ライフサイエンスコーパス: ps

1 tend the lifetime of the (5,7)MLCT from 14.0 ps for [Fe(dftpy)2](2+) to the largest known value at 17

2 of a greatly increased MLCT lifetime of 14.0 ps.

3 n slightly normal cavity dispersion at 0.055 ps(2), and delivers 152 fs pulses with 52.8 nm bandwidth

4 agnetoelectric coupling coefficient of 0.057 ps/m.

5 e observes an ultrafast ( approximately 0.06 ps) evolution that reflects relaxation from initial nonp

6 namics slow from 1.5 ps in bulk water to 3.1 ps for interfacial water.

7 TyrOH(*+) is formed in approximately 1 ps by electron transfer to excited flavin and decays in

8 The nearly approximately 1 ps dephasing time, efficient electron scattering with di

9 r electron and hole decay of approximately 1 ps suggests a Shockley-Read-Hall recombination mechanism

10 en excitation and reaction ( approximately 1 ps) was too short for molecular rotation before the seco

11 SiV(-) using ultrafast pulses as short as 1 ps, significantly faster than the centre's phonon-limite

12 , together with electron-phonon coupling (~1 ps) and normal phonon-phonon coupling (>100 ps) processe

13 encompassing 11 orders of magnitude (from 1 ps to 0.2 s).

14 n of the Raman pump pulses from ~80 fs to >1 ps confirms that the cross sections are independent of t

15 fer in the single-exciton regime occurs in 1 ps.

16 tion, respectively; is active for at least 1 ps.

17 of how MoS(2) interacts with ultrafast (< 1 ps) pulses.

18 nhanced by using ultrashort laser pulses (~1 ps) thus limiting heat flow during the interaction.

19 n both the weak resonant PL and the slower 1 ps(-1) exciton relaxation rate observed.

20 Efficient, sub-1 ps intersystem crossing leads to the population of a tri

21 her excited states are typically less than 1 ps.

22 idth products of ~100 for pulses of width ~1 ps are observed, with no fundamental limit on the system

23 ts show that singlet fission occurs within 1 ps in an amorphous thin film of BET-B with high efficien

24 ttraction to generate free carriers within 1 ps.

25 excitation (He[Formula: see text]) within 1 ps.

26 hot carrier cooling ( k(cooling) ~ 10(-1) 1/ps) compare favorably with what has been reported in the

27 d configuration that occurs in 1.61 +/- 0.10 ps.

28 cies forms with a time constant of 36 +/- 10 ps with a yet undetermined structure.

29 irac electronic recovery of approximately 10 ps at most in the bulk-metallic regime elongated to >400

30 is followed by rapid (t1/2 approximately 10 ps) and efficient surface electron transfer from C343(-)

31 oring groups on timescales between around 10 ps and a few ns (corresponding to the instrumental range

32 e "semi-dark" trions and biexcitons to be 10 ps, and analyse how these complexes appear in the temper

33 ong rotational coherence, extended beyond 10 ps.

34 the absence of such jumps is found to be >10 ps.

35 sonance state (S1) that relaxes quickly (<10 ps) to a charge-transfer state (S1*).

36 target rear only at later time-scales of 10 ps, resulting in a commensurate large-scale filamentatio

37 s decay led by lattice instabilities over 10 ps timescales.

38 lectron temperature and its decrease over 10 ps.

39 ination kinetics (lifetime shortening to ~10 ps).

40 zed high-energy (HE) state emerges within 10 ps after the pulse excitation.

41 photon counters capable of approximately 10-ps time tagging.

42 nonresonant 2 ps pulse excitation, a sub-10-ps transient circularly polarized high-energy (HE) state

43 ndently with different lifetimes (ca. 10-100 ps).

44 ion recovers on the timescale of 510 +/- 100 ps.

45 investigated for pulses between 0.6 and 100 ps.

46 re not resolved due to the approximately 100 ps duration of the available X-ray probe pulse.

