ライフサイエンスコーパス: agree well with

1 patients, both global LS and global CS 2DST agreed well with 2DTagg (ICC, 0.89 and ICC, 0.80; P<0.00

2 gan distribution volume ratio (DVR)-1 values agreed well with 2TCM DVR-1 values (R(2)= 0.99, slope =

3 (68)Ga-GFR agreed well with (51)Cr-GFR for estimation of GFR using

4 sufficient to produce myocardial images that agree well with 8.0-million-count images on quantitative

5 Quantitative measurements agree well with a kinetic model, providing a unified pic

6 mouse chromosome 1, finding that the results agree well with a prior genetic characterization of 3026

7 Moreover, the relative mobilities of the DNA agree well with a recent estimate for the Ogston sieving

8 Our IWF structure agrees well with a recently solved cryo-EM structure of

9 Because this agrees well with a value of 3.93 S in 137 mM NaCl, the o

10 intrinsic laser parameters, and our analysis agrees well with a wide range of parameters found in pub

11 d predicted probability of favorable outcome agreed well with all patients taken together.

12 Our simulation results agree well with approximations gained from the theory of

13 The simulations agree well with available biophysical data, suggesting t

14 and a higher compressibility modulus, which agrees well with available experiments.

15 play similar mechanical properties that also agree well with bending tests.

16 xperimental results revealed that our models agree well with both Bax and Bak pores, pointed to a con

17 fective mode for gating), the MDeFEM results agree well with both experiments and all-atom simulation

18 The MD simulations agree well with both the neutron scattering, which furni

19 rical results for computed action potentials agree well with cable model predictions for large cluste

20 r) heterodimer of 84.9 +/- 2.5 A(2) at 302 K agrees well with calculated angle-averaged cross section

21 ts of both a single ring and arrays of rings agree well with calculations based on a model of non-int

22 Our observations agree well with calculations of the strong-field ionizat

23 Results from patch-clamp recordings agreed well with cellular assays of p7 activity, namely,

24 tterns of deposition predicted by simulation agreed well with clinical observations.

25 fractionation-derived degradation estimates agreed well with concentration mass balances, providing

26 tively assessed, yielding an EC50 value that agrees well with conventional biochemical readout.

27 Results on real data agree well with current knowledge.

28 These observations agree well with current theories that relate the time ef

29 of the bulk serotonin release were found to agree well with data obtained from single platelet measu

30 -1), and K(4) = (1.6 +/- 0.6) x 10(6) M(-1), agree well with determinations by other methods and serv

31 In all cases, the extracted values agree well with direct observations or atomistic simulat

32 Both approaches agree well with each other and show that the adhering ve

33 At low temperatures, the two approaches agree well with each other, but at high temperatures, SS

34 lations with different microphysical schemes agreed well with each other and showed better agreement

35 components fit a self-consistent model that agree well with electron microscopy images of the C-ring

36 e PKC-DRS2 associated with long-standing DME agrees well with estimates from the ETDRS.

37 tures observed for the 2F5 and 4E10 epitopes agree well with existing structural data, and enzyme-lin

38 The B-factors for most heavy atoms agree well with experiment (Pearson correlation of 0.90)

39 The ONIOM calculated spectra agree well with experiment but indicate a very different

40 Calculations agree well with experiment with slight deviations for sa

41 Both responses are shown to agree well with experiment.

42 APW method confirm the direct-gap nature and agree well with experiment.

43 of the trajectory, and the structure factors agree well with experiment.

44 mputed from the relative O-state populations agree well with experiment.

45 on state ensembles were identified, and they agreed well with experiment on the basis of a comparison

46 ation of the lowest-energy transition moment agrees well with experiment.

47 Computed average values of Rise and Twist agree well with experimental data for B-form DNA from th

48 tries obtained by computational calculations agree well with experimental data, in particular fluores

49 with pH, and of alpha-amylase with mutation agree well with experimental data.

