanism involves a nonres

98 We show that, with the spectrum of a femtosecond laser driver centered at 3.9 mum, right at t

99 y (500 muJ), 45-fs, 800-nm Ti:sapphire-based femtosecond laser electrospray mass spectrometry (LEMS)

100 Femtosecond laser excitation and an ultrashort x-ray pro

101 ources based on supercontinuum generation in femtosecond laser filamentation have enabled application

102 erior and posterior stroma obtained with the femtosecond laser from 4 control samples were used for c

103 ter wavefront-guided ablation with IntraLase femtosecond laser in moderate to high astigmatism.

104 of the ring resonator by using 3-dimensional femtosecond laser inscription technology.

105 to predict the total ion flux emitted during femtosecond laser interaction that depends on laser para

106 l coherence tomography (OCT) to evaluate the femtosecond laser intrastromal incisions made during cat

107 ere grown in 3D through localized heating by femtosecond laser irradiation deep inside 35Li2O-35Nb2O5

108 Femtosecond laser irradiation is capable of crystallizin

109 erter based on this nanowire excited using a femtosecond laser is demonstrated to operate over a rang

110 al of controlled, and fibre-optic delivered, femtosecond laser light pulses to provide new pathways a

111 ctron diffraction from aligned molecules and femtosecond laser mass spectrometry to investigate the d

112 For instance, it might find applications in femtosecond laser material processing.

113 tor of 3.1-fold (PPC mean 73.3+/-24.9 mN vs. femtosecond laser mean 26.1+/-6.8 mN; P = 0.012, Wilcoxo

114 erwater superoleophobicity, fabricated using femtosecond laser micro-hole drilling of a titanium foil

115 a simple and compact all-fiber thulium-doped femtosecond laser mode-locked by carbon nanotubes.

116 significantly stronger than that produced by femtosecond laser or manual CCC.

117 ano-pore-structured metallic thin films with femtosecond laser pulse excitation.

118 de of a dielectric nano-grating excited by a femtosecond laser pulse with an optical period duration

119 brium warm dense copper heated by an intense femtosecond laser pulse.

120 -film patterning using a spatially modulated femtosecond laser pulse.

121 de following the interaction with an intense femtosecond laser pulse.

122 ffect will provide switching with one single femtosecond laser pulse.

123 Here, using a combination of femtosecond laser pulses and microwave excitations, we r

124 ve investigation of absorption of intense 30 femtosecond laser pulses by solid metal targets.

125 as an excellent mode-locker that can produce femtosecond laser pulses from fiber cavities.

126 ion of the circular polarization of incident femtosecond laser pulses into inertial displacement of a

127 s of vibration modes of solvent molecules by femtosecond laser pulses to produce controlled chemical

128 we show by first principles calculations how femtosecond laser pulses with circularly polarized light

129 Mach-Zehnder interferometer and time-delayed femtosecond laser pulses, we obtain a series of images t

130 using coherent acoustic phonons generated by femtosecond laser pulses.

131 With femtosecond laser radiation, more than 40-dB enhancement

132 hours in a pool of sub-cooled water using a femtosecond laser source.

133 We describe the use of a femtosecond laser system (800 nm wavelength, 100 fs puls

134 To assess the role of femtosecond laser technology in the management of severe

135 ly subluxated cataracts may be managed using femtosecond laser technology to perform the capsulotomy

136 yclooctynes with near-infrared pulses from a femtosecond laser triggers photodecarbonylation via nonr

137 complex from blood suggests that fiber-based femtosecond laser vaporization is a "soft" desorption so

138 al of a more robust and affordable laser for femtosecond laser vaporization to deliver biological mac

139 single crystals can be grown inside glass by femtosecond laser writing under optimized conditions.

140 ly, a waveguide waveplate was realized using femtosecond laser writing, but the device length is in m

141 Femtosecond laser-assisted cataract surgery (FLACS) has

142 To investigate the efficacy and safety of femtosecond laser-assisted cataract surgery (FLACS) rela

143 June 2015 were assessed for suitability for femtosecond laser-assisted cataract surgery, with the us

144 Oculus, Wetzlar, Germany) after penetrating femtosecond laser-assisted keratotomy (pFLAK) and laser

145 To analyze the effect of penetrating femtosecond laser-assisted keratotomy (pFLAK) during las

146 Femtosecond laser-based generation of radio frequency si

147 All patients underwent a femtosecond laser-enabled (150-kHz IntraLase iFS; Abbott

148 Femtosecond laser-produced plasmas may thus provide uniq

149 e the phase of the frequency components of a femtosecond laser.