47 nce time of the O state is approximately 100 ps for all examined amides, so the large variation in me

48 d with lifetime as long as approximately 100 ps, which is 2-3 orders of magnitude longer than those i

49 n timescales of <15 ps and approximately 100 ps.

50 While a NiTMP excited state present at 100 ps was previously identified by X-ray transient absorpti

51 S) over 10 decades of time spanning from 100 ps to 1 s.

52 he time ranges from 2 to 25 ps, and from 100 ps to 2 ns, using two spectrometers.

53 ps) and normal phonon-phonon coupling (>100 ps) processes.

54 ic and thermal effects in a long-lived (>100 ps) transient metastable state of Ge2Sb2Te5 with muted i

55 ear unit quantum yield on a time scale < 100 ps and an activation energy of 12.6 +/- 1.4 kJ/mol.

56 0.73)(N0.27O0.73) NCs has both a short (<100 ps) and a long-lived component, with a long overall aver

57 thynyl)[TIPS]--tetracene we find rapid (<100 ps) formation of excimers and a slower ( approximately 1

58 a measurement of short spin lifetimes (<100 ps), a regime that is not accessible in semiconductors u

59 An intrinsic switching time of 100 ps per magnet is observed.

60 achieve an effective time resolution of ~100 ps at a 25 nm spatial resolution to map micro-radian dyn

61 Using a single 100 ps synchrotron x-ray pulse, we have measured, by K-edge

62 y crystals, each collected with a single 100 ps X-ray pulse exposure per crystal using a setup optimi

63 ed having their relevant dynamics on the 100 ps timescale, our results open the way to ultrahigh-spee

64 e scale from hundreds of femtoseconds to 100 ps.

65 d creates a single optical photon within 100 ps.

66 by the heat release to the matrix on the 100-ps timescale.

67 bedding organic matrix, occurring on the 100-ps timescale.

68 scence lifetime for unpatched areas of ~1000 ps up to 24 h.

69 ere transferred with a time constant of 1087 ps.

70 experimentally demonstrate an ultrafast (<11 ps) yet efficient source of spontaneous emission, corres

71 function across all participants (rs > .11, ps < .031).

72 condary charge-shifting rate (tau(CS2) = 110 ps) and results in no change in ethynyl vibrational freq

73 ng autofluorescence lifetimes of around 1100 ps in either spectral channel.

74 akes place in tauSF = 22, 336, 195, and 1200 ps, respectively, to give triplet yields of 200%, 110%,

75 uring dynamic relaxation is obtained as 0.13 ps.

76 orientational randomization, slows from 136 ps in the bulk to 513 ps in the PES30.

77 he slowest decay constant increases from 140 ps in the bulk to 504 ps in the PES200 and increases fur

78 Discrepancy still exists at early time 0-15 ps, likely due to non-equilibrium conditions.

79 state show good agreement with data after 15 ps.

80 proximately 65 ps upon 400 nm excitation (15 ps slower than PSI-LHCI) and approximately 78 ps upon 47

81 to PSII occurs on two main timescales of <15 ps and approximately 100 ps.

82 using of the diffusive light is based on ~15-ps initial dipole moment depolarization followed by ~50-

83 equilibrates with the environment in 100-150 ps.

84 istics with tauS = 310 ps in toluene and 150 ps in benzonitrile.

85 740 nm, we observe a final approximately 150 ps decay assigned to trapping by charge separation, and

86 B(B) An ~10% population of P* decays in ~150 ps largely by internal conversion.

87 of quenching, which occurs at a rate of ~150 ps(-1) and is not induced by LHCII aggregation.

88 al time constant for the foldamer (tau = 150 ps), indicating the initial steps of unfolding of the he

89 nt transfer for charge separation on the 150 ps timescale.

90 metastable state can be generated within 150 ps at 190 K.