50 pounds predicted from these six alpha-values agree well with experimental data.

51 calculations of our transition-state model, agree well with experimental findings.

52 established PP-LFER-composition-based model agree well with experimental in vitro partition coeffici

53 The results of finite element modeling agree well with experimental measurements of the efficie

54 from our simulations, helix-helix distances agree well with experimental measurements using double e

55 energy and Young's modulus, and the patterns agree well with experimental observations.

56 d variation in the LSPR measurement response agree well with experimental results and support that th

57 Calculations using a full many-body theory agree well with experimental results and unambiguously d

58 itative estimation of coercive fields, which agree well with experimental results for ceramics and th

59 The calculated results agree well with experimental results, and allow differen

60 1), respectively, for EPO, IL4, hGH, and PRL agree well with experimental results.

61 theory as is the pK(a) shift, and the shifts agree well with experimental trends.

62 The results agree well with experimental values, but the model for t

63 l yielded droplet density distributions that agreed well with experimental observations without any m

64 Overall, the computer simulations agreed well with experimental results.

65 The predicted behavior agrees well with experimental data.

66 g effect of crowding on the folding kinetics agrees well with experimental observations.

67 A variation with different capping materials agrees well with experimental results.

68 The rate constants found using this method agreed well with experimentally and theoretically obtain

69 Results agree well with experiments on the nucleotide bias of Ge

70 The resulting (un)folding rates agree well with experiments.

71 The estimation of GPP from this model agreed well with flux tower observations of GPP (R(2 ) =

72 ecord based on subduction-zone length, which agrees well with geological records supporting the valid

73 R across spatial temperature gradients that agree well with global variation-across-space.

74 ons by o-DGT at a wastewater treatment plant agreed well with grab samples and appeared to be less in

75 of 198 +/- 57 and 229 +/- 58 pg m(-3) which agree well with in-flight observed RM and with model bas

76 ) based on a nation's gross domestic product agree well with independent estimates of MGEN for indivi

77 regions is thus 1.48 +/- 0.26 mm (-1), which agrees well with independent estimates of sea level rise

78 The experimental results reported here agree well with ion-size-corrected non-linear Poisson-Bo

79 es C. k(red) for the reductive half-reaction agrees well with k(cat) and exhibits a similar pH optimu

80 These results agree well with kinetic data for pol X and provide a str

81 ations obtained for the other compounds also agreed well with laboratory results.

82 The data agree well with light-scattering measurements, full-fiel

83 These values agree well with literature values determined by accepted

84 The derived HONO and HNO3 EFs agree well with literature values, with HONO being the s

85 ith H(2) or O(2) gave metal dispersions that agree well with mean cluster sizes measured from electro

86 pp-LFER predicted KS agreed well with measured KS reported in the literature.

87 matter, leaf area index and grain yields all agreed well with measured values.

88 The model agrees well with measured values of swimming speeds duri

89 enerated pH, computed from first principles, agrees well with measured values.

90 r observations in detergent in solution, but agree well with measurements by electrophysiology and ap

91 ons were lower than measured in benthos, but agreed well with measurements in fish.

92 The simulations agreed well with measurements of the cochlear partition

93 The self-paced results agree well with meta-analyses and other published result

94 DNMT1 expression levels agreed well with methylation levels at imprinted genes.

95 .82-1.18) over the 4 day deployment and also agreed well with Metsorb-DGT (CMBL/CMetsorb = 0.84-0.94)

96 Experimental results agree well with model predictions, thereby illustrating

97 The measurements of PCDD/Fs in air agree well with model-predicted concentrations performed

98 rate, separation factors and Raman spectrum agree well with models based on effusion through a small

99 Our results agree well with Monte Carlo simulations in two dimension

100 nts predicted by Bell's formula, kappaBell , agree well with multidimensional tunneling (canonical va

101 The measurement agrees well with multiscale and first-principles-based s

102 /regression model introduced in this article agrees well with murine models.

