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 rom the macrocycle to the hexayne (tau = 3.0 ps), whereas in the rhenium-rotaxane there is triplet EE

4 mulations with high sampling frequency (0.01 ps), to identify amino acid residue hubs whose global co

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

6 agnetoelectric coupling coefficient of 0.057 ps/m.

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

8 find fourfold prolonged values up to T2=2.1 ps compared with ensemble measurements.

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

10 After 1 ps, 10% of the CO populate the TS region, which is consi

11 f stepwise electron transfer with 3 ps and 1 ps time constants.

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

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

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

15 ate of the hexayne (lifetime approximately 1 ps) and on structural reorganization and cooling of hot

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

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

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

19 tungsten disulfide transfer to graphene in 1 ps and with near-unity efficiency.

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

21 The excimer-state absorption appears in ~1 ps, followed by conformational relaxation over 8-17 ps.

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

23 w that triplets transfer to PbSe rapidly (<1 ps) and efficiently, with 1.9 triplets transferred for e

24 H18) with core-metal atoms display rapid (<1 ps) as well as slower relaxation (~200 ns) while homolep

25 that addresses the origin of ultra-fast (<1 ps) dissociation by incorporating exciton delocalization

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

27 ttraction to generate free carriers within 1 ps.

28 We demonstrate a ~1-ps free-carrier-induced pulse acceleration and show that

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

30 e with a time constant tau(His) = 100 +/- 10 ps (k(His) = 10(10) s(-1)) after the release of NO from

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

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

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

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

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

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

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

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

39 to the parent complex on a time scale of 10 ps.

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

41 lectron temperature and its decrease over 10 ps.

42 0-30 ps lifetime, except for ReGV-PhNMe2 (10 ps in CH2Cl2, 100 ps in MeCN).

43 plete ionization did not occur during the 10 ps simulation, distinct correlations among the extent of

44 show any drastic structural changes up to 10 ps.

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

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

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

48 s of magnitude faster than tetracene (10-100 ps) but significantly slower than pentacene (80-110 fs).

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

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

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

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

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

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

55 except for ReGV-PhNMe2 (10 ps in CH2Cl2, 100 ps in MeCN).

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

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

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

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

60 0.73)(N0.27O0.73) NCs has both a short (<100 ps) and a long-lived component, with a long overall aver

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

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

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

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

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

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

67 y, the dipolar dynamics in the 100 fs to 100 ps range were unchanged with pH, although nanosecond yie

68 e scale from hundreds of femtoseconds to 100 ps.

69 cleotides show long-living states on the 100-ps time scale, which are not observable in a mixture of

70 extraction with the presence of GQDs (90-106 ps) than without their presence (260-307 ps).

71 ere transferred with a time constant of 1087 ps.

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

73 spectral acoustic phonon lifetime of 30-110 ps and mean free path of 0.5-2.5 mum exceed those for gr

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

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

76 uring dynamic relaxation is obtained as 0.13 ps.

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

78 mperature residence time of approximately 14 ps.

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

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

81 1 states having lifetimes approximately 5-15 ps.

82 state show good agreement with data after 15 ps.

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

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

85 equilibrates with the environment in 100-150 ps.

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

87 740 nm, we observe a final approximately 150 ps decay assigned to trapping by charge separation, and

88 tion time that ranges from approximately 150 ps to many nanoseconds, depending on the electric field

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

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

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

92 BT-I reduced levels of CRP (months 4 and 16, ps < .05), monocyte production of proinflammatory cytoki

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

94 lowed by conformational relaxation over 8-17 ps.

95 hole transfer time constants as fast as 170 ps.

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

97 constants in the film samples (tau=0.8+/-0.2 ps and tau=23+/-3 ps), which is attributed to structural

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

99 An even earlier ( approximately 0.2 ps) transient is observed and tentatively assigned to a

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

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

102 t manifold on time scales of approximately 2 ps and 0.4 ns, respectively, when excited at higher ener

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

104 ly after photoexcitation and dissociate in 2 ps forming highly mobile charges (25 cm(2) V(-1) s(-1))

105 ocalization and energy relaxation occur in 2 ps.

