ライフサイエンスコーパス: nanosecond

1 e hcp Au(30) NC had a very short lifetime (1 nanosecond).

2 they are metastable, with lifetimes below a nanosecond.

3 ly at 1 million metres-per-second for over a nanosecond.

4 to triplet-triplet annihilation after a few nanoseconds.

5 longer time scale of ten to several hundred nanoseconds.

6 be implemented with resonant driving in 200 nanoseconds.

7 e decreasing from tens of seconds to tens of nanoseconds.

8 termediate is stable for several hundreds of nanoseconds.

9 mping and determined a valley lifetime of 40 nanoseconds.

10 g more than ten microns at times as short as nanoseconds.

11 the matrix chains from subnanoseconds to 100 nanoseconds.

12 ibits ultrafast crystallization within a few nanoseconds.

13 nd have photoluminescence lifetimes of a few nanoseconds.

14 a longest-observed lifetime of 10.8 +/- 0.6 nanoseconds.

15 catalytic processes with a lifetime of a few nanoseconds.

16 conformational changes that occur in tens of nanoseconds.

17 phase-coherence time of T2 approximately 210 nanoseconds.

18 les of motions in an IDR from picoseconds to nanoseconds.

19 tant two orders of magnitude shorter, at 500 nanoseconds.

20 emand removal of surrounding matrices within nanoseconds.

21 -up and spin-down states in as little as ~20 nanoseconds.

22 ead-proximal carbons and occurs over tens of nanoseconds.

23 the recombination time to be of the order of nanoseconds.

24 dulated with interphase intervals of tens of nanoseconds, a prediction of the accelerated membrane di

25 distances of micrometers, takes hundreds of nanoseconds, a time orders of magnitude larger than expe

26 In the first few nanoseconds, actin binding induced an extra primed myosi

27 catalyst was quantified spectroscopically on nanosecond and longer time scales.

28 3'-endo to C2'-endo and vice versa is on the nanosecond and microsecond time scale, respectively.

29 d time-resolved emission spectroscopy on the nanosecond and millisecond time scales.

30 efficient tool for light manipulation on sub-nanosecond and sub-micron scales, and allow for the obse

31 ich lies at a time constant of a few hundred nanoseconds and a simultaneous energy resolution of the

32 on losses, limiting the gain lifetime to sub-nanoseconds and preventing steady laser action.

33 orescence lifetimes (LTs) of several hundred nanoseconds and superparamagnetic Fe(3)O(4) nanoparticle

34 sion experiments compare fast (picosecond to nanosecond) and intermediate (microsecond-to-millisecond

35 oduced from traditional focused femtosecond, nanosecond, and filament-assisted laser ablation.

36 Pulse lengths ranging from femtoseconds to nanoseconds are utilized at varying laser beam energies

37 c-labelling strategies enable studies of sub-nanosecond aromatic-ring dynamics using solution NMR rel

38 rge-separated states that persist for over a nanosecond as observed with transient absorption spectro

39 f the Cd(2+)-bound water molecule is tens of nanoseconds at 20 degrees C in both proteins.

40 luminescence via triplets occurs within 350 nanoseconds at ambient temperature, after reverse inters

41 The ability to detect nanosecond backbone dynamics with site-directed spin lab

42 tions from fast (approximately picosecond to nanosecond) backbone dynamics to amide hydrogen exchange

43 Ultrafast switching (in the range of a few nanoseconds) between amorphous and crystalline phases of

44 e cell is promising for the potential use of nanosecond bipolar pulse technologies for remote electro

45 ting on motions on time scales up to tens of nanoseconds, both in vitro and in cellulo.

46 lays a crucial role in modification by a sub-nanosecond burst.

47 omplexes exhibit panchromatic absorption and nanosecond charge-transfer excited state lifetimes, enab

48 as nanorods, nanowires and nanosheets, with nanosecond coalescence times.

49 Through multi-nanosecond combined quantum-classical molecular dynamics

50 Moreover, the level of screening achieved at nanosecond decay times is shown to change with the cover

51 m communication channel, equivalent to a 500-nanosecond delay line, we demonstrate the emission and r

52 hat ranges from approximately 150 ps to many nanoseconds, depending on the electric field strength.

53 s the junction takes place for up to tens of nanoseconds, depending on the laser fluence.