103 The theoretical prediction agrees well with numerics.

104 ospheric reservoir of 4.57 Gg, both of which agree well with observational constraints.

105 Expected events agreed well with observed events for each model, indicat

106 ntrations for both UV-B and UV-C experiments agreed well with our model (R(2) = 0.88-0.99), except un

107 Neither model agrees well with our in vivo data, suggesting that, in a

108 km/s velocity derived from these satellites agree well with parameters inferred from the wealth of s

109 Our model predictions agreed well with pH data from hypoxic zones in the north

110 al results for the bacterial flow statistics agree well with predictions from a minimal model for sel

111 partition coefficient and equilibration time agree well with predictions from the literature.

112 The D5 measurements agreed well with predictions from a Eulerian atmospheric

113 ith stereotypic concentration waveforms that agreed well with predictions of a mathematical model of

114 rations in the device and the tuning results agree well with previous measurements.

115 In general, the results obtained agree well with previous observations made using amplico

116 at the patterns extracted using SSA and MSSA agree well with previous patterns identified using wavel

117 ntified meaningful biological processes that agreed well with previous reports on T1D.

118 for the well-studied case of pure CO2-water agreed well with previous theoretical and experimental d

119 te of interaction between CheW and Tm14 that agrees well with previous biochemical and genetic data f

120 y delineates CA3/CA2 and CA2/CA1 borders and agrees well with previous cytoarchitectural definitions

121 al assignments from sequence analysis, which agrees well with previous feeding experiments, and has b

122 genetic changes within the "living biobank" agrees well with previous large-scale mutational analyse

123 We show that our method agrees well with previous methods based on measurement o

124 This agrees well with previous molecular dynamic simulations

125 become larger (26.9 +/- 6.7 degrees ), which agrees well with previous molecular dynamics simulation

126 ations of p53/p21 dynamics after irradiation agree well with previously published experimental studie

127 ulas for the PSD of this coupled system that agree well with PSDs obtained in experiments and simulat

128 0.4 mV for Plasmodium falciparum Trx, which agree well with published values (-283 or -285 mV and -2

129 n of abortive pits calculated from our model agrees well with published experimental data.

130 ical calculations via a thermochemical cycle agree well with reaction free energies from experiments,

131 RLB agreed well with REB (80%-86% agreement; kappa = 0.55-0.

132 Our predictions agree well with recent epigenomic data in human and mous

133 Overall, these results agree well with recent results of sequencing of a single

134 n as a minimal machinery for vesicle budding agrees well with recent findings that alpha-synuclein pl

135 The resulting consensus tree agrees well with recent higher-level mammalian phylogeni

136 obal multimedia mass-balance model generally agree well with reported field measurements, suggesting

137 ous state model fits to published data (that agreed well with reported error), we used a discrete sta

138 The determined concentrations agree well with results from counting with microscopy (a

139 nsemble absorption polarization measurements agree well with results obtained by single molecule fluo

140 new NMR structure of the Pdx-CYP101 complex agrees well with results from previous mutagenesis and b

141 The MD results agree well with scanning electron microscopy (SEM) and e

142 ary excitation intensities are quite low and agree well with simulated enhancements.

143 of transferrin receptor mRNA in single cells agrees well with single-molecule fluorescence in situ hy

144 on sites inferred from molecular simulations agrees well with site capacities of surface complexation

145 onformational dynamics computed for C26H34O2 agree well with solution NMR data and help in the assign

146 takes, and the concentration measured by DGT agreed well with solution concentrations.

147 a wide range of total RNA concentrations and agrees well with standard curve qPCR.

148 The testing results agree well with that obtained from 96-well plates with m

149 ae or in species of the gamma-Proteobacteria agreed well with that of the corresponding 16S rRNA gene

150 bution in the nanoparticle-ligand conjugates agreed well with that predicted by the Poisson model.

