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 scale molecular simulations totalling 26 000 ns.

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

4 ce lifetimes (tau(F)) vary from 1.50 to 3.01 ns depending on the solvent polarity.

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

6 nct OCP-quenched states, with lifetimes 0.09 ns (6% of unquenched brightness) and 0.21 ns (11% bright

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

8 800 nm with a concomitant decay (4.1 +/- 0.1 ns) at 675 nm.

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

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

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

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

13 s expected with gate delays of 42.7 +/- 13.1 ns.

14 rong TPE emission with a lifetime of 4 +/- 1 ns, no significant changes were observed between measure

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

18 voltages below 500 mV at speeds as fast as 1 ns in 30 nm devices, thus opening a new realm of high sp

19 s resulting in reasonably fast PL decays (~1 ns), large vibrational energy spacing, small Stokes shif

20 to average over ~10-nm spatial scales for ~1 ns, which is prohibitively impractical with QM.

21 vering four decades of time, ranging from ~1 ns to ~mus, can be rationalized by a remodeling of its r

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

23 tal exhibits a fast decay time constant of 1 ns at 7 K.

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

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

26 decoherence effects at longer timescales (~1 ns).

27 g an unexpectedly long spin lifetime up to 1 ns.

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 amic motions of base pair mismatches (0.1-10 ns).

31 maintaining fluorescence lifetimes above 10 ns.

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

33 scence measurements reveal an approximate 10 ns lifetime for bright valence states.

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

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

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

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

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

39 ores, with a long fluorescence lifetime (>10 ns) and fluorescence beyond 550 nm, has been expanded wi

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

41 (6.0 x 10(8) M(-1) s(-1)) and half-life (10 ns) of CO2(*-) can be evaluated by fitting the collectio

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

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

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

45 approximately 0.5 for times of less than 10 ns.

46 rom 0.24 ns/lambda to 5 ns/lambda and 2 x 10 ns/lambda, respectively.

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

48 Here we present a study totalling 37 100 ns investigating the LC13 TCR in its free form as well a

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

50 mic motion is roughly 50 nm in space and 100 ns in time.

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

52 t high voltage pulse widths as narrow as 100 ns with a pulse-to-pulse delay of ~900 mus can significa

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

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

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

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

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

58 Decay to the ground state in 100 ns is the primary loss pathway for (1)TT in this system.

59 and retention, a high switching speed of 100 ns, ultralow readout conductance (<100 nS), and ultralow

60 (9) Jones along with a fast response of ~100 ns in the technologically relevant 8-12 um band.

61 4 zwitterionic lipids, is monitored over 100 ns in all atom molecular dynamics simulations.

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

63 erature (n(e) ~ 8 x 10(17) cm(-3) at t = 100 ns and T ~ 8000 K at t = 10 mus, respectively).

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

65 broad emission line shape is constant to 100 ns.

66 ly dissociates from tropomyosin in under 100 ns, whereas actin-tropomyosin and TnT1 models themselves

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

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

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

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

71 e fluorescence lifetime of (ts)T (tau = 4-11 ns) was shorter than its anisotropy decay in well-matche

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

73 12-ns stimuli at 4.1-11 kV (3.3-8.8 kV/cm) evoked APs simil

74 50 Hz or 100 Hz for 1 min) alternately by 12-ns PEF and by conventional pulses.

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

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

77 product reports on the lifetime (520 +/- 120 ns) of a reactive carboxyl radical in solution, and spec

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

79 ; 2.77 +/- 0.26 ns compared to 2.57 +/- 0.14 ns in KU60019-treated cells).

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

81 Moreover, fast switching speed (<15 ns) is demonstrated via pulse operation.

82 om silicon to anthracene through a single 15 ns Dexter energy transfer step with a nearly 50% yield.

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

84 ximum of 43% when the positive phase was 150 ns at 3.1 kV/cm, and the negative phase was 800 ns at 0.