91 he thermalized (5,7)MLCT is long-lived at 16 ps, representing a > 100 fold increase compared to the (

92 a profoundly extended (3)MLCT lifetime (160 ps), (3)MLCT phosphorescence, and ambient environment st

93 in the PES200 and increases further to 1660 ps in the PES30.

94 hole transfer time constants as fast as 170 ps.

95 wed a single positron decay curve with a 175 ps lifetime component that was attributed to Zn vacancie

96 adiative relaxation times from 270 ps to 190 ps upon increasing excitation intensities.

97 Ac via intersystem crossing on a 1.5 +/- 0.2 ps time scale.

98 fast charge recombination with rates of ~0.2 ps(-1), thus inhibiting cage escape and photoproduct for

99 nitial radical formation time of 1.3 +/- 0.2 ps, which is identical to the time to populate the surfa

100 ives PDI(+*)-PDI(-*) in tauCS = 12.0 +/- 0.2 ps.

101 The (3) MC state is rapidly (2.2 ps) deactivated to the ground state.

102 ree pathways: (1) excimer formation (4 +/- 2 ps), (2) excimer relaxation (160 +/- 40 ps), and (3) exc

103 c state in i-(dC)(10) is responsible for a 2 ps red-shifted emission at 370 nm observed in the decay-

104 emical exchange with a time scale of about 2 ps.

105 s indicates that dissociation occurs in >/=2 ps, in agreement with theory.

106 ocalization and energy relaxation occur in 2 ps.

107 Under a circularly polarized nonresonant 2 ps pulse excitation, a sub-10-ps transient circularly po

108 triplet pair (1)(T1T1) on a time scale of 2 ps, which decays to the ground state without forming sep

109 The kinetics shows a rapid 2 ps time constant for almost complete transfer to chlorop

110 We find that the non-equilibrium state, 2 ps after the excitation, exhibits strongly suppressed lo

111 laxation of the excited state shorter than 2 ps in both cases.

112 Fast electron transfer in less than 2 ps is observed for a driving force between 0.2 and 0.6 e

113 long-lived coherent THz oscillations up to 2 ps at low temperature.

114 ly at an in plane rate of Dphi = 0.07 rad(2)/ps and an out of plane rate of Dtheta = 0.05 rad(2)/ps.

115 an out of plane rate of Dtheta = 0.05 rad(2)/ps.

116 g-wavelength chlorophyll forms within 0.1-20 ps and revealed little or no charge separation and oxida

117 ion time of neat BmimNTf2 liquid (870 +/- 20 ps) measured with optical heterodyne-detected optical Ke

118 randomization on a time scale of 900 +/- 20 ps, significantly slower than observed for SeCN(-) but i

119 ural deformation whose lifetime is around 20 ps at 298 K.

120 ompared to the monomer M (tau4,foldamer = 20 ps, tau4,monomer = 9 ps).

121 > P(+)H(B) (-) conversion takes place in ~20 ps by a superexchange mechanism mediated by B(B) An ~10%

122 tes a fast charge-transfer process within 20 ps of photoexcitation.

123 (8 GHz-12 GHz), and a time resolution of 200 ps (6 cm optical path in free space).

124 characterized by high speed switching (~200 ps), error rates as low as 10(-5) and decoherence effect

125 diffusive dynamics at times shorter than 200 ps, with a transient diffusivity up to 1,000 times highe

126 r(3) (0.27 ps, 4.6 meV/fs) > FAPbBr(3) (0.21 ps, 5.8 meV/fs).

127 quidistant on a logarithmic scale between 21 ps and 21 ns.

128 ole to Co3O4 catalyst proceeds in 255 +/- 23 ps.

129 tPhCbl forms an excited state with a ca. 247 ps lifetime.

130 endent charge separation rates of up to 1.25 ps(-1) that exceed the rates found for typical ruthenium

131 odulation depth (64%), fast relaxation (1.25 ps) and high thermal damage threshold.

132 randomization occurring in approximately 25 ps.

133 rly, their short excited state lifetime (<25 ps) renders them potential energy sinks able to compete

134 d regime, while the timing jitter remains 25 ps.