54 Here, we performed sub-nanosecond DFT-based QM/MM simulations of the E. coli an

55 scale of hundreds of picoseconds to several nanoseconds, due to electron injection into PCBM and ele

56 above [Formula: see text] in a bunch of sub-nanosecond duration.

57 densities in excess of 300 mg cm(-2) with a nanosecond-duration compression pulse--the highest areal

58 ctrum of each spin-labeled peptide indicates nanosecond dynamic disorder that is substantially reduce

59 n experiments to characterize the picosecond-nanosecond dynamics of the free mini-H2-L(d) MHC-I molec

60 The picosecond-to-nanosecond dynamics of the hydrated powders of the two r

61 The dynamics profiles closely match the sub-nanosecond dynamics S(2) values observed by model-free a

62 Here, we report nanosecond-dynamics of a 100nm-diameter magnetic skyrmio

63 oporation efficiency of bipolar and unipolar nanosecond electric field oscillations (NEFO).

64 A bipolar (BP) nanosecond electric pulse (nsEP) exposure generates redu

65 Electroporation by nanosecond electric pulses (nsEP) is an emerging modalit

66 nique aspect of electrostimulation (ES) with nanosecond electric pulses (nsEP) is the inhibition of e

67 resolution coherent vibrational spectrum and nanosecond electronic relaxation.

68 The nanosecond electronic spectra and kinetics of the radica

69 me-delays ranging from a few femtoseconds to nanoseconds enables critical capabilities of probing ult

70 ultrafast cellular probe with a single-pulse nanosecond excitation for a variety of in vitro and in v

71 ith earlier published attribution of the sub-nanosecond exciton radiative lifetime in nanoprecipitate

72 rstanding into the validity of EOS data from nanosecond experiments for geophysical applications.

73 ced from a uranium metal target in air using nanosecond, femtosecond, and femtosecond filament-assist

74 despite having only mild effects on pico- to nanosecond fluctuations as corroborated by NMR.

75 Nanosecond fluorescence anisotropy decay and picosecond

76 FRET-based nanosecond fluorescence correlation spectroscopy allows

77 erference from short-lifetime (approximately nanoseconds) fluorescence background.

78 anar Co(I) intermediate species within a few nanoseconds, followed by its decay in the microsecond ti

79 has to crystallize on a timescale of several nanoseconds following a moderate temperature increase to

80 anging from hundreds of picoseconds to a few nanoseconds for devices consisting of Cu active electrod

81 but long valley lifetimes exceeding several nanoseconds for the dark charged excitons.

82 we report a two-ion entangling gate with 700-nanosecond gate time that uses the strong dipolar intera

83 Here, we use nanosecond-gated spectral acquisition, combined with spe

84 or predominantly molecularly mixed domains), nanosecond geminate electron-hole recombination is obser

85 om the target and lead to the rapid (tens of nanoseconds) generation of large quasi-static electric f

86 cond transient spectroscopies, we report the nanosecond grow-in of a large transient Stark effect, ca

87 que allows detection of radical species with nanosecond half-lives.

88 Overall, nanosecond high-voltage pulsing can be used to significa

89 he gain medium and is pumped by a commercial nanosecond holmium doped yttrium-aluminum-garnet (Ho:YAG

90 These methods enable nanosecond imaging with standard optical systems and sen

91 ollective motions on time scales slower than nanoseconds in the backbone for GB3.

92 phan energy-transfer steps in picoseconds to nanoseconds, in excellent agreement with quantum computa

93 se conditions, water solidifies within a few nanoseconds into nanometre-sized ice grains that exhibit

94 The minimum observed time constant of 200 nanoseconds is well below the dephasing times of roughly

95 rns to its insulating state within 50 to 150 nanoseconds, it is possible to re-trigger the insulator-

96 Together, the nanosecond kinetics characterized here and the milliseco

97 Subthreshold nanosecond laser (SNL) treatment has shown promise in pr

98 effects and mechanical stress created during nanosecond laser ablation processes that were prominent

99 e Cobalt ablation chamber, integrated into a nanosecond laser ablation-inductively coupled plasma-mas

100 This work evaluates the use of nanosecond laser ablation-multicollector inductively cou

101 electrodes (FTCEs) are fabricated by facile nanosecond laser ablation.