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

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

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

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

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

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

112 of Cu-CO reveals unprecedented ultrafast (2 ps) nonequilibrium structural rearrangements launched by

113 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.

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

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

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

117 y formed hot and relax with approximately 20 ps lifetime.

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

119 nd a fluorescence lifetime shortening to ~20 ps.

120 opulated on a timescale of approximately 200 ps by recombination with NO ligands.

121 (8 GHz-12 GHz), and a time resolution of 200 ps (6 cm optical path in free space).

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

123 ynamics of the membrane from ~200 fs to ~200 ps as a function of the number of water molecules hydrat

124 ionic diffusion are ruled out within a 1-200-ps time window.

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

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

127 ow that interplate FRET ( approximately 6-23 ps, presumably for co-facial arrangements) can occur 15-

128 ne of the extended viologen units in ca. 240 ps and recombines in ca. 4 ns.

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

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

131 randomization occurring in approximately 25 ps.

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

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

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

135 scenario with highly mobile core water (~25 ps average rotational correlation time).

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

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

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

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

140 ilm samples (tau=0.8+/-0.2 ps and tau=23+/-3 ps), which is attributed to structural disorder within t

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

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

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

144 l ground state is then restored within ca. 3 ps.

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

146 itation and proton transfer that lives for 3 ps.

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

148 vior is consistent with rapid (faster than 3 ps) hole trapping by gold-sulfur sites at the surface of

149 picture of stepwise electron transfer with 3 ps and 1 ps time constants.

150 ssion with a dominant time constant of 10-30 ps and without strong thermal activation.

151 h a solvent-independent (CH2Cl2, MeCN) 20-30 ps lifetime, except for ReGV-PhNMe2 (10 ps in CH2Cl2, 10

152 -750 nm) and tauS = 2.8 ns in toluene and 30 ps in benzonitrile.

153 PT) with a time constant of approximately 30 ps (6 times slower than wild-type GFP) to reach the gree

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

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

156 er shows these structures interconvert in 30 ps.

157 We execute short timescale (30 ps) molecular dynamics simulations with high sampling fr

158 ated with the protein interface for up to 30 ps yet free to rotate at approximately "bulk" water rate

159 The transients at 70 and 300 ps are identical, but they deviate from the difference b

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

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

162 106 ps) than without their presence (260-307 ps).

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

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

165 repopulates the ground state with tau = 362 ps.

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

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

168 induced CS reaction (tauCS approximately 0.4 ps, PhiCS approximately 0.97).

169 ate of the exciton radiative lifetime of 0.4 ps.

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

171 verage coincidence time resolution was 375.4 ps FWHM.

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

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

174 ential ME coefficients on the order of 10(4) ps/m are achieved.

175 is followed by much slower approximately 40 ps vibrational relaxation typical of metal-CO vibrations

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

177 n the singlet manifold on a time scale of 40 ps; in contrast, cis-to-trans isomerization is not obser

178 -ring of this Russian doll complex within 40 ps.

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

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

181 ile the return to the ground state takes 450 ps.

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

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

184 The slow hot carrier relaxation time is 0.5 ps.

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

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

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

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

189 experimental evidence for the ultrafast (3.5 ps), polarity-independent and viscosity-dependent planar

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

191 ), the corresponding values are 0.16 and 7.5 ps, respectively.

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

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

194 ng internal conversion (over approximately 5 ps).