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

86 arriers, which have super long lifetime (>17 ns), are responsible for the long-term photoconductivity

87 tum yields up to 0.03 and lifetimes up to 17 ns were observed.

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

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

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

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

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

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

94 extraordinarily large dynamic range with a 2 ns lifetime change from pH 5.5 to 9.0.

95 ults in cells exposed to ultrashort (6 and 2 ns) electric fields, suggesting that cellular electropor

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

97 ing of eight time steps evenly spaced over 2 ns.

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

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

100 The response was eliminated by a 2-ns bipolar pulse with positive and negative phases of eq

101 drenal chromaffin cells show that a single 2-ns, 16 MV/m unipolar pulse elicited a rapid, transient r

102 s feature long fluorescence lifetimes (17-20 ns), high quantum yields (~60%), and high photostabiliti

103 dow (amounting to 113,000 times noise per 20 ns detection period).

104 decay in well-matched duplex DNA (theta = 20 ns), yet longer than the dynamic motions of base pair mi

105 With 20 ns time resolution, transient absorption measurements re

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

107 ires on a compact L-C (40 kV, 200 kA and 200 ns) generator, and the time integrated spectra are recor

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

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

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

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

112 and solidification into nano-onions over 200 ns by analysis of time-resolved, small-angle X-ray scatt

113 hite phase transition for DNTF products ~200 ns post-detonation.

114 (>6.5 ns) than intrinsic recombination (~200 ns) causing considerable PL enhancement.

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

116 the threshold voltage shift in less than 200 ns.

117 The 200 ns simulations, validated by available experimental data

118 r data show that in vitro nsPEF (20-200, 200-ns pulses, 7 kV/cm, 2 Hz) caused a rapid dose-dependent

119 nity in animals treated with nsPEF (750, 200-ns, 25 kV/cm, 2 Hz) with animals were tumors were surgic

120 simulations over a total of 1 mus and a 200-ns enhanced correlation guided MD simulation.

121 09 ns (6% of unquenched brightness) and 0.21 ns (11% brightness).

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

123 r to REST (pre-REST) sampling time from 0.24 ns/lambda to 5 ns/lambda and 2 x 10 ns/lambda, respectiv

124 SAP1, with a global correlational time of 24 ns at 15 degrees C, a wide range of conformational dynam

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

126 ane potential at temporal resolutions of ~25 ns.

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

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

129 orylated form, NADPH (NAD(P)H; 2.77 +/- 0.26 ns compared to 2.57 +/- 0.14 ns in KU60019-treated cells

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

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

132 ence lifetime in DNA is unusually long (9-29 ns), facilitating its selective measurement in complex m

133 t 800 nm), and a delayed growth (6.5 +/- 0.3 ns) in the kinetics at 800 nm with a concomitant decay (

134 g thermodynamic data in the literature (~0.3 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 n spectra with fluorescence lifetimes of 1.3 ns, indicating the formation of a new (ground-state) hyd

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

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

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

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

142 n (160 +/- 40 ps), and (3) excimer decay (>3 ns).

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

144 er a nanometer distance (tau(shuttling) ~ 30 ns) reported to date.

145 tween each phase of the bipolar pulse was 30 ns.

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

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

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

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

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

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

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

153 e wavelengths, from 93 ns (at 650 nm) to 345 ns (at 800 nm), and a delayed growth (6.5 +/- 0.3 ns) in

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

155 The equilibrated states survive for 36 ns and are lost to ground state through both radiative a

156 (lambda(max) = 621 nm, = 0.32, tau(av) = 366 ns) thermally activated delayed fluorescence (TADF) emit

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

158 m and fluorescence lifetime shortened by 0.4 ns compared to uncalcified regions.

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

160 achieved an optimum ring-down time of 159.4 ns and a minimum absorption coefficient of alpha(min) =

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

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

163 ence lifetimes were observed between 1.8-2.4 ns.