102 We demonstrate that 9 flashes by a nanosecond laser are required for the production of the

103 through a facile and flexible single pulsed nanosecond laser based reflection holography and a corne

104 Use of a second nanosecond laser beam, adequately synchronized with the

105 dG(N2-H)(.) is directly observed upon nanosecond laser flash photolysis (LFP) of 1.

106 Further evidence has been obtained by nanosecond laser flash photolysis through detection of l

107 ive irradiations, fluorescence measurements, nanosecond laser flash photolysis, and quantum chemical

108 applying synchronized ultrasound bursts and nanosecond laser irradiation, we developed a novel, sele

109 Nanosecond laser pulses, which are essentially instantan

110 c nanoparticles (NPs) in polymer media using nanosecond laser pulses.

111 e pump-probe experiment consists of a single nanosecond laser pump pulse followed, after a precisely

112 Subthreshold nanosecond laser treatment of one eye did not have an ef

113 ng kinetics of five natural WW domains using nanosecond laser-induced temperature jumps.

114 blate, it is more precise than a solid-state nanosecond laser.

115 es were observed, suggesting that changes in nanosecond-level TCR structural dynamics do not contribu

116 Nanosecond ligand exchange dynamics at metal sites withi

117 cattering with narrowband continuous wave or nanosecond light sources.

118 onds and a slow process from pico-seconds to nanoseconds, limited by exciton diffusion dynamics.

119 Here, we show that nanosecond-long current pulses can move domain walls in

120 a methylammonium vibration, we observe slow, nanosecond-long thermal dissipation from the selectively

121 oemission electron microscopy after applying nanosecond magnetic field pulses.

122 model of the PPi release utilizing extensive nanosecond MD simulations.

123 local dynamic features of substrates on the nanosecond-microsecond time scale that correlate with en

124 ke states, linking substrate dynamics on the nanosecond-microsecond time scale with large collective

125 that faster time scale structural dynamics (nanosecond-microsecond) were the source and therefore im

126 Multi-nanosecond molecular dynamics (MD) simulations of HBV-RT

127 tal and computational study of the nanoscale-nanosecond motion of water at the surface of a topologic

128 that perturbations in equilibrium picosecond-nanosecond motions impact zinc (Zn)-induced allosteric i

129 them (in particular for the fast picosecond-nanosecond motions), much greater differences occur for

130 Here we demonstrate sub-nanosecond nanocarbon synthesis through the application

131 Therefore, a nanosecond Nd:YAG laser beam was focused into a flux of

132 ric devices offer the potential to reach sub-nanosecond non-volatile strain switching at the attojoul

133 tributions concurrently within a few tens of nanoseconds of simulation time.

134 of the amplitudes and timescales (picosecond-nanosecond) of bond vector fluctuations, whereas high-re

135 Here we find that the chief cause of nanosecond-only operation has been thermal runaway: the

136 Hz optical parametric oscillator outputting nanosecond optical pulses at a wavelength of 1.7 mum was

137 ooled water films, which evolved for several nanoseconds per pulse during fast laser heating before q

138 With VPE, hot photoluminescence and nanosecond photo-Dember effect are revealed in inorganic

139 Here, we develop a nanosecond photochemical reaction (nsPCR)-based click ch

140 s between "light" and "heavy" enzymes on the nanosecond-picosecond time scale, suggesting relevant ti

141 ion is found to occur at much later times in nanosecond plasma evolution.

142 ethered to the membrane, for following fast (nanosecond) proton transfer events on the surface of mem

143 nanoporation) of cell plasma membranes after nanosecond pulse (nsEP) exposure remains poorly understo

144 ulse durations between 600 fs and 1.5 ns and nanosecond pulse excitation at 351 nm and 532 nm.

145 sintering comprises the second step, where a nanosecond pulse laser beam welds the nanowires.

146 With the addition of CW and nanosecond pulse lasers, four wave mixing measurements c

147 heating and gas bubble evolution from common nanosecond pulse treatment that lead to high toxicity an

148 g of mammalian cells by electroporation with nanosecond pulsed electric field (nsPEF) facilitates the

149 technologies enable deep tissue focusing of nanosecond pulsed electric field (nsPEF) for non-invasiv

150 Nanosecond pulsed electric fields (nsPEF) are emerging a

151 Nanosecond pulsed electric fields (nsPEF) have been show

152 Nanosecond Pulsed Electric Fields (nsPEF) have the poten

153 esorption (LDTD) at 940 nm and compared with nanosecond pulsed laser ablation at 2940 nm.

