ライフサイエンスコーパス: be in good agreement with

1 The observed difference in reactivity is in good agreement with a computational model system w

2 Our simulation is in good agreement with a new sediment record (ANDRILL

3 The predicted kinetic behavior is in good agreement with a range of experimental findin

4 d from small-angle X-ray scattering data and was in good agreement with a model consisting of one Rho

5 ited satisfactory accuracy and precision and was in good agreement with a standard spectrophotometric

6 a-like disease on the weighted contact graph are in good agreement with absentee data during the most

7 The obtained results are in good agreement with activity data determined from

8 The model results are in good agreement with an experimental study in whic

9 n to the TAT liposome SHG data, was shown to be in good agreement with an approximated solution.

10 ing this device with spectroscopic detection are in good agreement with analysis done with a standard

11 the amplifier in terms of gain and bandwidth are in good agreement with analytical predictions.

12 A length and nucleocapsid internal structure are in good agreement with available experiments for the

13 few weeks to several months, and predictions are in good agreement with available field data.

14 Our results are in good agreement with available simulations and exp

15 for SCLs of varying oxygen transmissibility is in good agreement with available theory.

16 The final converged structures are found to be in good agreement with both experimental data and pre

17 sks, and the wavelengths of these resonances are in good agreement with calculations carried out in t

18 The results were in good agreement with certified sulphur concentrat

19 n on the lateral Ga doping dimensions, which are in good agreement with conductive AFM images.

20 c field drops across the selectivity filter, are in good agreement with continuum electrostatic calcu

21 cardial perfusion imaging scans was found to be in good agreement with core lab standards, suggesting

22 y the metal-ligand NBOs and that these rates are in good agreement with corresponding rates measured

23 e overall structure of the C-terminal domain is in good agreement with crystallographic models derive

24 herical equivalent (P < 0.0001 for both) but was in good agreement with cycloplegic retinoscopy for c

25 A2 obtained values were found to be in good agreement with data previously reported in li

26 n positively and negatively charged surfaces were in good agreement with Derjaguin-Landau-Verwey-Over

27 It is shown that these descriptors are in good agreement with DFT calculations, allowing de

28 metric information for the two proteins that is in good agreement with dynamic light scattering measu

29 direct optical transition at 0.74 eV, which is in good agreement with electrical transport measureme

30 Furthermore, the experimental spectra are in good agreement with electronic structure calculat

31 1-relaxation rates after ESMA administration were in good agreement with ex vivo histomorphometry (El

32 obability distributions that are measured to be in good agreement with exact quantum calculations up

33 These results are in good agreement with existing experimental data.

34 ermeability coefficients of H2S and H2O that are in good agreement with experiment.

35 Predicted diffusivities are in good agreement with experiment.

36 otential iron-sulfur protein is predicted to be in good agreement with experiment using density funct

37 The predicted profiles are in good agreement with experimental binding data; fu

38 growth mechanisms and crystallization speed are in good agreement with experimental data.

39 one by DFT shows that the HOMO-LUMO bandgaps are in good agreement with experimental data.

40 The predicted relative stabilities are in good agreement with experimental data.

41 mical shifts obtained from the aiMD averages are in good agreement with experimental data.

42 ion with a series of sulfonamide derivatives are in good agreement with experimental data.

43 l studies of the mechanism of HCP generation are in good agreement with experimental data.

44 Transition states derived from this model are in good agreement with experimental findings and ena

45 The simulation results are in good agreement with experimental high-resolution

46 th the DFT results and empirical predictions are in good agreement with experimental observations in

47 he computational analysis and MD simulations are in good agreement with experimental results, validat

48 d by quantum mechanical DFT calculations and are in good agreement with experimental results.

49 of metric parameters and activation enthalpy are in good agreement with experimental values [DeltaH(d

50 se along ssDNA in the 3'-5' direction, which is in good agreement with experimental data and the inch

51 We then demonstrate that it is in good agreement with experimental data for shape, s

52 formula, with (In kappa)(-)(1) = .32 +/- .01 is in good agreement with experimental data.

53 intermediate in both simulation systems, and was in good agreement with experimental data available f

54 Predicted QSPR results were in good agreement with experimental amino acid prof

55 Model simulations were in good agreement with experimental results for bot

56 All computational results were in good agreement with experimental results.

57 ted dynamic properties of the three proteins are in good agreement with experimentally determined B f

58 edicted theoretical drift time values, which were in good agreement with experimentally measured valu

59 As an example, we report values that are in good agreement with experiments and that concern

60 Simulations are in good agreement with experiments for a series of s

61 Predictions are in good agreement with experiments on both thermal a

62 Predictions are in good agreement with experiments on ribosomal conc

63 The model predictions are in good agreement with experiments on the growth rat

64 The results of the FEP/MD calculations are in good agreement with experiments, enabling a detai

65 The results of the free energy simulations are in good agreement with experiments, thereby enabling

66 d by Dismukes et al., the calculated results are in good agreement with experiments.

