ライフサイエンスコーパス: ns

1 ormational microstate transitions on the 1.0 ns to 10.0 mus timescales were observed, with post-equil

2 ground state occurs in tauCR = 1.12 +/- 0.01 ns with no evidence of triplet excited state formation.

3 a robust response to T ( approximately 0.037 ns/K).

4 A lifetime of 4.49 +/- 0.04 ns was found for 1a organic NPs in water saturated with

5 rates of 5.91+/-0.60 ns(-1) and 1.03+/-0.09 ns(-1) respectively), ultrafast hole transfer occurs onl

6 nce lifetime of Spinach-DFHBI is 4.0 +/- 0.1 ns irrespective of the extent of photoconversion.

7 placements and protein resilience on the 0.1 ns timescale demonstrate that the L-type state is more f

8 , local piezostrains (rise/release time <0.1 ns) on the Pb(Zr,Ti)O3 film surface.

9 siently-with a lifetime in the region of 0.1 ns.

10 pace biexciton Auger recombination (0.01-0.1 ns; ref.

11 nts involving spherical quantum dots (0.12-1 ns; refs 7-9) do not outpace biexciton Auger recombinati

12 ) with an excited-state lifetime of 13 +/- 1 ns.

13 cay components with lifetimes of 0.5 and 3.1 ns.

14 , the fluorescence lifetime decreased to 3.1 ns.

15 e' = 660 ps in the mixture versus 1/ke = 4.1 ns in g-C3N4 alone.

16 29.4% and with a minimum pulse width of 5.1 ns.

17 and exhibits a fluorescence lifetime of 5.1 ns.

18 idues, with a prevalence of motions around 1 ns in the IDR.

19 dominant mode occurs on time scales around 1 ns, apparently reporting on backbone sampling within Ram

20 is (3)MLCT(SQ) state is very short-lived (<1 ns) as expected from the energy gap law for nonradiative

21 aration and it is relatively short-lived, <1 ns.

22 it excited-state lifetimes on the order of 1 ns and remarkably large excitonic g-factors of 10.

23 a high speed photodetector (rise time of ~1 ns) and applied to remove ringing distortions from imped

24 The modeling protocol was based on 1 ns Langevin dynamics simulation.

25 Longer than 1 ns lifetimes for holes photoexcited to the lower valence

26 length scales (85-340 nm) and timescales (1 ns-1mus) that we examine, we use recently developed meth

27 atalyst (Ru(2+) --> Ru(3+)) on a 100 ps to 1 ns timescale.

28 Despite a short lifetime of 22.1(1) ns, the anion exhibited a photoluminescence quantum yiel

29 yields up to 0.81(2) and lifetimes to 117(1) ns.

30 l electron configurations such as (n-1)d(g-1)ns(1) or (n-1)d(10)ns(2)np(1).

31 spontaneous emission with lifetimes of 1-10 ns, creating a mismatch with high-speed nanoscale optoel

32 roethanol (lambda = 580 nm, tau = 690 +/- 10 ns).

33 V and 7 ns-and loose cuts-350-700 keV and 10 ns.

34 r laser (193 nm wavelength, approximately 10 ns pulse duration) usually used with the instrument.

35 s of 170 nA currents over a approximately 10 ns timescale.

36 of excimers and a slower ( approximately 10 ns) break up of the excimer to two triplet exciton-beari

37 *)) state has a lifetime of approximately 10 ns, while CdS(+*):ExBox(3+*) recombines with multiple ti

38 Occurring in ca. 10 ns, this NR red-shift was caused by the formation of an

39 tter convergence of sampled states during 10 ns simulations compared to 20 times longer standard MD s

40 ency nuclear noise, responsible for fast (10 ns) inhomogeneous dephasing, can be removed by echo tech

41 here the iSF occurs with a time constant >10 ns, comparable to the fluorescence lifetime, we used ele

42 (6.0 x 10(8) M(-1) s(-1)) and half-life (10 ns) of CO2(*-) can be evaluated by fitting the collectio

43 +*) was found to be nonluminescent, tau < 10 ns.