135 f the lasing gain profile with time up to 25 ps, and assign this as a signature for lasing involving

136 was studied in the time ranges from 2 to 25 ps, and from 100 ps to 2 ns, using two spectrometers.

137 constants (tauCR approximately 31.8 and 250 ps) that likely reflect CR dynamics involving both an in

138 les for durations of 10's - 100's fs for 250 ps, 800 nm chirped pump pulses.

139 resolution of 12%, timing resolution of 256 ps, and a noise-equivalent count rate above 1,000 kcps b

140 r(3) (0.39 ps, 2.9 meV/fs) > MAPbBr(3) (0.27 ps, 4.6 meV/fs) > FAPbBr(3) (0.21 ps, 5.8 meV/fs).

141 proximately 78 ps upon 475 nm excitation (27 ps slower).

142 on in PL radiative relaxation times from 270 ps to 190 ps upon increasing excitation intensities.

143 SC: lesion, 400 ps; unremarkable retina, 294 ps; P < 0.001; LSC: lesion, 404 ps; unremarkable retina,

144 n optical dipole allows us to assign the 1.3 ps time constant to the production of both O-site radica

145 t laser pulse lengths shorter than about 2.3 ps, while the other two are observed for longer pulses.

146 transfer process with a lifetime of about 3 ps mediated by photo-excited polaron pairs which has a m

147 excited flavin and decays in approximately 3 ps by charge recombination.

148 estricted wobbling motion of approximately 3 ps, and complete randomization occurring in approximatel

149 have intrinsic response times as short as 3 ps implying photodetection bandwidths as wide as 300 GHz

150 f the thietane intermediate in as short as 3 ps, which intersystem crosses to its ground state and re

151 the trajectories require an extraordinary 3 ps to descend an exergonic slope.

152 itation and proton transfer that lives for 3 ps.

153 f the magnetic order by ~10% and within </=3 ps by optically controlling the magnetic exchange intera

154 an be demonstrated with quick formation of 3 ps but prolonged lifetime of ~0.5 mus.

155 -750 nm) and tauS = 2.8 ns in toluene and 30 ps in benzonitrile.

156 width on the time scale of approximately 30 ps, while the rest of inhomogeneity is static on the tim

157 microscopy has temporal resolution below 30 ps and spatial resolution determined by the area of ther

158 er shows these structures interconvert in 30 ps.

159 relaxation from HS to LS taking place in ~30 ps.

160 he band-edge are seen to recombine within 30 ps while higher lying transitions observed near 1.2 eV a

161 d state interactions is the formation of 300 ps lived charge separated states once photoexcited.

162 hard X-ray pulses on time scales down to 300 ps, comparable to the X-ray pulse width from typical syn

163 having time separation in the range 10-3000 ps.

164 two distinct carrier lifetimes of 0.6 and 31 ps and a long-lived component of several ns.

165 iate optical characteristics with tauS = 310 ps in toluene and 150 ps in benzonitrile.

166 SC: lesion, 404 ps; unremarkable retina, 316 ps; P < 0.001).

167 occurs in tau(CS1) = 5 ps and tau(CS2) = 330 ps, respectively, while charge recombination in ca. 300

168 dependent decay with a time constant of ~350 ps.

169 he energy transfer to P(700) occurred at ~36 ps, similar to the DM-PSI.

170 -) occurred with a characteristic time of 36 ps, being kinetically controlled by energy transfer from

171 repopulates the ground state with tau = 362 ps.

172 nd-state with 560 fs pulse duration and 1.37 ps separation; and singlet+doublet soliton structures wi

173 chieved with the Discovery MI, including 375 ps FWHM coincidence time resolution and sensitivity of 1

174 rate in the following order: CsPbBr(3) (0.39 ps, 2.9 meV/fs) > MAPbBr(3) (0.27 ps, 4.6 meV/fs) > FAPb

175 D to FAD(*-) by the proximal tryptophan (0.4 ps) and is followed by delocalized migration of the prod

176 three LHP NCs show fast HC relaxation (<0.4 ps) with the cooling time and rate in the following orde

177 py)2](2+) to the largest known value at 17.4 ps for [Fe(dbtpy)2](2+).