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

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

197 nular magnetic field profile was observed 5 ps after the interaction, indicating a relatively smooth

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

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

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

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

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

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

204 a surprisingly long lifetime of more than 50 ps, and a simultaneous transient shift of chemical poten

205 e-resolved magnetic X-ray microscopy with 50 ps temporal resolution and 35 nm spatial resolution, we

206 her structural evolution on less, similar 50-ps timescales is modest, indicating that the polymer con

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

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

209 he LMCT state, which has a approximately 500 ps lifetime, as well as that of a precursor d-d excited

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

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

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

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

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

215 achieve compression of 3.7 ps pulses to 1.6 ps with <10 pJ energy.

216 ate from the (3)MLCT state occurs within 1.6 ps, while the return to the ground state takes 450 ps.

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

218 ization, which occurs with a lifetime of 3.6 ps, the phycoviolobilin twists or distorts slightly with

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

220 ecombination exhibits a 50% decay time of ~6 ps, ~10(3) times faster than that of TiO2 under comparab

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

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

223 Charge recombination occurs in 60 ps before the O radical cation can lose a deuteron to wa

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

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

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

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

228 IR) fiber laser of 1 MHz repetition rate, 65 ps pulse duration, and 1 cm(-1) spectral resolution to r

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

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

231 4 decays with a time constant of 1/ke' = 660 ps in the mixture versus 1/ke = 4.1 ns in g-C3N4 alone.

232 luctuations have time constants of 7 and 670 ps with no solvent.

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

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

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

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

237 Here we achieve compression of 3.7 ps pulses to 1.6 ps with <10 pJ energy.

238 NO rebinds with a time constant tau(NO) = 7 ps (k(NO) = 1.4 x 10(11) s(-1)) and shown that rebinding

239 and the excited state lifetime from 0.4 to 7 ps and activates previously inaccessible reaction channe

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

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

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

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

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

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

246 tential, spanning time scales from 3 ns to 8 ps over a approximately 1 V increase.

247 and slow components of the FFCF of 5 and 80 ps, respectively.

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

249 ally long excited state lifetimes, up to 815 ps, in IFP1.4 and IFPrev.

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

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

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

253 nversion of singlets to triplet pairs is ~90 ps.

254 A melting speed of just 900 ps was achieved to perform multiple Boolean algebraic op

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

256 experienced seizures during their admission (ps<0.02).

257 atory cytokines (months 2, 4, 7, and 16; all ps < .05) and proinflammatory gene expression (month 4,

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

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

260 , and overnight retention of word pairs (all ps < 0.05).

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

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

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

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

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

266 ent absorption and the rapid ( approximately ps) nonradiative vibrational relaxation of molecular ele

267 uantitatively model the experimental data at ps and ns respectively.

268 aspects of executive function and attention (ps<0.04).

269 erved: on one hand, an ultrafast component (~ps) that relates to the excitons; on the other hand, a l

270 The derived FAPAR(ps) was then related to three vegetation indices (i.e. N

271 mine their potential as surrogates for FAPAR(ps) .

272 The maximum FAPAR(ps) from the inversion approach ranged between 0.6 and 0

273 Finally, the FAPAR(ps) was evaluated against two operational satellite data

274 ional FAPAR products overestimated the FAPAR(ps).

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

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

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

278 he distributions of the ES were homogeneous (ps > .90), and there was no indication of a publication

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

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

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

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

283 ytic residues in RNase H are preorganized on ps-ns time scales via a network of electrostatic interac

284 auses the appearance of electron trapping on ps-mus time scales.

285 DP+ differed significantly from each other (ps < .05) and the effect of smoking (versus abstinence)

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

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

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

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

290 score were decreased and increased (log-rank ps for trend: 6 x 10E-4 and 9 x 10E-45), respectively.

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

292 r time was greater for DP+ than DP- smokers (ps < .05).

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

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

295 We find two contributions with sub-ps lifetimes in line with recent excited-state QM/MM mol

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

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

298 R has greater flexibility than EcDHFR on the ps-ns time scale, which affects the coupling of the envi

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

300 worse and having problems with school work (ps=0.001), as well as performing below average on aspect