44 o, completely eliminating shorter-lived (<10 ns) emission signals from organic chromophores or tissue

45 At small observation times (<10 ns) particle vibrations dominate phospholipid diffusion

46 n 1 micrometer, and carrier life-times of 10 ns and 120 ns for CH3NH3PbI3 and CH3NH3PbI(3-x)Clx, resp

47 found that laser pulses on a timescale of 10 ns rapidly heat carbon nanoparticles to temperatures on

48 approximately 0.5 for times of less than 10 ns.

49 polarization without any ions with (n-1)d(10)ns(0), d(0), or stereoactive lone-pair electrons.

50 ations such as (n-1)d(g-1)ns(1) or (n-1)d(10)ns(2)np(1).

51 The calculated pKa values based on 10-ns sampling per replica have the average absolute and ro

52 the TT to be thermally dissociated on 10-100 ns timescales to form free triplets.

53 urations at average time intervals of 50-100 ns.

54 ump experiments reveal time scales of 70-100 ns for fraying and 10-30 mus for complete dissociation n

55 protein during the passage time of about 100 ns.

56 scale for the seventh helix G approaches 100 ns.

57 on of spins is possible on approximately 100 ns timescales.

58 d by a single long-pulse ( approximately 100 ns) irradiation of an Al target in water.

59 del quality and stability was checked by 100 ns of molecular dynamics simulations previously to the v

60 del quality and stability was checked by 100 ns of molecular dynamics simulations.

61 ime scale of the hyperfine coupling (ca. 100 ns).

62 e photoluminescence (PL) with long tau > 100 ns excited state lifetimes.

63 Three long lasting (>100 ns) meta-stable states were apparent in the presence of

64 rich tapestry of motion on both short (<100 ns) and long (>1 ms) timescales.

65 orientational correlation time of nearly 100 ns.

66 Dynamics simulation study consisting of 100 ns simulations of 172 different complexes.

67 lar dynamics simulations on the order of 100 ns to study the mechanisms of the pH-responsive gelation

68 4 zwitterionic lipids, is monitored over 100 ns in all atom molecular dynamics simulations.

69 d open-state stabilization, we performed 100 ns molecular dynamics simulations of S100A1 in the apo/h

70 ependent molecular dynamics simulations (100 ns each) are performed to identify its favorable conform

71 s of the protein were extracted from the 100 ns simulation and were used for an ensemble docking camp

72 energic receptor through a total of 12 x 100 ns molecular dynamics simulations.

73 oke myosin then relaxed the complex by a 100-ns long unrestrained molecular dynamics.

74 The binding groove opens on a 100-ns timescale in a highly nonexponential manner, and the

75 We performed multiple 100-ns molecular-dynamics (MD) simulations and elastic netwo

76 The results of 100-ns simulations in explicit bilayers corroborate the high

77 ation status over multiple replicates of 100-ns simulations.

78 scopy in the 340-650-nm range and in the 100-ns to 3-s time window.

79 We also compared to a 1000 ns molecular dynamics simulation of a non-binding peptid

80 G (GB3), which was extrapolated to 371+/-115 ns at 310 K.

81 olvent selectivities, range from 250 to 1150 ns with identical lifetimes for 11a and 11f.

82 12-ns stimuli at 4.1-11 kV (3.3-8.8 kV/cm) evoked APs simil

83 50 Hz or 100 Hz for 1 min) alternately by 12-ns PEF and by conventional pulses.

84 a peripheral nerve can be accomplished by 12-ns PEF without electroporation.

85 ve damages even from tens of thousands of 12-ns stimuli and the similarities with the conventional st

86 ter, and carrier life-times of 10 ns and 120 ns for CH3NH3PbI3 and CH3NH3PbI(3-x)Clx, respectively.

87 tumbling with a correlation time tauc of 120 ns.