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

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

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

167 to have a long-lived excited state (tau = 4 ns), which was computationally assigned as a metal-to-li

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

169 ited ground state coherence time of about 40 ns.

170 -0.001 and a reset time of approximately 400 ns.

171 drenal chromaffin cells to single 150 to 400 ns electric pulses triggers a rise in intracellular Ca(2

172 .29, and fluorescence lifetimes from 3 to 42 ns.

173 4.4 cm(2) V(-1) s(-1) with a lifetime of 484 ns in the bulk of the single crystal.

174 decay component varying between 0.08 and 0.5 ns - a feature that can be readily exploited for tempera

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

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

177 g power of 1000 and a time resolution of 0.5 ns.

178 53-nm pulse durations between 600 fs and 1.5 ns and nanosecond pulse excitation at 351 nm and 532 nm.

179 ge energy with the living samples on the 1.5 ns time scale, thereby excluding the signal from the hig

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

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

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

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

184 We extended the REST simulations from 5 ns to 8 ns to achieve reasonable free energy convergence

185 V cm(-1) and improving switching times to <5 ns for a 20 um diameter capacitor in a 100-nm-thick film

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

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

188 REST) sampling time from 0.24 ns/lambda to 5 ns/lambda and 2 x 10 ns/lambda, respectively.

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

190 rpulse intervals as short as 50 ns but not 5-ns intervals, consistent with the 10-50-ns lifetimes of

191 tive for interpulse intervals as short as 50 ns but not 5-ns intervals, consistent with the 10-50-ns

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

193 e series-coupled silicon quantum dots in ~50 ns via a series of pairwise interdot charge transfers.

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

195 relatively short all-atom simulations of 50 ns.

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

197 ot 5-ns intervals, consistent with the 10-50-ns lifetimes of electropores in MD simulations.

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

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

200 in alpha7 activation, we ran triplicate 500-ns molecular dynamics simulations with an alpha7 extrace

201 eometry and electron-transfer kinetics of 51 ns.

202 in each of them, that is, 1240, 740, and 56 ns for BTMPA-Im->AlPorF(5)-Ph-C(60), BTMPA-Im->AlPorF(3)

203 on lifetimes of CPA and its analogs (140-580 ns), and identified ring-opened products, support the us

204 long photoluminescence (PL) lifetime of 582 ns, while the intensity is constant over a very broad te

205 Following the rapid decay (0.6 ns) of a small spectral side band, the broad emission li

206 of the fluorescence lifetime from 4.3 to 2.6 ns.

207 = 0.48) with long fluorescence lifetime (5.6 ns) and large Stokes' shift, suggesting FH could be used

208 after a single electric pulse lasting only 6 ns.

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

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

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

212 were permeabilized by multiphasic nsEP (600 ns per phase) from two generators; these nsEP were synch

213 By applying a single 600-ns electric pulse, we observed sub-microsecond, continuo

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

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

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

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

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

219 1.27 eV and a long carrier lifetime of 657.7 ns.

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

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

222 esence of crowders using a long-duration (70 ns) classical molecular dynamic simulations.

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

224 ce cardioprotection (Prop-RIPC: 63% [56-70%] ns vs Prop-Con).

225 th correlation times ranging from 1.0 to 1.8 ns.

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

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

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

229 16% and an excited-state lifetime of 7.7-7.8 ns.

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

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

232 extended the REST simulations from 5 ns to 8 ns to achieve reasonable free energy convergence.

233 Nanosecond pulses with 400-800 ns duration are found effective on disrupting nuclear me

234 Compared to microsecond pulses, ~800 ns pulses can be used to increase the signal-to-noise an

235 at 3.1 kV/cm, and the negative phase was 800 ns at 0.2 kV/cm.