151 stern U.S. (-0.37 +/- 0.13 mug m(-3) yr(-1)) agrees well with that from in situ measurements (-0.38 +

152 usivity predicted by this DFT + KMC approach agrees well with that from previous independent experime

153 nsition voltage via the Newns-Anderson model agrees well with that of the Fermi/HOMO energy level dif

154 d that the timing of ice-volume fluctuations agrees well with that of variations in Antarctic climate

155 oclusters, respectively, which were shown to agree well with the average diameters of the correspondi

156 he obtained band structure and Fermi surface agree well with the band structure calculation of Na2Ti2

157 ce contamination, while the FY and STXM data agree well with the bulk NRIXS analysis.

158 The second-order rate constants for O attack agree well with the calculated rate constants for rate-d

159 ernal friction time scales and found them to agree well with the corresponding experimental measureme

160 These results agree well with the data from other countries.

161 The experimental results agree well with the developed theory.

162 Our molecular data agree well with the differential phenotypic effect on bw

163 In all cases linear fits have slopes which agree well with the dilute limit.

164 in the optimal feature length range, and all agree well with the evolutionary phylogeny based on a re

165 Model simulations that agree well with the experimental data include a pre-equi

166 mulations yield a set of rupture events that agree well with the experimental data.

167 In most cases the free energetic estimates agree well with the experimental observations.

168 calculations, and the corresponding results agree well with the experimental ones.

169 All these facts agree well with the experimental reports for the reactio

170 ur molecules in the low-conductance geometry agree well with the experimental results and show that t

171 relation functions at different temperatures agree well with the experimental results.

172 rature ranges from 10 to 50 degrees C, which agree well with the experimental turnover numbers.

173 parameters calculated from these simulations agree well with the experimental values.

174 ion energies and oscillator strengths, which agree well with the experimental XAS spectra.

175 f the rigid carboxylates for these complexes agree well with the experimentally determined associatio

176 The measurements agree well with the modelings and confirmed that these t

177 than 96% and 67% for the two devices, which agree well with the numerical simulation of the master e

178 The results agree well with the numerical simulation using CST's Mic

179 The data agree well with the numerical simulations which take the

180 g based on elastic network models, and these agree well with the peaks of the statistical distributio

181 rimentally determined [CO2]/[HCO3(-)] ratios agree well with the predicted values for experiments per

182 at half maximum of the line spread functions agree well with the predicted values.

183 Our results agree well with the prediction from gravity theory, incl

184 These values agree well with the prediction from the Wimley-White int

185 on of aperiodic boundaries, their structures agree well with the prediction of the coincident-site-la

186 Quantum chemically computed (13)C shifts agree well with the present NMR measurements.

187 d between the frozen and the nonfrozen state agree well with the proposed ice-binding site.

188 unctional and structural data presented here agree well with the proposed pharmacophore.

189 n product and several reaction intermediates agree well with the relevant crystal structures, validat

190 or the degraded solvent and product mixtures agree well with the results from a total organic carbon

191 Boson peak in our simulations of bulk water agree well with the results from experiments on nanoconf

192 he physical pictures described by simulation agree well with the SFG experimental result.

193 The experimental results agree well with the simulated ones showing an average op

194 Quantum mechanical calculations agree well with the superstructure revealed by X-ray cry

195 tions where the phase transition is observed agree well with the theoretical predictions for these 2D

196 e best fit parameter sets, model simulations agree well with the two different data sets but one mode

197 kcal/mol) and oxidation (21 kcal/mol) steps agree well with the values derived from the kinetics mea

198 eir respective ionophores are calculated and agree well with the values obtained by the potentiometri

199 e diffusion as in buffer, whereas the slower agreed well with the bulk viscosity.

200 , and the degree in their drug effectiveness agreed well with the data in the literature.

201 different diffuse intensities, none of which agreed well with the data.

202 3LYP/6-31++G(d,p) level of theory, and these agreed well with the experimental data.

203 Computer simulations agreed well with the experimental results only when the

204 efficiencies calculated by numerical models agreed well with the experimental results.