88 ith a charge separation time constant of 125 ns.

89 ealed an effective hole hopping rate of (130 ns)(-1).

90 me of BaP fluorescence was measured to be 14 ns in N,N-dimethylformamide, an average of 7 ns in Bold'

91 Bipolar NEFO was a damped sine wave with 140 ns first phase duration at 50% height; the peak amplitud

92 al-correlation-time component (1.37 +/- 0.15 ns), independent of global tumbling, represents a charac

93 For this purpose, we ran triplicate 150 ns molecular dynamics simulations of cTnI-R145G Ca(2+)-b

94 single acceptor time constants as fast as 16 ns to as slow as 0.13 ms.

95 e ruthenium bound to the DNA mismatch is 160 ns versus 35 ns when bound to a matched site.

96 teristic emission lifetimes of more than 160 ns, while shorter-lived cytoplasmic emission is also obs

97 ulation of a relatively long-lived (tau = 19 ns) Ru(dpi) --> qdpq(pi*) (3)MLCT excited state where th

98 and in-out motions on short time scales (0.2 ns).

99 I(-*) that recombines in tauCR = 1.2 +/- 0.2 ns, which is >100 times longer than that in the monomeri

100 longer in the aggregated state (taucra > 1.2 ns) as compared to that of monomeric dyad (taucrm < 110

101 The trapping is shown to last for 1.2 ns, which is long enough to establish conditions for flu

102 erature, and its excited-state lifetime (2.2 ns in deaerated THF at 20 degrees C) is nearly 2 orders

103 constants ranging from (800 ps)(-1) to (2.2 ns)(-1), which are 1-2 orders of magnitude faster than p

104 lectron to the adenine moiety in 12 ps and 2 ns, respectively.

105 rrier transport of approximately 220 nm in 2 ns for solution-processed polycrystalline CH3NH3PbI3 thi

106 Ioff ratio (>5400), fast switching speed (<2 ns), and high operating temperature (>453 K) characteris

107 monstrated 75 qubit rotations in less than 2 ns.

108 time was determined in the range of 1.5 to 2 ns by spectral analyses which enable separation of the F

109 GFP lifetimes consistently decreased (3 to 2 ns) with inoculation time.

110 ranges from 2 to 25 ps, and from 100 ps to 2 ns, using two spectrometers.

111 IE of 1 determined in the time range from 20 ns to 5 ms is incompatible with early deprotonation of E

112 +) and TiO2(e(-)) was followed by rapid (<20 ns) nearest-neighbor -Ru(II)OH2(2+) to -Ru(III)P(3+) ele

113 Twenty 20 ns straightforward simulations at several load levels re

114 With 20 ns time resolution, transient absorption measurements re

115 Similar time scales of roughly 100-200 ns are estimated for the B-C and F-G loops.

116 el change occurs on the timescale of 100-200 ns before the proton-loading site is protonated.

117 The four pores relaxed to toroidal by 200 ns, only one porelike structure containing two transmemb

118 d and all peptides were surface-bound by 200 ns.

119 he local carrier lifetimes are long (ca. 200 ns) and surprisingly homogenous among grains, and unifor

120 ational changes rise with a half-life of 200 ns, silent to UV/vis but detected by IR spectroscopy.

121 (>6.5 ns) than intrinsic recombination (~200 ns) causing considerable PL enhancement.

122 d (<1 ps) as well as slower relaxation (~200 ns) while homoleptic clusters (e.g., Au(10-12)GSH(10-12)

123 erimental-molecular dynamics simulation (200 ns) approach.

124 the threshold voltage shift in less than 200 ns.

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

126 state Re(I) with biexponential kinetics, 220 ns and 6 mus.

127 an substates, while a slower component (5-25 ns) reports on segmental dynamics dominated by the chain

128 ional changes (the CTT release) on short (25 ns) timescales.