154 cron feature pattern on the metal film using nanosecond pulsed laser ablation.

155 Under nanosecond pulsed laser illumination, small nanorods are

156 orous metal-organic framework crystals using nanosecond pulsed laser irradiation.

157 erimental evaluation of damage thresholds in nanosecond pulsed laser-irradiated gold nanospheres, and

158 cs of the domain walls after excitation with nanosecond pulsed magnetic fields.

159 at exposure of carbon black nanoparticles to nanosecond pulsed near-infrared laser causes intracellul

160 Cellular effects of nanosecond-pulsed electric field exposures can be attenu

161 strates under dry, ambient conditions, using nanosecond-pulsed laser irradiation and magnetic gold na

162 performed based on irradiation with a 532 nm nanosecond-pulsed laser over a range of nanoparticle dia

163 photoacoustic flow cytography coupled with a nanosecond-pulsed melanoma-specific laser therapy mechan

164 A combination treatment, long nanosecond pulses followed by standard millisecond pulse

165 lls, while irreversible electroporation with nanosecond pulses is explored to alter intracellular act

166 Nanosecond pulses with 400-800 ns duration are found eff

167 Using nanosecond pulses, the detection limit for DMMP and PFOA

168 e fast, picosecond timescale, whereas in the nanosecond range, a significantly less resilient structu

169 rgy transfer (T-TET) is slow, in the tens of nanoseconds range, whereas it is ultrafast in the oxygen

170 ate lifetimes of iron(II) complexes into the nanosecond regime and expand the range of potential appl

171 ned, agent-based model of mRNA export in the nanosecond regime to gain insight into these issues.

172 n the scanning speed from the microsecond to nanosecond regime, which represents a major technologica

173 able of both femtosecond time resolution and nanosecond relaxation measurement has hampered various a

174 ereafter is monitored by Mie scattering with nanosecond resolution, for all of the time needed for th

175 ntrol, we observed its rethermalization with nanosecond resolution.

176 quantum cascade laser IR spectroscopies with nanosecond resolution.

177 namic range and detectivity, and similar sub-nanosecond response speeds compared to the Au-based devi

178 -processed perovskite photodetector with sub-nanosecond response time is presented.

179 enic, efficient scintillation detectors with nanosecond response time, marking a step-change in oppor

180 ure fast multitransient dynamics at the meso-nanosecond scale and discovered new spatter-induced defe

181 antages of a random Raman laser to image the nanosecond scale dynamics of cavitation formation in wat

182 The appearance of ET-induced nanosecond-scale kinetics in TA features is consistent w

183 h detection efficiency, sub-50-ps jitter and nanosecond-scale reset time.

184 illisecond-scale unbinding events using many nanosecond-scale trajectories that are run without intro

185 The charging current associated with the nanosecond screening process is an important experimenta

186 Formula: see text]) and fast rise time of 17 nanoseconds (setup-limited), among others, hence achievi

187 Phosphorylation was found to block some nanosecond side-chain motions while increasing the flexi

188 of long- and short-lifetime ( approximately nanosecond) signals adds a second dimension for multiple

189 ctures severely destroyed within hundreds of nanosecond simulations.

190 , P(D1) (+*), is only fully developed in the nanosecond spectra, indicating an unusually delayed form

191 Here we demonstrate that sub-nanosecond spin-orbit torque pulses can generate single

192 Rapid (for example, tens of nanoseconds) switching is achieved by an electrostatic,

193 l quantum dot solids has been limited to the nanosecond temporal regime, curtailing their application

194 ckels cells for wide-field image gating with nanosecond temporal resolution and high photon collectio

195 Nanosecond temporal resolution enables new methods for w

196 for the combination of nanometer spatial and nanosecond temporal resolution.

197 e slower collective motions occurring on the nanosecond (tens to hundreds of nanoseconds) time scales

198 e-transfer excitons with lifetime in the sub-nanosecond time domain.

