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

1 The results are in good agreement with a theory accounting for the c

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

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

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

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

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

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

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

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

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

11 The k(tau) ratio values were in good agreement with bias estimates from existing

12 The results were in good agreement with certified sulphur concentrat

13 ST 1568a rice flour was analyzed and results were in good agreement with certified values.

14 UISS-TB shows to be in good agreement with clinical trial results suggest

15 The computational model was in good agreement with clinical findings: the overal

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

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

18 The outcomes are in good agreement with current cryo-electron microsc

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

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

21 In vitro data were in good agreement with data from a 96 h in vivo exp

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

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

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

25 en softening of the bulk modulus is shown to be in good agreement with elastic moduli measurements pe

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

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

28 1-relaxation rates after ESMA administration were in good agreement with ex vivo histomorphometry (El

29 ements for the elastin- and iron oxide-probe were in good agreement with ex vivo histopathology (Prus

30 rements for the elastin and iron-oxide-probe were in good agreement with ex-vivo histopathology (Elas

31 zeta-Values were in good agreement with exclusive outside localizati

32 vibrational state-resolved rate coefficients are in good agreement with existing experimental results

33 Predicted diffusivities are in good agreement with experiment.

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

35 results for surface and core melting points are in good agreement with experiment.

36 onated (356 nm) and neutral species (440 nm) are in good agreement with experiment.

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

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

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

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

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

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

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

44 These results are in good agreement with experimental observations and

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

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

47 ry (DFT) and time-dependent DFT calculations are in good agreement with experimental spectra, spectra

48 e-art free energy protocol and were found to be in good agreement with experimental data, thus corrob

49 ried out and the obtained data were found to be in good agreement with experimental findings.

50 time-dependent coupled-mode theory, found to be in good agreement with experimental results, is utili

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

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

53 Our model is in good agreement with experimental results and a use

54 The predicted level of enantioselectivity is in good agreement with experimental values.

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

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

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

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

59 For all conditions, simulated results were in good agreement with experimental results.

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

61 Our simulations are in good agreement with experimentally determined par

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

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

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

65 Predictions are in good agreement with experiments on ribosomal conc

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

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

68 as the consensus UUCG tetraloop structures, are in good agreement with experiments, there are remain

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

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

71 esolution three-dimensional simulations that are in good agreement with experiments.

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

73 The computational results are in good agreement with experiments.

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

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

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

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

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

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

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

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

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

83 The results from the IQ-DCNN were in good agreement with human expert reading, and th

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

85 atio (CNR) measurements of the elastin probe were in good agreement with ICP-MS (y = 0.11x-11.3, R2 =

86 o, collision cross sections of MD structures were in good agreement with IMS data.

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

88 The data were in good agreement with independent measurements obt

89 rements for the iron oxide and elastin-probe were in good agreement with inductively coupled mass spe

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

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

92 The results are in good agreement with known experimental structures

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

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

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

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

97 from the optical measurements were shown to be in good agreement with measurements obtained from loa

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

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

100 simulation of theoretical pore density which are in good agreement with numerical simulation.

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

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

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

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

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

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

107 Calculated S values were in good agreement with OLINDA/EXM 2.0 (commercial)

108 ulations of surfactant delivery in rat lungs are in good agreement with our experimental data.

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

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

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

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

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

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

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

116 ngly, the practical CO(2) adsorption amounts are in good agreement with predicted values using surfac

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

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

119 ion thermodynamics obtained with this method are in good agreement with previous results from tempera

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

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

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

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

124 in one of the examples, the obtained results are in good agreement with previously reported biologica

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

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

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

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

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

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

131 at the DNN model generates ESP surfaces that are in good agreement with QM and that the ESP values co

132 These were in good agreement with quantitative polymerase chai

133 Our computed barriers are in good agreement with racemization barriers estimat

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

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

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

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

138 agonist/GHS-R1a in the absence of G proteins are in good agreement with recently reported data.

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

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

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

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

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

144 -fold enhancement of SHG nonlinearity, which is in good agreement with simulations and calculations.

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

146 hydrocarbons in diesel fuel by this approach is in good agreement with state-of-the-art techniques re

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

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

149 We show that the reconstructed spectrum is in good agreement with that measured directly by a Fo

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

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

152 system, and the obtained heat of desorption was in good agreement with that calculated from the conv

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

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

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

156 These are in good agreement with the biological understanding

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

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

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

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

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

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

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

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

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

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

167 in the fibers and the theoretical estimates are in good agreement with the data.

168 electrochemistry and UV-visible transitions are in good agreement with the DFT and time-dependent DF

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

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

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

172 power dissipation due to the dielectric loss are in good agreement with the experiment data.

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

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

175 The trends obtained using simulations are in good agreement with the experimental measurements

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

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

178 The computed cis/trans ratios are in good agreement with the experimental ones and thu

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

180 rtate obtained using this intermediate state are in good agreement with the experimental values.

181 The calculated cross sections are in good agreement with the experimentally reported v

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

183 Our observations are in good agreement with the known effects of choleste

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

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

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

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

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

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

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

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

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

193 tants with impaired or altered LPS synthesis are in good agreement with the results of simpler tests

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

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

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

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

198 ity distribution was determined and found to be in good agreement with the best established experimen

199 material (INCT-TL-1 tea sample) was found to be in good agreement with the certified value.

200 and Whatman filter paper strips was found to be in good agreement with the color change of P2 in solu

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

202 The simulated spectra proved to be in good agreement with the experiment.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

224 - 0.1 for the G.C Hoogsteen base pair, which is in good agreement with the pKa value (7.1 +/- 0.1) ca

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

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

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

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

229 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

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

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

232 sted by the analysis of SRM 1566b and DORM-4 was in good agreement with the certified values.

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

234 specific charge generated by corona charging was in good agreement with the experimental results.

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

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

237 The deterministic simulation was in good agreement with the Monte Carlo simulation on

238 The performance of the PoD was in good agreement with the results obtained using a

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

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

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

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

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

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

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

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

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

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

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

250 DC values based on the denoised hb DW images were in good agreement with the reference ADC values (me

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

252 The obtained results were in good agreement with the results from the HPLC-UV

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

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

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

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

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

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

259 nt ranging from -1.5 to 4, where our results were in good agreement with the values reported in the l

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

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

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

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

264 s the protein by 6 kJ mol(-1) , a value that is in good agreement with theoretical estimates of the e

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

266 The measured Hall voltage noise is in good agreement with theoretical models and we demo

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

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

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

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

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

272 SUMO1-Ubc9 interaction based on this method are in good agreement with those determined by other tec

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

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

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

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

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

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

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

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

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

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

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

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

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

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

287 d at a concentration level of 7-10 mug L(-1) were in good agreement with those obtained using the con

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

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

290 ed from the immunochromatographic strip test were in good agreement with those realized from enzyme-l

291 Reducing sugar values determined were in good agreement with those recorded using a comme

292 globin in reduction and oxidation NPSV modes were in good agreement with those reported earlier by in

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

294 opologues (18)O(16)O and nitrogen (15)N(14)N were in good agreement with typical values.

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

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

297 e linking number per stacked nucleosome that were in good agreement with values measured here experim

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

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

300 ectrode surface, where the experimental data are in good agreement with well-established chronopotent