129 ields a 1,064.58-nm-wavelength pulse with 25-ns duration and 1.1-kW peak power at a 1-kHz repetition

130 xplored the pulse-duration space between 250 ns and 100 mus and determined the lethal electric field

131 ure of T = 298 K and midfolding time t = 250 ns, the fraction of structures in the native-state (alph

132 hen decays with time constants of 63 and 270 ns, respectively.

133 he upper limit, i.e., between 27 mus and 270 ns.

134 hort as 0.5 ns but can be extended up to 270 ns.

135 lifetime (tauS) of 4.7 ns in toluene and 1.3 ns in benzonitrile.

136 m initial nonpolar S3(FC) to long-lived (1.3 ns in n-hexane and 3.4 ns in acetonitrile) polar S1.

137 A fast overall switching time of about 2.3 ns is also demonstrated.

138 fluorescence lifetime in RNA duplexes is 4.3 ns and generally two lifetimes are required to fit the e

139 y-NDI and TAPD-Ru, as it passes from about 3 ns in each dyad to 850 ns in the tetrad.

140 oton transfer from TsOH (tau approximately 3 ns for the first step).

141 hole potential, spanning time scales from 3 ns to 8 ps over a approximately 1 V increase.

142 ximately 350 devices), fast switching (</=30 ns), excellent endurance ( approximately 10(12) cycles),

143 nsition occurs within simulation times of 30 ns and depends on both temperature and NC size.

144 Six 30 ns molecular dynamics (MD) simulations of maize and barl

145 ively, while charge recombination in ca. 300 ns.

146 han 75% lethality in nsEP-treated cells (300 ns, 1.8-7 kV/cm, 50-700 pulses).

147 The thermal chirp during 300 ns pulses was about 1.2 cm(-1) and allowed scanning of r

148 y protegrin arcs are stable for at least 300 ns.

149 expressing cells, a train of 120 pulses (300 ns, 20 Hz, 6 kV/cm) decreased cell survival to 34% compa

150 1gamma2 protein reoriented itself within 300 ns.

151 was created by a train of 200 to 600 of 300-ns pulses (50 Hz, 300-600 V) delivered by a two-needle p

152 lectroporation was achieved by bursts of 300-ns, 9 kV/cm pulses (50 Hz, n = 3-100) and quantified by

153 al cause of cell death induced by 60- or 300-ns pulses in U937 cells is the loss of the plasma membra

154 In HEK 293 cells treated with a single 300-ns pulse of 25.5 kV/cm, Tmem16f expression knockdown and

155 rate quantum control over these states in 32 ns, which is orders of magnitude faster than previous ex

156 dynamics simulations extending up to 200-330 ns reveal that Lys-377 (helix XI) interacts with the ani

157 ound to the DNA mismatch is 160 ns versus 35 ns when bound to a matched site.

158 s as it possesses a fast tuning time of 0.36 ns, a low pump light intensity of 9.6 muW/mum(2), and a

159 A long rotational correlation time of 36 ns was observed for the excited states of the ACs bound

160 e phase transition temperature) in just 0.37 ns with a low light intensity of 95 nW/mum(2), owing to

161 maximum) and longest lifetime (tauavg = 1.39 ns).

162 on time scales of approximately 2 ps and 0.4 ns, respectively, when excited at higher energies (e.g.,

163 pears to be kinetically limited to 1.4+/-0.4 ns.

164 olymers showed long lifetimes of 1.6 and 2.4 ns for PNSW and PNTPD, respectively, while PNPDI and PEC

165 amorphous phase on shock release in only 2.4 ns from 33.6 GPa.

166 ence lifetimes were observed between 1.8-2.4 ns.

167 C) to long-lived (1.3 ns in n-hexane and 3.4 ns in acetonitrile) polar S1.

168 re ignited by ultraviolet laser (355 nm, 6.4 ns) pulses.

169 antum yields above 80% and lifetimes above 4 ns.

170 units in ca. 240 ps and recombines in ca. 4 ns.