178 y observed for the phenyl-derivative in ~2.4 ps while absent in the other two dimers.

179 verage coincidence time resolution was 375.4 ps FWHM.

180 tion is rapid and complete, occurring in 4.4 ps.

181 ver a nanoscale region, remaining cold for 4 ps.

182 In an ~40% population, P* decays in ~4 ps via a 2-step process involving a short-lived P(+)B(B)

183 s, revealing ultrafast charge separation (~4 ps) occurring from the PE(4) segment to NDI when excited

184 e electron transfer completes in less than 4 ps, it triggers a proton transfer lasting over hundreds

185 /- 2 ps), (2) excimer relaxation (160 +/- 40 ps), and (3) excimer decay (>3 ns).

186 hannels with a time-resolved capability ( 40 ps temporal resolution) using fewer than N(2) optical me

187 stems, an unusually slow ( approximately 400 ps) but ultimately efficient charge generation mediated

188 n the bulk-metallic regime elongated to >400 ps when the charge neutrality point was approached.

189 oxic lesions in the retina (SSC: lesion, 400 ps; unremarkable retina, 294 ps; P < 0.001; LSC: lesion,

190 retina, 294 ps; P < 0.001; LSC: lesion, 404 ps; unremarkable retina, 316 ps; P < 0.001).

191 trol subjects (N170 ES = .64; N250 ES = .49; ps < .001).

192 )ExBIPY(2+) unit to the DAPP(2+) unit in 0.5 ps to yield (1*)DAPP(2+).

193 gap domains to the low-bandgap domains (<0.5 ps) compared to the randomly oriented films.

194 tic X-ray laser-plasma source (duration ~0.5 ps, photon energy >1 keV) to the study of a laser-driven

195 The slow hot carrier relaxation time is 0.5 ps.

196 o generate a hydronium ion approximately 1.5 ps after excitation.

197 en bond rearrangement dynamics slow from 1.5 ps in bulk water to 3.1 ps for interfacial water.

198 h interference oscillatory signals up to 1.5 ps were reported and interpreted as direct evidence of e

199 cP slows down water motions from 0.9 to 1.5 ps, as measured by the carbonyl frequency fluctuations.

200 +*)-ExBIPY(+*) radical ion pair in tau = 1.5 ps.

201 s an unprecedented relaxation process of 4-5 ps-a fast phonon-phonon relaxation process, together wit

202 After a 4.5 ps delay, another distinct surface species forms with a

203 y to the 4-coordinate (4c) heme (tauG1 = 7.5 ps; 97 +/- 1% of the population) or exits the heme pocke

204 venges the excitonic hole in approximately 5 ps to form QD(*-); electron transfer to nitrobenzene or

205 cond electron transfer takes approximately 5 ps, which leads to a mixture of redox states of the acce

206 (+*)-ANI-NDI(-*) that occurs in tau(CS1) = 5 ps and tau(CS2) = 330 ps, respectively, while charge rec

207 nnular magnetic field profile was observed 5 ps after the interaction, indicating a relatively smooth

208 d to form rapidly (with a time constant of 5 ps), but in this case it occurs in concert with establis

209 oes a lattice expansion on a time scale of 5 ps, which is due to the excitation of short-wavelength i

210 h intensity (10(18) W/cm(2)), short-pulse (5 ps) laser with wavelength of 1.054 mum.

211 lowed by a pulsed state that lasts for 20-50 ps at a low energy (LE) state.

212 dical along the tryptophan triad (~4 and ~50 ps).

213 Fast (tau </= 50 ps) components report on librational motions, a dominant

214 ermal contraction with a time constant of 50 ps is observed and associated with the excitation of out

215 e quantum yield squaraine dye molecule on 50 ps timescales.