205 etermining step, i.e., the homolysis of I2k, agreed well with the experimental value.

206 The increase in FDG6P in nerve terminals agreed well with the increase in cortical neuronal gluco

207 The results agreed well with the landscapes reconstructed by establi

208 the infrared camera based NDVI (camera-NDVI) agreed well with the leaf expansion process that was mea

209 es obtained using this space-domain approach agreed well with the lifetimes from time-domain measurem

210 ition of the Texas Red labeled lipids, which agreed well with the MALDI-MS imaging results.

211 the fraction of observed outcomes generally agreed well with the mean predicted outcome.

212 ly measured corneal biomechanical properties agreed well with the measurements obtained by using esta

213 Our results agreed well with the most recent theoretically calculate

214 Targeted measurements of both metabolites agreed well with the non-targeted measurements, especial

215 The borders and locations of these regions agreed well with the Paxinos mouse brain atlas.

216 scFv7F9Cys and dendribody in blood and urine agreed well with the PCKN data.

217 iability in the frozen state and this metric agreed well with the population-averaged viability and t

218 of the secondary and the tertiary structure agreed well with the predictions from a homology model.

219 y and qualitatively, the model-based results agreed well with the pressure and flow measurements obta

220 Ts to the (1)H-(13)C and (13)C-(15)N vectors agreed well with the results of ab initio calculations,

221 s >3 M, and the FRET-derived Rg of protein L agreed well with the Rg previously measured by equilibri

222 m the second-order annihilation reaction and agreed well with the simulation.

223 ent accessibility expressed by the PF values agreed well with the solvent accessible surface areas ob

224 arameters determined by this DGAT SPA method agreed well with the values determined with the conventi

225 zation-dependent oscillator strengths, which agreed well with the XANES spectroscopy measurements.

226 This agrees well with the calculated tumor control probabilit

227 The KPS method agrees well with the CKD method under all experimental c

228 ch unfolding step in our thermodynamic model agrees well with the corresponding values predicted by t

229 A second, smaller distance of 3.4 A agrees well with the distance between stacked base pairs

230 tion obtained for the system without defects agrees well with the experiment, while the simulated tim

231 The x-ray model agrees well with the experimental and theoretical result

232 P functional, only the 6-311++G** set for Ti agrees well with the experimental charge density distrib

233 th morphine affecting co-receptor expression agrees well with the experimental data from simian immun

234 of the folding rate predicted from the data agrees well with the experimental folding rate (approxim

235 frequency shift analyzed from MD simulations agrees well with the experimental infrared results.

236 s the origin of the interlayer rotations and agrees well with the experimental observations.

237 ment of a minimum jump size k=k(omega) which agrees well with the experimental observations.

238 The calculated E(a) (17.8 kcal/mol) agrees well with the experimental one.

239 was shown that the registry of these models agrees well with the experimental results.

240 The nearly barrierless formation of C4aOOH agrees well with the experimental results; based on tran

241 local density approximation-derived band gap agrees well with the experimentally measured band gap.

242 The proposed mechanism agrees well with the experimentally observed features of

243 tions due to metallic characteristics, which agrees well with the experiments of passively Q-switched

244 or the formation of colloidal molecules that agrees well with the experiments.

245 The measured weak anti-localization effect agrees well with the Hikami-Larkin-Nagaoka model and the

246 al map of the 5-HT3A receptor portals, which agrees well with the homology model.

247 Although the system-level GTP affinity agrees well with the individual affinities of the GTP-de

248 ed critical lattice depth for few-ion chains agrees well with the infinite-chain prediction.

249 tly oxidative local conditions of burial and agrees well with the limited negative cerium anomaly obs

250 ose molecular weight (20,497 Da by MALDI MS) agrees well with the molecular weight of the hypothetica

251 gnificant discrimination among protein folds agrees well with the number of independent parameters es

252 A multilayer Mie theory model agrees well with the observations, indicating that lower

253 th low levels of pollen since this technique agrees well with the organoleptic analysis.