171 al pulse in a radio-frequency burst within 4 ns, achieving a reconfiguration speed three orders of ma

172 ited ground state coherence time of about 40 ns.

173 -0.001 and a reset time of approximately 400 ns.

174 decylphosphocholine micelle, followed by 400 ns of all-atom molecular dynamics simulation, saw severa

175 explicit solvent (total simulation time >400 ns).

176 .29, and fluorescence lifetimes from 3 to 42 ns.

177 the shorter lived EGFP emitting state (2.43 ns) to the longer lived (ca. 2.77 ns) minority component

178 YE remained in this state throughout our 450-ns simulation.

179 4.4 cm(2) V(-1) s(-1) with a lifetime of 484 ns in the bulk of the single crystal.

180 triplet pair lifetime can be as short as 0.5 ns but can be extended up to 270 ns.

181 n bubble dynamics are imaged at times of 0.5 ns to 50 mus after the pulsed laser microbeam irradiatio

182 ly 18.3 +/- 0.8 to approximately 7.6 +/- 0.5 ns) after releasing of pressure from 11 GPa.

183 plex (3)MLCT state to the hexayne (tau = 1.5 ns).

184 inescence lifetimes of approximately 0.8-1.5 ns.

185 nd minority carrier lifetimes as long as 2.5 ns.

186 on-SP coupling takes place much faster (>6.5 ns) than intrinsic recombination (~200 ns) causing consi

187 minately rebinds to the 5c heme (tauG2 = 6.5 ns), whereas the other diffuses out to the solution, fro

188 an excited-state lifetime of tau = 65 +/- 5 ns.

189 o autofluorescence with lifetimes of about 5 ns in the visible spectrum.

190 ngle-file water chains through transient (<5 ns) tunnels or pores.

191 ol and that K(+) ions bind transiently (</=5 ns) and nonspecifically (nine different positions) to th

192 witched pulse output with a pulse width of 5 ns and peak power of 255 W was achieved in the 10-mm-lon

193 entanglement between photons emitted up to 5 ns apart, exceeding the exciton lifetime.

194 Two 1.5-ns-long comprehensive evolution portraits are reconstruc

195 one are loosened rapidly compared with the 5-ns temperature jump.

196 sicles is observed to occur in as fast as 50 ns, with a temperature dependence characteristic of crit

197 transient absorption, time-resolved EPR (50 ns), photo-chemically induced dynamic nuclear polarizati

198 s from the longer time-scale bulk value (>50 ns) of 8.5x10(-7) cm(2) s(-1).

199 mophore leads to prompt Cu(I) oxidation (<50 ns), followed by slow back ET to regenerate Cu(I) and gr

200 The PL has a lifetime of 50 ns, almost 2 orders of magnitude shorter than small PbS

201 ds are long lived, showing decay times of 50 ns, and forming strings of lipids, and leading to reorie

202 speed emission spectroscopy revealed that 50 ns after flyer plate impacts, an emission pulse was gene

203 A 500 ns long molecular dynamics simulation of PI-PLC at the s

204 The first spectrum at 500 ns shows major contributions from the FAD anion radical,

205 ur for slow motions with motions in the >500 ns range being more prevalent in the complex.

206 one of the enzymes is indicated over the 500 ns timescale.

207 eometry and electron-transfer kinetics of 51 ns.

208 d ester of 8a, generates the long-lived (530 ns) nitrenium ion 11a by hydrolysis or photolysis in wat

209 nusually long excited state lifetime of 13.6 ns.

210 ernal friction (ZIF), a large offset of 81.6 ns is needed as an addition to all relaxation times due

211 e data, combined with data from studies of 6 ns microbeam irradiation, demonstrates the primacy of sh

212 after a single electric pulse lasting only 6 ns.