236 We ran 800-ns long molecular dynamics simulations of the PRD using

237 ristic energy transfer time to the dye of 81 ns, and thus must be determined by the excited state lif

238 The tau(fl) values range between 20 and 85 ns, and the tau(ph) values are in the 50-200 mus regime.

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

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

241 ring a unique pulse train structure with 886 ns between pulses.

242 within trains are currently separated by 889 ns.

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

244 atform, a cavity ring-down time of about 900 ns was obtained allowing spectroelectrochemical studies

245 times with longer probe wavelengths, from 93 ns (at 650 nm) to 345 ns (at 800 nm), and a delayed grow

246 programmed HB pacing correctly diagnosed all ns-HB cases and all RV myocardial pacing cases.

247 lography at an X-ray free-electron laser and ns-resolved pump-probe UV-visible spectroscopy.

248 me-tagging accuracy limited to approximately ns.

249 During permanent nonselective His bundle (ns-HB) pacing, it is crucial to confirm HB capture/exclu

250 activity (THAM 103%, HCO(3) 113% of NC cAMP, ns; Forskolin 168%, p < 0.05) and PM repair (THAM 87%, H

251 condition studies using dynamic compression (ns) or fast laser heating (ms).

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

253 that it should be possible to differentiate ns-HB capture from RV myocardial capture using programme

254 relatively long-duration laser pulses (i.e., ns or longer).

255 In RV myocardial-only pacing cases (false ns-HB pacing, n=14), such responses were not observed-th

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 abrupt change of paced QRS morphology: from ns-HB to RV myocardial QRS (34 of 36 cases) or to select

259 antify motions spanning a dynamic range from ns to ms.

260 XRD, AFM, XPS, NEXAFS, R-SoXS, TEM, STEM, fs/ns TA spectroscopy, 2DES, and impedance spectroscopy.

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

262 ese g4 and g7 strains contain nonstructural (ns) protein 3 and 5A polymorphisms associated with resis

263 HB QRS in patients with otherwise obligatory ns-HB pacing (RV myocardial capture threshold <HB captur

264 In 34 of 36 cases of ns-HB pacing, the RV myocardial ERP was shorter than HB

265 Zero-dimensional halides of ns(2) elements (Sn, Pb, Sb) have recently gained attenti

266 The beam duration of hundreds of ns to tens of [Formula: see text] is evaluated for neutr

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

268 correlate with CA19-9 (r = 0.049-0.141, p = ns).

269 score of, 35 for dCLKT and 34 for eCLKT (P = ns).

270 20 years postvaccination, respectively, (P = ns).

271 is, pulse steroids, IVIG, and rituximab (P = ns).

272 /-0.011 to 0.042+/-0.016 cm(-)(2) s(-)(1); P=ns) and failed to convert AF to sinus rhythm.

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

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

275 ologic MELD 35 for dCLKT and 34 for eCLKT (p=ns).

276 +/-6 (IST), 123+/-8 (POTS), 124+/-7 (VVS), P=ns.

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

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

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

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

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

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

283 eins are, on average, more dynamic in the ps-ns timescale than any soluble protein characterized to d

284 87%, HCO(3) 108% of NC likelihood to repair, ns; Forskolin 160%, p < 0.01).

285 ntermediates exchanging on a mus time scale (ns at room temperature).

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

287 31 ps and a long-lived component of several ns.

288 nductively coupled plasma-mass spectrometry (ns-LA-MC-ICP-MS) for Fe isotopic analysis of glassy cosm

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

290 eficiency also contributed to non-syndromic (ns) CL/P.

291 Ten ns after photoexcitation, the crystal structure features

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

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

294 overall, there was a good match between the ns-LA-MC-ICP-MS and solution MC-ICP-MS results.

295 uctures, experimentally a sudden drop in the ns values is observed for samples with very thin channel

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

297 34 and RV myocardial QRS in 14 of 34 of the ns-HB cases.

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

299 e short-lived conformational states over the ns-ms timescale.

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