254 real drug experiments shows that the result agrees well with the prior drug MOA knowledge.

255 This observation agrees well with the proposed role of the M-box riboswit

256 culated on the basis of the mode frequencies agrees well with the results obtained from the electron

257 stematic, may be applied to any network, and agrees well with the results of simulations in all cases

258 ncreased by phosphorylation, and this result agrees well with the significant increase in the K(actin

259 The measured propagation of shear waves agrees well with the simulation results obtained from fi

260 d channels, for which the measured SPR curve agrees well with the single SPR curve calculated using t

261 The bundle stoichiometry in the mesophase agrees well with the size found in solution for alpha-he

262 The resulting membrane curvature agrees well with the size of RC-LH1-PufX tubular vesicle

263 This path agrees well with the small experimental effects of subst

264 anoshells measured by the NIR-MSI microscope agrees well with the spectra calculated theoretically us

265 etic field are observed to be avoided, which agrees well with the theoretical predictions considering

266 richia coli cultures, and the activity trend agrees well with the thermodynamic predictions.

267 erage spacing between two adjacent nanowires agrees well with the thickness of single atomic layer of

268 The experimentally recorded focal force maps agree well with theoretical predictions based on a dipol

269 fragment ions into unoccupied spectral space agreed well with theoretical predictions from averagine-

270 corresponding effective permeability, which agrees well with theoretical predictions.

271 show that the magnitude of the Hanle signal agrees well with theory, and that the spin lifetime vari

272 TAN values determined by the technique agree well with those by the titration method.

273 t the results obtained from the iTRAQ method agree well with those determined by other conventional m

274 otofilaments from our PRIME20/DMD simulation agree well with those from solid state NMR experiments.

275 In both cases, the deduced values of rhoeta agree well with those measured using viscosity and densi

276 The dimensions determined by SAS agree well with those obtained by (dried-state) atomic f

277 gle distributions and (3)J(C'C') values that agree well with those of a recent maximum entropy analys

278 The Q values of the V(BM) tuning curve agree well with those of cochlear neurons across species

279 oth NPs and RPM concentrations were found to agree well with those of the IOSH respirable cyclone and

280 The predicted probe-protein interactions agree well with those seen in the complexes of HEWL with

281 lesions outlined by the automated algorithm agreed well with those defined manually in consensus by

282 valent diameter for quantifying GFs with AFM agreed well with those determined by substrate-free HTDM

283 onstants derived from the transient kinetics agreed well with those from the conventional Stern-Volme

284 tes obtained using the benchmarking approach agreed well with those from the mass balance approach (1

285 icients (D) measured using MBL-DGT generally agreed well with those measured by Chelex-DGT (DMBL/DChe

286 The results agreed well with those obtained by hydride generation co

287 PET-derived (124)I concentrations agreed well with those obtained by well counting of surg

288 using the [(2)H(4)]AEA and HPLC-MS/MS method agreed well with those obtained using the [(3)H]AEA radi

289 ts obtained for "real-world" patient samples agreed well with those of the conventional immunosorbent

290 dicating that smartphone-based test acuities agreed well with those of the ETDRS and Snellen charts.

291 Measured spectra agreed well with those predicted.

292 ial fraction obtained with caval subtraction agreed well with those with fluorescent microspheres (me

293 f the out-of-plane displacements in graphene agrees well with those observed in experiments and can e

294 The extended model agrees well with two sets of detailed quantitative data

295 ve locations on either side of the resonance agree well with universal theory, whereas a systematic d

296 s solution and describe a kinetic model that agrees well with UVRR results.

297 timate of SSDE for the whole scan range that agreed well with values from an image-by-image approach,

298 on of bacteria in samples of sugar cane, and agreed well with values obtained using other methods.

299 ion of fructose in real samples of semen and agrees well with values obtained from conventional metho

300 detection of cholesterol in real samples and agrees well with values obtained from the conventional m