150 psulotomy edge compared to those produced by femtosecond laser.

151 f the light-constricted pupil created with a femtosecond laser.

152 S on a dielectric surface using a high power femtosecond laser.

153 ctrons in n-doped samples with a Ti:sapphire femtosecond laser.

154 Capsulotomy was performed smoothly using a femtosecond laser.

155 hesia after creating a corneal tunnel with a femtosecond laser.

156 s and biomolecules at low photon flux, while femtosecond-laser optical tweezers can probe the nonline

157 Using two femtosecond lasers simultaneously, we could scan and sev

158 n the 10(-14) s range in optics had to await femtosecond lasers to be detected with difficulty.

159 on the interaction of relativistic-intensity femtosecond lasers with aligned copper nanorod array tar

160 and communication, and passively mode-locked femtosecond lasers.

161 Femtosecond LCS did not demonstrate clinically meaningfu

162 on, and should naturally scale to the sub-10 femtosecond level with shorter X-ray pulses.

163 n energy and confirm both the nature and sub-femtosecond lifetime of the virtual intermediate electro

164 t on previously unexplored parameters of the femtosecond light pulse, including pulse front tilt and

165 This method uses a few femtoseconds long relativistic electron bunch to probe t

166 The mutagenic uncoupling of femtosecond motions between catalytic site groups and re

167 red different irradiation conditions using a femtosecond near-infrared laser and found distinct damag

168 Femtosecond nonlinear optical imaging with nanoscale spa

169 generation from the Bi2Se3 basal plane upon femtosecond optical excitation.

170 Here we apply state-of-the-art femtosecond optical Kerr effect spectroscopy, which is c

171 le collisions directly in the time domain: a femtosecond optical pulse creates excitonic electron-hol

172 With femtosecond optical pulses, electronic and lattice degre

173 acterization of electron bunches with single femtosecond or attosecond durations.

174 His are heavy supports local catalytic site femtosecond perturbations coupled to transition-state fo

175 ional helix-coil transition by time-resolved femtosecond/picosecond pump-probe spectroscopy in the vi

176 novel platform for continuous wave (CW) and femtosecond plasmonic optical tweezers, based on gold-co

177 Femtosecond polarized XANES provides the crucial structu

178 rystal-to-liquid phase transition induced by femtosecond pulse laser excitation is an interesting mat

179 y focus one or many spectral components of a femtosecond pulse, and how it can be turned into a contr

180 9-12 yr) using white-light generation under femtosecond pulsed laser illumination.

181 Using a femtosecond pulsed laser, lapatinib release from a nanos

182 2Phatal) that uses focal illumination with a femtosecond-pulsed laser to bleach a nucleic acid-bindin

183 A confocal microscope equipped with a femtosecond-pulsed near-infrared laser was used to simul

184 multiple spectral and temporal modes of the femtosecond pulses can improve the computational perform

185 Here we report the use of femtosecond pulses from an X-ray free electron laser (XF

186 d silica and sapphire by means of a burst of femtosecond pulses having time separation in the range 1

187 on of Murine Leukemia Virus (MLV) via 805 nm femtosecond pulses through gold nanorods whose localized

188 ggests a promising new way of generating sub-femtosecond pulses.

189 When femtosecond pump pulses with average input power P av of

190 By the use of a new femtosecond pump-probe scheme, based on time-resolved ac

191 n molybdenum disulfide, using non-degenerate femtosecond pump-probe spectroscopy to excite and probe

192 Here, we incorporate femtosecond pump-probe spectroscopy to reveal the sub-45

193 Here, by combining femtosecond pump-probe techniques with spectroscopic pho

194 e Mid-Wavelength Infrared (MWIR) range using femtosecond pump-probe techniques.

195 Here, the authors predict that an ultrafast (femtosecond) radiative cooling regime takes place in pla

196 ng Z-scan and pump-probe measurements in the femtosecond regime within the 1.5 mum telecom band.

197 lved X-ray absorption spectroscopy at sub-30-femtosecond resolution and high signal-to-noise ratio.