216 dipole moment depolarization followed by ~50-ps repolarization into desired directions.

217 Despite 50-ps breakdown in time-of-flight reciprocity, the sites' t

218 because of high detection efficiency, sub-50-ps jitter and nanosecond-scale reset time.

219 c with time constants in the 3-30 and 30-500 ps range.

220 ics generated by the delivery of focused 500 ps duration laser radiation at lambda = 532 nm within fi

221 rapidly, reaching a value of D0 roughly 500 ps after the excitation pulse.

222 ant increases from 140 ps in the bulk to 504 ps in the PES200 and increases further to 1660 ps in the

223 zation, slows from 136 ps in the bulk to 513 ps in the PES30.

224 cal population lifetimes of approximately 54 ps for both TA* and TB* tautomers.

225 d fluorescence lifetimes to between ~518-583 ps.

226 II) sites in the octahedral sheet within 0.6 ps of photoexcitation; (ii) Mn(III) migration into the i

227 were determined to be (1.7 ps)(-1) and (3.6 ps)(-1), respectively.

228 MLCT state then decays much more slowly (7.6 ps) to the (3) MC state.

229 he two reactions are 640+/-130 fs and 74+/-6 ps, respectively.

230 oliton structures with 1.8 ps duration and 6 ps separation.

231 ally overlapping noise photons, within the 6 ps detection window (amounting to 113,000 times noise pe

232 ime reduces to ultralow value of ca. 0.66(6) ps, resulting in ultralow thermal conductivity in TlInTe

233 LHCII to PSI-LHCI occurs in approximately 60 ps.

234 y invariant for all foldamer lengths (ca. 60 ps), the subsequent hole transfer to the donor varies fr

235 from photoselection are maintained on the 60 ps timescale that corresponds to the dominant energy tra

236 ructural spectral diffusion component of 600 ps in addition to short and intermediate time scales sim

237 II) migration into the interlayer within 600 ps; and (iii) increased nanosheet stacking.

238 a period of 249 fs and damping time of 0.63 ps is observed on the (5)T(2g) surface, and the spectrum

239 time for PSI-LHCI-LHCII is approximately 65 ps upon 400 nm excitation (15 ps slower than PSI-LHCI) a

240 on transfer from the two TAA units (tau = 65 ps), followed by intermolecular proton transfer from TsO

241 nd rise time and a recovery time of about 66 ps, which suggests a modulation speed performance of ~15

242 4 decays with a time constant of 1/ke' = 660 ps in the mixture versus 1/ke = 4.1 ns in g-C3N4 alone.

243 ty, on week-8 depression levels (Fs >= 9.67, ps <= 0.002).

244 at half maximum durations of 610 fs and 1.68 ps at wavelengths of 1480 nm and 1845 nm, respectively,

245 ement of proton bursts as short as 3.5+/-0.7 ps from laser solid target interactions for this purpose

246 OH with calculated jump times of 1.4 and 1.7 ps for the air and hydrophobic interfaces, respectively.

247 ) proton transfer were determined to be (1.7 ps)(-1) and (3.6 ps)(-1), respectively.

248 ynchrotron-limited temporal resolution of 70 ps.

249 The switching time is faster than 70 ps, extending perovskite microlasers to previously inacc

250 roximal His rebinds to the 4c heme with a 70-ps time constant.

251 ial decays of the excited state with 600~700 ps dominate in all three iRFPs, while photoinduced isome

252 s slower than PSI-LHCI) and approximately 78 ps upon 475 nm excitation (27 ps slower).

253 , with anomalous group delays as long as 1.8 ps detected across the bandwidth covered by 80-fs laser

254 singlet+doublet soliton structures with 1.8 ps duration and 6 ps separation.

255 1)-S(0) evolution to the ground state in 4.8 ps.

