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1 ends were consistent between theoretical and experimental results.
2 conductivity, which completely describes our experimental results.
3 different chromophore protonation states in experimental results.
4 l, and fungal cells from previously reported experimental results.
5 on state model is also in agreement with the experimental results.
6 e hydroxylation that accounts for many prior experimental results.
7 as sufficient to mechanistically explain our experimental results.
8 fracture mechanics principles well model our experimental results.
9 ted that omitting K(+) channels supports our experimental results.
10 te configurations were in agreement with the experimental results.
11 two catalytic mechanisms to account for our experimental results.
12 exed Fe(III)SRFA is most consistent with our experimental results.
13 ble and point to misinterpretation of recent experimental results.
14 ellent agreement between the theoretical and experimental results.
15 nterparticle interaction potentials based on experimental results.
16 ic systems, showing excellent agreement with experimental results.
17 d the emission rate enhancements support the experimental results.
18 lose resemblance between the simulations and experimental results.
19 finite element simulations are fitted to the experimental results.
20 y the theoretical model and by the analogous experimental results.
21 al models and the difficulty of interpreting experimental results.
22 The model largely supported the experimental results.
23 ng it difficult for researchers to interpret experimental results.
24 pparent discrepancy in the interpretation of experimental results.
25 these simulations did not exactly match the experimental results.
26 electronic band structure to rationalize the experimental results.
27 er models aided in the interpretation of the experimental results.
28 eans of AIMD simulations and compared to the experimental results.
29 simplified theories are consistent with the experimental results.
30 so established, which compares well with the experimental results.
31 as accurate as a MCC model in describing the experimental results.
32 full-length domain, consistent with previous experimental results.
33 We draw conclusions in light of the experimental results.
34 computational study provides insights to the experimental results.
35 age-matched healthy controls, confirming our experimental results.
36 greement is found between the simulation and experimental results.
37 geted in-depth studies rationalizing complex experimental results.
38 nterpretation of biological observations and experimental results.
39 are being developed in order to explain the experimental results.
40 ser powder bed interactions to elucidate the experimental results.
41 combined therapy provide good agreement with experimental results.
42 ned about 10(-19) m(2)/V(2) by analyzing the experimental results.
43 ich the model's behavior was consistent with experimental results.
44 l simulations, all in perfect agreement with experimental results.
48 These results are important for transferring experimental results across scales and material structur
50 culations yield excellent agreement with the experimental results, allow the assignment of spectral s
52 smatch between modelling predictions and the experimental results allowed us to construct an improved
60 ationalize the stereoselectivity for several experimental results and demonstrate a combined classica
62 derlying mechanism can aid with interpreting experimental results and designing future experiments.
72 e system are in excellent agreement with the experimental results and prove that the measured interac
74 ivisive modulatory mechanism, reproduces our experimental results and suggests that qualitative varia
75 he LSPR measurement response agree well with experimental results and support that the LSPR measureme
77 one receptor are in very good agreement with experimental results and the Perron-cluster cluster anal
80 ations are extensively used to (1) interpret experimental results and understand the atomic-level dyn
81 t simulations showed good agreement with the experimental results, and indicated that for our system
82 onstitutive model is calibrated based on the experimental results, and is used to investigate the mec
97 le as particulate matter (PM).] However, the experimental results are very heterogeneous, and a gener
98 review will cover these studies, focusing on experimental results, as well as covering recent results
99 he researcher in locating key references and experimental results, as well as understanding the featu
103 The results provide insight into recent experimental results by several groups and suggest new w
106 of analytical models that were validated by experimental results, comprehensive understanding of var
107 yclin dependent kinase (CDK) activities, and experimental results concur in showing that progression
116 l materials are widely estimated as 0.5, our experimental results demonstrate that for FN networks th
119 formula calculation and fits to the previous experimental results demonstrate that the quality factor
132 imated in the benchmark test compared to the experimental results for a group of protein complexes.
133 odel simulations were in good agreement with experimental results for both successful and unsuccessfu
135 ted a different activation trend compared to experimental results for different time points of a stre
136 matical model shows excellent agreement with experimental results for silk with various diameters: 50
137 any CV-PAC and demonstrate its validity with experimental results for sodium and potassium ions in pr
141 ase profile is qualitatively consistent with experimental results from micropipette measurements.
149 e crystal structure explains the accumulated experimental results, identifies possible effector bindi
154 hasizing the need for computation to predict experimental results in advance of their measurement.
155 te the approach on crystalline GB1, with our experimental results in good agreement with theoretical
170 the temperature range of 77-297 K, which the experimental results indicated that LBO has very low opt
176 tudy are general in that they explain extant experimental results obtained for both so-called moody a
177 mechanistic studies and slow translation of experimental results obtained in animal models into the
178 e-level tunnel model satisfactorily explains experimental results obtained in three different molecul
179 e importance of continuous reality checks of experimental results obtained in vitro or with genetical
180 ations for single-level tunneling to explain experimental results obtained under a wide range of expe
182 nalytical platform, for visual comparison of experimental results of National Institute of Standards
189 is end, we perform a network analysis of 951 experimental results on DOM-PM interactions, which enabl
191 magnets, which is distinct from the reported experimental results on heavy rare-earth diffusion.
194 lear downturn on the O site, consistent with experimental results on single layer materials but diffe
196 nalize nearly all of the previously reported experimental results on the selectivity of ORR catalyzed
206 egime beneath the East Pacific Rise with our experimental results requires that existing estimates fo
210 on theory (XMCQDPT2) methods and compared to experimental results, revealing that high quantum yields
236 t density functional theory calculations and experimental results showed that the emission is not fro
241 eads to quantitative insights into important experimental results, such as the greater Cas9 tolerance
258 o the extracellular solution, explaining the experimental result that PT in E148A is blocked whether
259 des of intensive study, there are still many experimental results that are not well understood becaus
260 e from that model, and we present additional experimental results that extend our understanding of th
261 In contrast to the reported simulations and experimental results that rear-located surface plasmon o
262 The opposed defined-pathway model stems from experimental results that show that proteins are assembl
264 this has so far proven sufficient to predict experimental results, there is no theoretical reason to
266 theoretical framework, supported by existing experimental results, thus helps us to understand and pr
267 charge transfer in excellent agreement with experimental results, thus providing a guide towards eng
271 Further study is required to extrapolate experimental results to reservoir-scale and to explore t
279 t a well-defined graphene nanostructure with experimental results, we propose a model based on interf
281 investigated at variable concentrations, the experimental results well fit the kinetic equation for c
285 nescence measurements were conducted and the experimental results were compared to molecular docking
286 ubjected to biochemical assay validation and experimental results were in accordance with the in sili
289 omputational results are consistent with the experimental results, where the selected proteins were s
290 uding the quantum size effect reproduces the experimental results, whereas a classical model only pre
300 Furthermore, we quantitatively explain our experimental results within the Landauer framework for q
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