213 A single 6 ns laser pulse (lambda = 532 nm) was used to pattern an

214 The optimal coincidence time window was 6 ns for the MiniPET-2 and 8 ns for the MiniPET-3.

215 the 5-CT triplet (with rates of 5.91+/-0.60 ns(-1) and 1.03+/-0.09 ns(-1) respectively), ultrafast h

216 es along with its persistence of about 50-60 ns makes this dyad a potential electron-transporting cat

217 AA-MD simulations were then conducted for 60 ns, starting from different initial CG structures, to re

218 e sampling (16 replicas per sequence and 600 ns per replica), we investigate the structure of the mon

219 r, and 1-Cy with lifetimes of 24, 67, and 61 ns, respectively.

220 A lower bound of spin dephasing time of 63 ns is extracted.

221 l photoluminescence (PL) lifetime of ca. 660 ns, which is very encouraging for photovoltaic applicati

222 er, high-spin quartet state, persists for 67 ns due to spin-forbidden back-electron transfer, constit

223 RNG bias, for random bits produced up to 690 ns too early by the random number generator.

224 P-PMI has an S1 lifetime (tauS) of 4.7 ns in toluene and 1.3 ns in benzonitrile.

225 ght energy and timing cuts-400-650 keV and 7 ns-and loose cuts-350-700 keV and 10 ns.

226 ns in N,N-dimethylformamide, an average of 7 ns in Bold's basal medium, and 8 ns in Chlorella cells.

227 observed fragment motion on a timescale of 7 ns with motional amplitudes of about 1 nm relative to ea

228 s of a fast photobisdecarbonylation within 7 ns from the triplet and singlet states of 2 and a lack o

229 th a lambdamax= 570 nm with a lifetime of 70 ns.

230 find that the S1 state has a lifetime of ~70 ns and undergoes intersystem crossing (ISC) to the T1 st

231 )6 and W(CNIph)6 with lifetimes of 17 and 73 ns, respectively.

232 tate (2.43 ns) to the longer lived (ca. 2.77 ns) minority component (ca. 16%) of the optically excite

233 radical undergoes extremely rapid (tau = 77 ns) formate dissociation accompanied by a free valence s

234 asure an interlayer exciton lifetime of ~1.8 ns, an order of magnitude longer than intralayer exciton

235 th correlation times ranging from 1.0 to 1.8 ns.

236 The excimer state then decays in 6.9-12.8 ns, as measured by time-resolved fluorescence spectrosco

237 pectral coverage (350-750 nm) and tauS = 2.8 ns in toluene and 30 ps in benzonitrile.

238 , and Ax330 are all markedly slower (2.3-2.8 ns) in Galphai1:Ric-8A than in Galphai1*GXP, and only mo

239 t decays with time constants of 0.28 and 5.8 ns and does not transfer energy to PSI or to PSII.

240 16% and an excited-state lifetime of 7.7-7.8 ns.

241 time window was 6 ns for the MiniPET-2 and 8 ns for the MiniPET-3.

242 verage of 7 ns in Bold's basal medium, and 8 ns in Chlorella cells.

243 intermediate radical pairs within the ca. 8 ns laser pulse of our laser setup.

244 , an explicit solvent MD simulation over 800 ns was run on r[5'GGGC(CAG)3GUCC]2, which closely repres

245 in complex with Gs (beta2AR-Gs), through 824-ns duration molecular dynamics simulations in a fully hy

246 quency resolution defined by its inverse (85 ns and 24 MHz respectively are demonstrated).

247 t passes from about 3 ns in each dyad to 850 ns in the tetrad.

248 rescence lifetimes that range from 30 to 860 ns, depending on the type of interface between the core

249 asure a spin coherence time, T2*, of 115+/-9 ns at 3.6 K.

250 ge recombination takes place over sub-ns and ns time scales.

251 tively model the experimental data at ps and ns respectively.

252 me-tagging accuracy limited to approximately ns.

253 tive ET quenching by Fe(2+)cyt b5 as well as ns-time scale oxidative ET quenching by Fe(3+)cyt b5, bo

254 Peptides corresponding to 4 common ns-SNPs showed limited binding to 11 HLA-DRB1 proteins.

255 of demise of both Tc and superfluid density ns on the overdoped side is a major puzzle.