67 The computational results are in good agreement with experiments.

68 rls and helices, and whose length and number are in good agreement with experiments.

69 DNA with limited secondary structure, which is in good agreement with experiments.

70 olding and the structure of the native state were in good agreement with experiments.

71 ciency as a fitting parameter, model results were in good agreement with field observations when spat

72 normal, but the final CSF Abeta measurements were in good agreement with florbetapir cortical retenti

73 s of actual clinical samples and the results are in good agreement with fluorescence polarization imm

74 a model with a single diffuse actin species is in good agreement with FRAP experiments.

75 These results are in good agreement with GC/MS concentrations, and an

76 The results of this analysis were in good agreement with GC-MS results and with repor

77 Results are in good agreement with high-quality summertime obser

78 This result is in good agreement with HPLC analysis that indicated 9

79 observations in this vortex-free superfluid are in good agreement with hydrodynamic predictions, dem

80 eactions: the MALDI-TOF-MS profiles obtained were in good agreement with hydrophilic liquid interacti

81 Model simulations are in good agreement with in vitro data on the signal t

82 and division zones), our simulation results being in good agreement with independent experimental ob

83 The data were in good agreement with independent measurements obt

84 calculations provide structural results that are in good agreement with infrared and X-ray absorption

85 Results of CE fraction were in good agreement with INR (R(2) = 0.73; p < 0.001)

86 The results are in good agreement with known experimental structures

87 Lipid-based concentrations derived from EPS were in good agreement with lipid-normalized concentrati

88 the D measurements achieved in our platform are in good agreement with literature values measured us

89 and biocide compounds in water, and the data were in good agreement with literature data.

90 timate their statistical significance, which is in good agreement with manual classifications by huma

91 Model predictions were found to be in good agreement with measured values, demonstrating

92 The RASREC Rosetta models were in good agreement with models obtained using tradit

93 c inter- and intramolecular interactions and were in good agreement with MS measurements.

94 b initio and reverse Monte Carlo simulations are in good agreement with neutron and X-ray diffraction

95 also measured experimentally and the results are in good agreement with numerical simulations.

96 The experimental measurements are in good agreement with numerical simulations.

97 Overall, our simulation results are in good agreement with observations from biological

98 e three distinct phases, and its predictions are in good agreement with observations.

99 e model was well-calibrated; predicted risks were in good agreement with observed risks.

100 dicted in male and female bottlenose dolphin were in good agreement with observed tissue concentratio

101 annels, achieving high stretching (90%) that is in good agreement with Odijk deflection theory, and w

102 lationship predicts processivity values that are in good agreement with our estimates from published

103 Quantum-optical simulations are in good agreement with our experiments and provide i

104 This model is found to be in good agreement with our results and indicates a gr

105 ectron vertical detachment energy of 2.30 eV is in good agreement with our computational prediction.

106 flow as proportional, variant Pe(3/4), which is in good agreement with our experimental results.

107 ylindrical symmetry (asymmetric) shape which is in good agreement with our molecular dynamics simulat

108 The experimental data are in good agreement with particle tracing simulations

109 onsumption by the HS under anoxic conditions were in good agreement with past electrochemical measure

110 chroism of our switchable plasmonic material is in good agreement with predictions based on dipole ap

111 s (r) dependence of approximately 1/r, which is in good agreement with predictions for a nanotube Mot

112 kling instability followed by folding, which is in good agreement with predictions from classical ela

113 Our data are in good agreement with previous measurements of MutS

114 ls formed by the yeast prion protein Sup35NM are in good agreement with previous results from scannin

115 These predictions were found to be in good agreement with previous in vitro and in vivo

116 to the corresponding endo cycloadduct, which is in good agreement with previous experimental observat

117 the hyperphosphorylated form of NS5A, which is in good agreement with previous observations that hyp

118 value is based upon lipid derived energy and is in good agreement with previous weight prediction for

119 iability as a function of fitted-sensitivity was in good agreement with previous estimates.