199 tii in the visible and infrared regions with nanosecond time resolution, the latter being accomplishe

200 The results show that fast pico- to nanosecond time scale active site loop fluctuations play

201 ploration of the conformational space on the nanosecond time scale and might have implications in und

202 e ion dynamics in any material observed on a nanosecond time scale by quasielastic neutron scattering

203 trolled induction of optical activity at the nanosecond time scale for exploitation in a new generati

204 o directly observe oxide ion dynamics on the nanosecond time scale in bismuth vanadate with formula B

205 occurs in the normal Marcus regime on a sub-nanosecond time scale in the complexes with exTTF and Zn

206 obases into better aligned geometries on the nanosecond time scale, thus modulating the pi-pi electro

207 ia energy and electron transfer on the femto-nanosecond time scale, thus outcompeting reductive quenc

208 ions of individual atoms on a surface at the nanosecond time scale, using an all-electric scheme in a

209 e controlled by the spin-orbit torque on the nanosecond time scale, which points to exciting opportun

210 that surrounds the flavin chromophore on the nanosecond time scale, while the dark state of AppA is t

211 e and phenylhydroxylamine then occurs on the nanosecond time scale.

212 ered about the internal rotation axis on the nanosecond time scale.

213 le followed by back electron transfer on the nanosecond time scale.

214 bsequent electron dynamics on the picosecond-nanosecond time scale.

215 h two-photon emission processes can occur on nanosecond time scales and can be nearly 2 orders of mag

216 of delocalized singlet excitons on pico- to nanosecond time scales in single supramolecular nanofibe

217 ded temporal dynamics are further chirped to nanosecond time scales using the dispersion in the optic

218 d perovskite nanocrystals occurs on pico- to nanosecond time scales via two spectrally distinct radia

219 ump probe experiments on the femtosecond and nanosecond time scales were carried out.

220 equilibrium dynamics spanning picosecond to nanosecond time scales.

221 dynamic diffractive optics they can generate nanosecond time windows with over 100-kHz repetition rat

222 hnique, which combines pulse radiolysis with nanosecond time-resolved infrared (TRIR) spectroscopy in

223 Associating nanosecond time-resolved spectroscopy and quantum mechan

224 , and temperature-dependent steady-state and nanosecond time-resolved spectroscopy.

225 emission spectroscopies, and femtosecond and nanosecond time-resolved transient absorption and infrar

226 tching field distribution arising on the sub-nanosecond time-scale even in the absence of size and an

227 rocking of low amplitude and of hundreds of nanoseconds time scale.

228 which should be at least in the hundreds of nanoseconds time scale.

229 rring on the nanosecond (tens to hundreds of nanoseconds) time scales, are smaller in the central par

230 tructural transformation is not seen even on nanosecond times following an intense photoexcitation.

231 airs, which undergo spin-state mixing on the nanosecond timescale and subsequent geminate recombinati

232 A major spectral feature on the nanosecond timescale at 725 nm is attributed to an elect

233 ion NMR spectroscopy and also the picosecond-nanosecond timescale backbone dynamics of this domain.

234 talline stishovite grains is resolved on the nanosecond timescale just after shock compression.

235 efficients were found, which converge on the nanosecond timescale toward diffusion coefficients deter

236 port kinetics were detected in response to a nanosecond timescale variation in the applied electric p

237 These times are on the nanosecond timescale, and are longer than the characteri

238 Overall, in the nanosecond timescale, the degree of the observed flexibi

239 in response to the action of the drug on the nanosecond timescale.

240 ion of the permeant molecule on the pico- to nanosecond timescale.

241 al recombination and heating dynamics on the nanosecond timescale.

242 observed, which are enhanced on the slower, nanosecond timescale.

243 ntial reduction in thermal conductivity on a nanosecond timescale.

244 Here, we map nanosecond-timescale dynamics and structural heterogenei

245 ransport and relaxation dynamics at pico- to nanosecond timescales and at length scales relevant to c

246 f NML architectures repetitively operated on nanosecond timescales and identify relevant engineering

247 bone dynamics in solution is confined to sub-nanosecond timescales and, hence, it is dynamically more

248 raction measurements of diamond formation on nanosecond timescales by shock compression of pyrolytic

249 rding processes and events that occur on sub-nanosecond timescales poses a difficult challenge.

