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

6 nsity and group order during this transition agrees well with a generic self-propelled particle model

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

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

9 OCTA-based simulated VF agreed well with actual 24-2 VF in terms of both the loc

10 These observations agreed well with AFM experiments and provided new insigh

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

12 The R-PO(4) pool agrees well with ammonium oxalate (AO)-extractable phosp

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

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

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

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

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

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

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

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

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

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

23 These agreed well with corresponding experimentally determined

24 Results on real data agree well with current knowledge.

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

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

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

28 pologies and relative transition time scales agree well with direct estimates from time-dependent mol

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

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

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

32 p exponents obtained from two kinds of tests agree well with each other.

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

34 online and offline coupling of AF4-NTA also agreed well with each other.

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

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

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

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

39 Calculations agree well with experiment with slight deviations for sa

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

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

42 Both responses are shown to agree well with experiment.

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

44 lectronic promotion to the 1(1)paipai* state agrees well with experiment, and results in nonadiabatic

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

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

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

48 nctions of non-dimensional parameters, which agree well with experimental data.

49 numerical simulations, and the model results agree well with experimental data.

50 spark frequency, and Ca(2+) amplitude, which agree well with experimental data.

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

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

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

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

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

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

57 Numerical simulations agree well with experimental results and reveal that a b

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

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

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

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

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

63 Our model predictions agreed well with experimental observations and suggested

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

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

66 The predicted behavior agrees well with experimental data.

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

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

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

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

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

72 22), over the temperature range of 277-330 K agrees well with fibrillation experiments and transmissi

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

74 tem parameters is calculated and the results agree well with full numerical simulations.

75 The model agrees well with genome-scale in vivo transposon mutagen

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

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

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

79 The results agree well with ICP-AES, which used as a reference metho

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

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

82 ial biomass to total SOC predicted by MIMICS agree well with independent observations from globally d

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

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

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

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

87 These values agree well with literature values determined by accepted

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

89 The observed rotational transitions agree well with low-frequency rotational dynamics of sin

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

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

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

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

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

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

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

97 The simulations agreed well with measurements of the cochlear partition

98 hat DWS-microrheological [Formula: see text] agrees well with mechanically measured [Formula: see tex

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

100 .82-1.18) over the 4 day deployment and also agreed well with Metsorb-DGT (CMBL/CMetsorb = 0.84-0.94)

101 Experimental results agree well with model predictions, thereby illustrating

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

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

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

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

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

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

108 The theoretical prediction agrees well with numerics.

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

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

111 These results agree well with our numerical simulations of a chaotic H

112 The experimental results agree well with our theoretical calculations.

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

114 This agrees well with our computational investigation, where

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

116 The experimental observation agrees well with our theoretical calculations and is una

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

118 The measured fetal concentrations agreed well with PBK-modeled predictions.

119 bstrates better than Sph3(h), a finding that agrees well with PelA(h)'s highly electronegative bindin

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

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

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

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

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

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

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

127 AXS and AFM experiments, an observation that agreed well with previous biochemical and functional ana

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

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

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

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

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

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

134 This agrees well with previous molecular dynamic simulations

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

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

137 constants ranged from 60 to 400 d(-1), which agree well with prior laboratory studies.

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

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

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

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

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

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

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

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

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

147 The theoretical predictions agree well with results from guided ion beam experiments

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

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

150 Our results agree well with simulations and with the traditional qua

151 They agree well with simultaneous measurements of HONO by Las

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

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

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

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

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

157 we predicted PID rates in 4 age groups that agree well with surveillance data.

158 Our measurements agree well with T-G gas theory.

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

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

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

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

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

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

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

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

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

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

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

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

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

172 The experimental results agree well with the developed theory.

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

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

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

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

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

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

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

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

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

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

183 ration results obtained for 1800 and 4000 nm agree well with the frequency-resolved optical gating me

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

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

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

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

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

189 d pressure conditions (10(-6)-1 Torr), which agree well with the populations determined from APXPS.

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

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

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

193 y obtained dispersion relations are shown to agree well with the predictions of a numerical model.

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

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

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

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

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

199 polymerase chain reaction (ddPCR) techniques agree well with the results.

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

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

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

203 al quantum efficiency of ~28.5% ph/el, which agree well with the theoretical maximum values from opti

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

205 The experimental observations agree well with the trends obtained from density functio

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

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

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

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

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

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

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

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

214 The results agreed well with the landscapes reconstructed by establi

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

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

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

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

219 The NTA results from both methods agreed well with the mean size and relative variance val

220 Our results agreed well with the most recent theoretically calculate

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

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

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

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

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

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

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

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

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

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

231 This agrees well with the calculated tumor control probabilit

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

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

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

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

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

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

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

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

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

241 is S(N)2-like reaction in the adenine system agrees well with the experimental value of 102.7 kJ/mol.

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

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

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

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

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

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

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

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

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

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

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

255 Our theoretical analysis agrees well with the scattering rates extracted from mea

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

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

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

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

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

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

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

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

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

265 mille to -0.18 per mille, respectively, and agreed well with theoretically predicted values for equi

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

267 ltiple temperatures and water concentrations agree well with this interpretation.

268 These values are comparable and agree well with those determined by others in the litera

269 ition profiles of PFAS in Antarctic seabirds agree well with those expected from long-range transport

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

271 g interface and regions with direct contacts agree well with those in the solid-state structure, as c

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

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

274 EUV TOF results agree well with those obtained on the same enriched pell

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

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

277 Overall, these findings agree well with those of previous biochemical studies an

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

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

280 Models agreed well with those based on children from the United

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 hotosynthetic electron transport rate, which agrees well with two existing photosynthesis models (Far

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

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

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

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

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

300 It agrees well with VF_MD in early glaucoma but underestima