120 s approach at pH 7.4 and 37 degrees C, which was in good agreement with previous values determined by

121 The resulting pathways are in good agreement with previously reported results f

122 desorption of enolate and H as acetaldehyde are in good agreement with previously reported TPD resul

123 This model is in good agreement with previously reported Vif and A3

124 The pattern of MeHg yields was in good agreement with previously determined methyla

125 from continuous fluorescent assays with MTA were in good agreement with previously measured literatu

126 These are shown to be in good agreement with product specification sheets.

127 The procapsid structural model is in good agreement with published biochemical data ind

128 The e-nose analysis results are in good agreement with pyruvic acid analysis.

129 son ranking provided a severity ranking that was in good agreement with ranking obtained by classific

130 Our results are in good agreement with recent experiments, and highl

131 iate derived from the time-resolved IR study are in good agreement with recent predictions by DFT ele

132 All observed phenomena are in good agreement with recent quantum-based models o

133 estimated as omega approximately 0.21, which is in good agreement with recent independent estimates.

134 the Ca(2+)-CaM state obtained in this study is in good agreement with residual dipolar coupling, par

135 sed alpha-helical site, at residue 28; these are in good agreement with rotamers previously reported

136 rected using measures of the losses of PRCs, were in good agreement with separately measured equilibr

137 The positive delta(66)ZnIRMM signatures are in good agreement with signatures characteristic for

138 While the global folding mechanism is in good agreement with simulation predictions, we obs

139 side both [2]catenanes, an observation which is in good agreement with spin-density calculations usin

140 ic rate constants determined from these data are in good agreement with steady state data confirming

141 rized with our sensing platform and found to be in good agreement with that of previous studies.

142 [DeltaH(double dagger) = 11.5 kcal.mol(-1)] is in good agreement with that measured experimentally.

143 n (129)I/(131)I atomic ratio of 16.0 +/- 2.2 is in good agreement with that measured from rainwater a

144 mber of latrine events measured by the PLUMs was in good agreement with that measured by trained obse

145 the level of antibody binding to fusion tags was in good agreement with that measured in solution usi

146 of metabolites from the ME-EP-JRESI sequence were in good agreement with that of the EP-JRESI sequenc

147 ).M(delta-)] superalkali-alkali mixed dimers are in good agreement with the aforementioned experiment

148 Gene trees based on each of these regions are in good agreement with the Aliatypus species tree, w

149 The numerical findings are in good agreement with the analytical results and qu

150 temperatures from the specific heat profiles are in good agreement with the available experimental da

151 These are in good agreement with the biological understanding

152 pecifically, the voltammetric peak positions are in good agreement with the calculated energies for C

153 ring synthesis of phage-related proteins and are in good agreement with the calculated potential cont

154 s (deprotonation DeltaG, DeltaH, and DeltaS) are in good agreement with the calculated values for the

155 These experimental energy differences are in good agreement with the calculated values of 9.7

156 The experimentally obtained data are in good agreement with the calculated values.

157 erimentally determined activation parameters are in good agreement with the calculated values.

158 The ATR-FTIR results of extracted oils/fat are in good agreement with the capillary gas chromatogra

159 the certified reference material (INCT-TL-1) are in good agreement with the certified value.

160 The results obtained from the soil analysis are in good agreement with the certified values, demonst

161 d temporal nature of self-folding structures are in good agreement with the companion finite element

162 The resulting VSD structures are in good agreement with the consensus model of the re

163 The corresponding structures obtained are in good agreement with the crystal structure of rubr

164 ions are made independently at each site and are in good agreement with the data.

165 d using potential of mean force calculations are in good agreement with the differences in rates obta

166 h some exceptions, modeled PAS uptake curves are in good agreement with the empirical PAS data.

167 The results are in good agreement with the expected values, demonstr

168 te the separation procedure, and the results are in good agreement with the expected values.

169 The predicted rates and transition states are in good agreement with the experimental data for a b

170 alance equations, and the simulation results are in good agreement with the experimental data.

171 We find that theoretically predicted spectra are in good agreement with the experimental line shapes

172 e calculated conductance and ion selectivity are in good agreement with the experimental measurements

173 d vertical and adiabatic detachment energies are in good agreement with the experimental measurements

174 We produced ensembles that are in good agreement with the experimental NMR chemical

175 ansitions of the superoxo and peroxo species are in good agreement with the experimental observation.

176 The computational models are in good agreement with the experimental observations

177 XRD) spectra of a few polymorphic structures are in good agreement with the experimental spectrum, su

178 for known carbohydrate ligands of galectin-3 are in good agreement with the Kd values reported and me

179 s across residues M(1)-L(15) and N(25)-R(42) are in good agreement with the known secondary structura

180 The model's predictions are in good agreement with the known spatial distributio

181 These results are in good agreement with the near-ubiquitous seropreva

182 rates analytically and demonstrate that they are in good agreement with the numerical results.