198 mons at buried interfaces with nanometre and femtosecond resolution has yet to be achieved and is cri

199 e present X-ray diffraction experiments with femtosecond resolution that capture in situ, lattice-lev

200 With femtosecond-resolution measurements, we confirm the extr

201 e we show, with the use of X-ray laser-based femtosecond-resolution spectroscopy and advanced quantum

202 Femtosecond resonant soft X-ray diffraction is used to d

203 Here we show that the femtosecond response of small polyatomic molecules that

204 The observed sub-femtosecond rise of energy transfer from the field to th

205 The use of femtosecond Rydberg spectroscopy as a novel means to use

206 cheap and compact particle accelerators with femtosecond scale control of particles.Controlled genera

207 Upon excitation with an intense femtosecond-short IR laser pulse, the film exhibits the

208 te that single-shot wide-angle scattering of femtosecond soft X-ray free-electron laser pulses allows

209 retch technique, we resolve the evolution of femtosecond soliton molecules in the cavity of a few-cyc

210 Stable transform-limited femtosecond soliton pulses were generated with full widt

211 riven wakefield accelerators require intense femtosecond sources and direct laser-driven accelerators

212 In this study, we used femtosecond spectroscopy to deconvolute seven electron-t

213 By using a tryptophan scan with femtosecond spectroscopy, we simultaneously measured the

214 are followed on the ultrafast time scale by femtosecond stimulated Raman spectroscopy (FSRS) and tra

215 Femtosecond stimulated Raman spectroscopy (FSRS) is a vi

216 transient absorption spectroscopy as well as femtosecond stimulated Raman spectroscopy.

217 ion and fluorescence spectroscopy as well as femtosecond stimulated Raman spectroscopy.

218 on the water droplet is observed with a few femtoseconds, suggesting a mechanism for the gas to part

219 signals (of several hundred eV), coupled to femtosecond temporal resolution as well as ultrafast ene

220 icometre spatial resolution and the inherent femtosecond temporal resolution of lasers, laser-induced

221 Further improvements may lead to femtosecond temporal resolution, with negligible pump-pr

222 ns as they occur requires atomic spatial and femtosecond temporal resolution.

223 science that requires atomic spatial and few-femtosecond temporal resolutions.

224 eriod of optical fields is on the order of a femtosecond, the current switching and its control by an

225 On a time scale of a few hundred femtoseconds, the optical laser pulse excites motions of

226 -fs X-ray pulses, we are able to observe the femtosecond time dependence for the formation of F ions

227 iton's binding energy and coherent size with femtosecond time resolution.

228 olling the electron beam properties with few-femtosecond time resolution.

229 sible semimetallization in fused silica on a femtosecond time scale by using a few-cycle strong field

230 f generating intense X-rays on the tenths of femtosecond time scale enables structure determination w

231 investigation of structural dynamics on the femtosecond time scale, with spatial resolution on the a

232 double bond is up to 0.8 A and occurs on the femtosecond time scale.

233 le energy gaps and Floquet band formation on femtosecond time scales.

234 Here, using femtosecond time- and angle-resolved photoemission spect

235 ed theoretical and experimental treatment of femtosecond time-resolved ARPES (tr-ARPES) show how popu

236 By steady-state and femtosecond time-resolved fluorescence we showed that, u

237 Steady state and femtosecond time-resolved polarized spectroscopies evide

238 Femtosecond time-resolved small- and wide-angle X-ray sc

239 athways was accomplished through analysis of femtosecond time-resolved strong-field ionization and ph

240 Using femtosecond time-resolved two-photon photoelectron spect

241 hemistry predicts that atomic motions on the femtosecond timescale are coupled to transition-state fo

242 xtracting the underlying dynamics on the few-femtosecond timescale from noisy experimental X-ray free

243 flip the ferromagnetic magnetization within femtosecond timescale is unphysically high, some theorie

244 mentally, the IMT in VO2 can be triggered on femtosecond timescale to allow ultrafast nanoscale contr

245 arge-separated (CS) states are formed on the femtosecond timescale upon visible excitation.

246 ges in molecular geometries on their natural femtosecond timescale with sub-Angstrom spatial precisio

247 onal current of energetic electrons on a few-femtosecond timescale.

248 sferred to a neighboring nanoisland within a femtosecond timescale.

249 as light-based electronics operating on sub-femtosecond timescales and at petahertz rates.