250 720-nm negative feature on the picosecond-to-nanosecond timescales, coinciding with charge separation

251 magnetic field, which can be manipulated on nanosecond timescales, providing a platform for addressi

252 scattering spectroscopy on the picosecond to nanosecond timescales.

253 rain profiles in laser compressed samples on nanosecond timescales.

254 off the bond of the photonic molecule on sub-nanosecond timescales.

255 than one order of magnitude on picosecond to nanosecond timescales.

256 nd imprinting processes, but at ultra-short (nanosecond) timescales.

257 enable imaging lifetimes within the relevant nanosecond to microsecond range.

258 has the potential for such studies over the nanosecond to microsecond real time scales.

259 emission lifetime of the nanofiber from the nanosecond to microsecond regime.

260 rains exhibits unprecedented mobility on the nanosecond to microsecond timescales, and the experiment

261 ge (13)C-(13)C scalar couplings reporting on nanosecond to millisecond motions can be quantified in p

262 possible to extract kinetic information from nanosecond to millisecond time scales.

263 d the role of conformational dynamics on the nanosecond to millisecond timescale in HIV-1 CA assembli

264 me 1 by transient absorption spectroscopy on nanosecond to millisecond timescales.

265 r of supercooled metallic liquids within the nanosecond to picosecond regimes.

266 Unexpectedly, studies of fast (nanosecond to picosecond) motions revealed that F508del

267 ntaneous binding and unbinding pathways from nanosecond to second time-range.

268 r four orders of magnitude in time, from one nanosecond to ten microseconds, with a single adjustable

269 appeared and grew on time scales between 20 nanoseconds to 3 microseconds, whereas crystallization o

270 from changes in molecules that occur within nanoseconds to changes in populations that occur over mi

271 isolated protein domains to live cells, from nanoseconds to hours.

272 , with nominal simulation times ranging from nanoseconds to microseconds depending on system size.

273 s with a recombination lifetime from several nanoseconds to microseconds.

274 of conformations on timescales ranging from nanoseconds to milliseconds and above.

275 of the femtosecond bond motions into slower (nanoseconds to milliseconds) motions of the larger prote

276 f its structural dynamics on timescales from nanoseconds to milliseconds.

277 petitive phenomenon with the time scale from nanoseconds to milliseconds.

278 ologies for time-resolved measurements (from nanoseconds to minutes).

279 ndensation, with time scales increasing from nanoseconds to tens of millions of years.

280 tic jump of coherence times from few tens of nanoseconds to the microsecond regime between 2 and 3 T

281 Ultrafast and nanosecond transient absorption and time-resolved infrar

282 Nanosecond transient absorption measurements provide com

283 g 2-to-4 tetrads by means of femtosecond and nanosecond transient absorption spectroscopy with global

284 rated and spectroscopically characterized by nanosecond transient absorption spectroscopy.

285 state photolysis, as well as femtosecond and nanosecond transient absorption spectroscopy.

286 radicals were generated and characterized by nanosecond transient absorption spectroscopy.

287 hylgermane cation radicals were generated by nanosecond transient absorption spectroscopy.

288 established from studies involving femto- to nanosecond transient absorption techniques.

289 ing the photochemical initiation approach to nanosecond transient infrared and visible absorbance spe

290 CCGGATCCGG}2 and 5'-{CCGGTACCGG}2 using pico/nanosecond transient visible and time-resolved IR (TRIR)

291 Here we interpret a nanosecond transient yellow emission band at 590 nm (2.1

292 Nanosecond transient-absorption and steady-state photoly

293 tes from surface related states and exhibits nanosecond transition.

294 the photoreactions are characterized here by nanosecond UV-vis and IR absorption spectroscopy.

295 acts, driven into extreme non-equilibrium by nanosecond voltage pulses.

296 two dimers associate rapidly within tens of nanoseconds when their binding surfaces are separated by

297 locate through the interior over hundreds of nanoseconds, while Cer and cholesterol take around a mic

298 igid body motions on a time scale of tens of nanoseconds, while the time scale for the seventh helix

299 ed PCRAM products are limited by the tens of nanoseconds writing speed, originating from the stochast

300 00 ps range were unchanged with pH, although nanosecond yield, rates, and access all changed.