183 aviours on the square-post patterned surface are in good agreement with the predicted values by the t

184 These values obtained for betac are in good agreement with the predictions of a three-di

185 The experimental results are in good agreement with the present model.

186 Our results are in good agreement with the previous steady-state and

187 These findings are in good agreement with the results of our recent opt

188 holds predicted by the continuum description are in good agreement with the results of stability calc

189 The nucleophilicity values are in good agreement with the sigma basicities of all o

190 gnificant (19)F-(19)F J couplings, and these are in good agreement with the splittings observed in a

191 ements of the band gap of the Ti(17) cluster are in good agreement with the theoretical values and sh

192 ental barriers as a function of M and olefin are in good agreement with the trends in the calculated

193 imley-White interfacial hydrophobicity scale are in good agreement with the values derived from exper

194 Our results are in good agreement with the well-studied hydride tran

195 ic resonance (EPR) measurements are found to be in good agreement with the available crystal structur

196 The experimental assay results were found to be in good agreement with the computed data, confirming

197 ta(DeltaDeltaE(double dagger))) was found to be in good agreement with the experimentally observed se

198 ha and Mbeta X-ray intensities were found to be in good agreement with the measurements, allowing the

199 hree sequences for IPH detection appeared to be in good agreement with the quantitative contrast of I

200 es showed nonsignificant trends that seem to be in good agreement with the results of the National Lu

201 These equations are shown to be in good agreement with the simulations and enabled ev

202 ic model for TLS folding is developed, which is in good agreement with the [M(n+)]-dependent evolutio

203 The classification by chemometric methods is in good agreement with the classification by the mice

204 sured transition time of about a millisecond is in good agreement with the computed time.

205 This is in good agreement with the core-accretion theory of p

206 ents between the strained and relaxed layers is in good agreement with the differences in the piezoel

207 This finding is in good agreement with the expected influence of a la

208 The simulated molecular transport is in good agreement with the experimental data, indicat

209 This model is in good agreement with the experimental data.

210 The model is in good agreement with the experimental data; however

211 This is in good agreement with the experimental Ea for N2O ac

212 eating of populations and quantum coherences is in good agreement with the experimental results and t

213 The predicted sense of stereoselectivities is in good agreement with the experimental results.

214 es with alpha-substitution show a trend that is in good agreement with the experimental results.

215 This is in good agreement with the experimental value (koff =

216 oropropene molecules of 36.9 kcal/mol, which is in good agreement with the experimentally determined

217 in polymers are treated as entropic springs, is in good agreement with the experimentally measured sh

218 tical pressure PC approximately 8 GPa, which is in good agreement with the experiments.

219 C) for the Fe4-bound Cys20 backbone nitrogen is in good agreement with the large 13.0/14.6 MHz (14)N

220 namics and find that the resulting structure is in good agreement with the mutagenesis results.

221 The obtained structure is in good agreement with the NMR coordinates 1O8R.

222 - 0.1 for the G.C Hoogsteen base pair, which is in good agreement with the pKa value (7.1 +/- 0.1) ca

223 al conditions was found to be 30.049%, which is in good agreement with the predicted value of 30.054%

224 -life is 244900 +/- 670 years (k = 1), which is in good agreement with the previously reported result

225 he amount of total titanium found, 48.7 ppb, is in good agreement with the result of the reference me

226 The experimental map is in good agreement with the results of a theoretical m

227 g step, and the obtained free energy barrier is in good agreement with the value derived from the exp

228 al/mol at the B3LYP/6-31 G(d,p) level, which is in good agreement with the value of 7.6 kcal/mol and

229 s, the volume of irreversibly damaged tissue was in good agreement with the 6-month late gadolinium e

230 om the USC-CO2 dynamic extraction curves and was in good agreement with the calculated values for the

231 A mathematical model was proposed and was in good agreement with the experimental results.

232 formance of exhaled nitric oxide measurement was in good agreement with the gold standard chemilumine

233 ined by correcting Kd(ND) by the factor fND, was in good agreement with the half maximal inhibitory c

234 spacing of 14 nm as measured by SAXS, which was in good agreement with the lamellar thickness measur

235 This result was in good agreement with the simulated near field prof

236 trend found on the polycrystalline surfaces was in good agreement with the trend in the discharge vo

237 The satellite results were in good agreement with the annual official NOx emis

238 external calibration with aqueous standards were in good agreement with the certified values.

239 reference sample (bush branches and leaves) were in good agreement with the certified values.

240 The aggregation kinetics data were in good agreement with the classic Derjaguin-Landau

241 for a reversible protein-protein interaction were in good agreement with the data obtained by other s

242 y surface plasmon resonance, and the results were in good agreement with the determined enzymatic act

243 estimates of analyte diffusion coefficients were in good agreement with the expected values.