256 ery similar rotation rates ( approximately 8 ps) at room temperature, despite differences in other te

257 thways have rate constants ranging from (800 ps)(-1) to (2.2 ns)(-1), which are 1-2 orders of magnitu

258 (*+) and deprotonation then proceeds in ~800 ps, without any significant kinetic isotope effect, nor

259 the modulation rise-time was limited to ~800 ps by our measurement system, theoretical considerations

260 species (G[-H]C[+H]) with a lifetime of 2.9 ps was tracked.

261 r M (tau4,foldamer = 20 ps, tau4,monomer = 9 ps).

262 The fastest EnT process occurs in 90 ps and is potentially competitive with Auger recombinati

263 h across two orders of magnitude down to 900 ps, a broadly-tunable repetition rate across three order

264 nd higher number of heavy drinking days (all ps < 0.05).

265 iation between %5 mC and LTL in females (all ps < 0.01), but not in males.

266 e, Cmax, AUC, and shorter T1/2 than men (all ps<0.04).

267 making, quality of life, or preferences (all ps > 0.05).

268 differences between the four quartiles (all ps < 0.042) for most groups, with the exception of penta

269 [(11)C]OMAR VT was significantly (all ps < .05) lower in SCZs in the amygdala, caudate, poster

270 implants may need replacement over time (all ps < 0.002).

271 iations in African Americans and whites (all ps < 0.03).

272 helix while the overall structure of aps and ps DNA is maintained.

273 es spatial and time resolution on the nm and ps scale, respectively, thus enabling measurements at el

274 The beta(ps)-integrin Myospheroid, which is necessary for basal c

275 l cortex; all false discovery rate-corrected ps < .05), which are regions of the default mode network

276 ural outcomes revealed a therapeutic effect (ps < 0.01) of hUCBC or IL-8 administration, which was co

277 ignaling proteins through modulation of fast ps-ns sidechain dynamics.

278 s, with the inverse agonist suppressing fast ps-ns timescale motions at the G protein binding site.

279 Transient spectroscopic studies (from ps to s) show that the bimolecular recombination of phot

280 nism of LDH and establish the coupling of fs-ps protein dynamics to barrier crossing.

281 (15)N relaxation studies show a decrease in ps-ns backbone dynamics in the free state of consensus-H

282 earance of speed-of-sound (for example, 6 nm ps(-1)) wavefronts are influenced by spatially varying n

283 t a velocity of approximately 1.4 +/- 0.5 nm/ps (km/s), in close agreement with the expected speed of

284 ue is well-accommodated at the 7-position of ps DNA and even led to a stabilization of the parallel d

285 ed light absorber in less than 1 picosecond (ps).

286 and, with a transient close to a picosecond (ps), new electronic states appear in the O K-edge x-ray

287 PPVs) on the femtosecond (fs) to picosecond (ps) time scale to promote crossing of the chemical barri

288 bBr(3) perovskite nanowires with picosecond (ps) time resolution and show that lasing originates from

289 charge-transfer lifetime of 100 picoseconds (ps) and room-temperature photoluminescence.

290 tron injection into TiO2, followed by rapid (ps-ns) and sequential two-electron oxidation of TEOA tha

291 ps) DNA as well as DNA with parallel strand (ps) orientation.

292 We present a sub-ps X-ray spectroscopy study of an Fe(II) NHC complex tha

293 helical coil targets with a few joules, sub-ps laser pulses at an intensity of 2 x 10(19) W cm(-2).

294 The ps-ns motions were not significantly altered upon substr

295 were measured to capture motions across the ps to ms timescale.

296 roteins are, on average, more dynamic in the ps-ns timescale than any soluble protein characterized t

297 Whereas excited-state events on the ps timescale have been structurally characterized, confo

298 ata suggests that the dynamics occurs on the ps-ns time scales as verified by measurements of R(1rho)

299 ations take place within a few hundred fs to ps, using a 3D imaging and laser pump-probe technique.

300 se proton radiography probed the target with ps order temporal and 10 mum spatial resolution, reveali