256 on timescales between around 10 ps and a few ns (corresponding to the instrumental range).

257 of 10(5)-10(6) m(-1) that lasts up to a few ns depending on the film thickness.

258 tion when polydisperse, laboratory-generated ns-soot particles were embedded within or coated with am

259 High flux of water (up to 13,000 molecules/ns) is obtained by the electro-mechanical, piston-cylind

260 UGIB during concomitant use of nonselective (ns)NSAIDs, cyclooxygenase -2 selective inhibitors (COX-2

261 ove on relatively slow timescales of tens of ns to sub-mus to be directly involved in binding and rec

262 (22.2%; P = 0.001) and mortality (3.7%; P = ns) were higher.

263 her urge to drink juice or food craving (p = ns).

264 differences in side effects were found (p = ns).

265 8.8%], DJBL versus control respectively (P = ns).

266 20 years postvaccination, respectively, (P = ns).

267 s than in lymphoma (U = 15.0; two-tailed p = ns).

268 and 534 (279) seconds for those without (P = ns).

269 er various conditions using fixed P(s) and P(ns) values derived for the rat.

270 g characteristic curves, 0.90 versus 0.87; P=ns).

271 in scores remained similar (3.97 vs. 3.87; P=ns).

272 between days 7 and 21 (1.8+/- versus 3.8; P=ns), Gd-ESMA showed markedly higher CNR on day 21 after

273 , and 71.0%, 70.1%, 63.6% in the ID group (p=ns).

274 versus 1209.0+/-64.6/mm(2) in eMSC group; P=ns).

275 nsynonymous single-nucleotide polymorphisms (ns-SNPs) in the F8 gene encoding FVIII-H484, FVIII-E1241

276 -synonymous single nucleotide polymorphisms (ns-SNPs) in the F8 gene occur as six haplotypes in the h

277 ionship between motions on the mus-ms and ps-ns timescales in CheY.

278 aling proteins through modulation of fast ps-ns sidechain dynamics.

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

280 5)N relaxation studies show a decrease in ps-ns backbone dynamics in the free state of consensus-HD,

281 methyl groups with the largest changes in ps-ns dynamics localize to the regions of conformational ch

282 The limited spread of changes in ps-ns dynamics suggests a distinct relationship between mot

283 mescale and the picosecond-to-nanosecond (ps-ns) timescale.

284 c residues in RNase H are preorganized on ps-ns time scales via a network of electrostatic interactio

285 n injection into TiO2, followed by rapid (ps-ns) and sequential two-electron oxidation of TEOA that i

286 The ps-ns motions were not significantly altered upon substrate

287 as greater flexibility than EcDHFR on the ps-ns time scale, which affects the coupling of the environ

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

289 adenovirus (Ad-TD) to deliver non-secreting (ns) IL-12 to tumor cells and examine the therapeutic and

290 Fresh kerosene nanosphere soot (ns-soot) exhibited a mean M.A.C and standard deviation o

291 measured, by K-edge absorption spectroscopy, ns-lived equilibrium states of WDM Fe.

292 le charge recombination takes place over sub-ns and ns time scales.

293 nelastic reorganization ([Formula: see text] ns), and structural relaxation ([Formula: see text]s).

294 ribing elastic response ([Formula: see text] ns), inelastic reorganization ([Formula: see text] ns),

295 by transient absorption spectroscopy in the ns-mus time regime.

296 , but this did not correlate with any of the ns-SNPs.

297 reveal that Y731 changes conformation on the ns-mus time scale, significantly faster than the enzymat

298 t technique with time resolution down to the ns scale, opening a new door to in-situ structure-proper

299 ited singlet state of MMb ((1)MMb) undergoes ns-time scale reductive ET quenching by Fe(2+)cyt b5 as

300 rom regions of the Factor VIII protein where ns-SNPs occur and showed that these wild type peptides f