244 spersion processes, and the modeling results were in good agreement with the field observations.

245 ique was performed, and the resulting values were in good agreement with the former method.

246 tion that absorption is the dominant process were in good agreement with the measurements for PAHs, O

247 The TIFA gene essentiality calls were in good agreement with the MR-1 FBA essentiality pr

248 e de novo construction of genetic maps which were in good agreement with the NCCCWA genetic map.

249 PET/CT scans with 70%-90% SUVmax thresholds were in good agreement with the recurrent volume at a 40

250 Both the qPCR and ddPCR assays were in good agreement with the reference assay.

251 hydrochloric and methanesulfonic acid salts were in good agreement with the results observed in solu

252 The model calculations for SA and QED were in good agreement with the simulation results, whic

253 and sugar cane bagasse), and lignin contents were in good agreement with the total gravimetrically de

254 rmal conductivity of AlN@PI/epoxy composites were in good agreement with the values calculated from t

255 The results were in good agreement with the values from ELISA.

256 The measured values with the Bi-FE were in good agreement with the values obtained using th

257 de concentrations ranging from 0.005 to 2 mM were in good agreement with the values predicted by the

258 iphatic side chains (Ala, Val, Ile, and Leu) are in good agreement with their DeltaG(tr) values from

259 red concentrations of proteins in a solution were in good agreement with their volumetrically prepare

260 tructure on the nature of the nucleobase and are in good agreement with theoretical calculations perf

261 ng linear sweep voltammetry, and the results are in good agreement with theoretical predictions for e

262 entally observed in the gigahertz range, and is in good agreement with theoretical analysis and full-

263 This observation is in good agreement with theoretical expectations but c

264 gs concerning reactivities and selectivities were in good agreement with theoretical investigations u

265 nse observed for the Fe(CN)(6)(3-/4-) couple were in good agreement with theoretical predictions for

266 ion data to compute line tension values that are in good agreement with theory and the analysis from

267 ra of Ga(0.97)Mn(0.03)As and GaAs, and these are in good agreement with theory.

268 bserving its time dependence and is found to be in good agreement with theory.

269 The observed structures were found to be in good agreement with thermodynamic growth trends pr

270 ine calcium carbonate saturation states that are in good agreement with those determined by more labo

271 ated activation parameters for this reaction are in good agreement with those determined experimental

272 btained for %HbA1c in human blood hemolysate are in good agreement with those determined using a refe

273 give rise to cluster size distributions that are in good agreement with those found in experiments.

274 hymotrypsin, the kinetic parameters obtained are in good agreement with those in the literature.

275 d with a passive atmospheric sampling system are in good agreement with those measured with an active

276 meters extracted from snapshot voltammograms are in good agreement with those obtained by conventiona

277 he gas-phase electron diffraction parameters are in good agreement with those obtained from theory at

278 ng parameters computed from DFT calculations are in good agreement with those of experimental values.

279 ition time distribution of multiple pathways are in good agreement with those of long Langevin dynami

280 ined for the synthesized supramacromolecules are in good agreement with those predicted by molecular

281 ha6/alpha3 chimeras in oocytes were found to be in good agreement with those from previous studies of

282 The results were found to be in good agreement with those obtained by HPLC method.

283 strated in human serum samples, with results being in good agreement with those determined using a st

284 of transport and ligand binding: koff values were in good agreement with those derived from uptake ex

285 The results obtained by FlavonQ were in good agreement with those determined conventiona

286 acid in blood serum samples and the results were in good agreement with those from the current perio

287 All reported values were in good agreement with those in the literature.

288 metal ions obtained by the proposed methods were in good agreement with those obtained by FAAS.

289 The collected data were in good agreement with those obtained by reference

290 The MIC results measured by dAST were in good agreement with those of BDT (essential agre

291 measured velocities showed that mean values were in good agreement with those predicted using contin

292 tate (alpha-helical) basin equals 22%, which is in good agreement with time-resolved experiments and

293 ents that accurately detected severe AVS and were in good agreement with TTE.

294 Results of mu for two particle standards are in good agreement with values determined by phase an

295 The results are in good agreement with values obtained by X-ray refl

296 jectories according to the DNA length, which were in good agreement with values predicted from electr

297 e between the ribosomal components, and they are in good agreement with various experimental data.

298 The mesoscopic view presented here is in good agreement with various mechanistic proposals

299 Our results are in good agreement with very recently reported experi

300 We show that measured EE(2) metabolites are in good agreement with what is expected based on FED