250 respond to on-off ratios of 220x gateable on femtosecond timescales.

251 eps in the melting transition on hundreds of femtosecond timescales.

252 bunch charge, sub-micron tolerances and sub-femtosecond timing requirements due to the short wavelen

253 y free-electron laser data recorded with 300-femtosecond timing uncertainty.

254 fastest processes in materials, occurring on femtosecond to attosecond timescales, depending on the e

255 ual water molecules to larger pools and from femtosecond to microsecond time scales.

256 In this work we exploit femtosecond to microsecond transient IR spectroscopy to

257 The issues of femtosecond to picosecond timescales in defining displac

258 alkynylcobalamin PhEtyCbl are examined using femtosecond to picosecond UV-visible transient absorptio

259 eedom of these systems on the time scales of femtosecond to picoseconds delivers new insight into our

260 are observed at time scales ranging from the femtosecond to the picosecond and beyond.

261 structure) on a time scale from hundreds of femtoseconds to 100 ps.

262 ein microcrystals over a time range from 100 femtoseconds to 3 picoseconds to determine the structura

263 e constant increasing from a few hundreds of femtoseconds to a few picoseconds with solvent viscosity

264 with distinct time scales, from hundreds of femtoseconds to a hundred picoseconds.

265 W = tryptophan) on time scales ranging from femtoseconds to milliseconds.

266 ter rearrangement on timescales ranging from femtoseconds to minutes.

267 Pulse lengths ranging from femtoseconds to nanoseconds are utilized at varying lase

268 carbon nitrides on time scales ranging from femtoseconds to seconds.

269 ics of condensed matter samples ranging from femtoseconds to several hundred seconds.

270 nd-order harmonic generation microscopy, and femtosecond transient absorbance spectroscopy.

271 Here, we use visible and near-infrared femtosecond transient absorption (TA) spectroscopy to re

272 Herein we combine femtosecond transient absorption experiments with quantu

273 sion in CH2Cl2 and from 96.3% to 97.6% using femtosecond transient absorption measurements in toluene

274 Femtosecond transient absorption reveals the formation o

275 Femtosecond transient absorption spectroscopic measureme

276 ions are excited-state dynamics deduced from femtosecond transient absorption spectroscopic measureme

277 Femtosecond transient absorption spectroscopy (fsTA) rev

278 ree-way junction systems by a combination of femtosecond transient absorption spectroscopy and molecu

279 electronic structure, we performed broadband femtosecond transient absorption spectroscopy as a funct

280 urprisingly non-metallic based on UV/Vis and femtosecond transient absorption spectroscopy as well as

281 Herein, we present a femtosecond transient absorption spectroscopy study of t

282 Here, we combine femtosecond transient absorption spectroscopy with time-

283 ITIC to PTPD3T hole-transfer, as observed by femtosecond transient absorption spectroscopy.

284 ence and presence of graphene was studied by femtosecond transient absorption spectroscopy.

285 eric dyad (taucrm < 110 fs), monitored using femtosecond transient absorption spectroscopy.

286 amolecular excimer formation, as revealed by femtosecond transient absorption spectroscopy.

287 roscopic techniques such as fluorescence and femtosecond transient absorption.

288 Femtosecond transient IR absorption spectroscopy provide

289 Femtosecond transient mid-IR and stimulated Raman spectr

290 Here we combine femtosecond transient optical absorption spectroscopy wi

291 We compared femtosecond transient visible absorption changes of norm

292 -protected cluster (MPC) were examined using femtosecond two-dimensional electronic spectroscopy (2DE

293 at a resolution of 2.3 A, obtained by serial femtosecond X-ray crystallography (SFX) with an X-ray fr

294 iciently delivering microcrystals for serial femtosecond X-ray crystallography analysis that enables

295 The structure was obtained by serial femtosecond X-ray crystallography from microcrystals at

296 Here we use femtosecond X-ray free electron laser (XFEL) pulses to o

297 However, a recent experiment at a femtosecond X-ray free-electron laser suggests sub-100 f

298 acilities allow the generation of two-colour femtosecond X-ray pulses, opening the possibility of per

299 'proteinquake' observed in myoglobin through femtosecond X-ray solution scattering measurements perfo

300 We introduce polarized femtosecond XANES, combined with UV-visible spectroscopy