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1 ions K as approximately , close to the ideal theoretical value.
2 ish lysate backgrounds were within 5% of the theoretical value.
3 chiometry of O(2)/NADPH is very close to the theoretical value.
4 approximately 8 nm that is comparable to the theoretical value.
5 ncorporation, but to be less than 25% of the theoretical value.
6 d (154)Dy cross sections are higher than the theoretical values.
7 satisfactory, and MWs were in agreement with theoretical values.
8 with quantitative modeling and comparison to theoretical values.
9 e selected and mass accuracy was compared to theoretical values.
10 entally quantified in very good agreement to theoretical values.
11 uently, utilize these models to estimate the theoretical values.
12 rgy densities that could approach their high theoretical values.
13  compare it to the reported experimental and theoretical values.
14 brane fusion is at the lowest range of these theoretical values.
15  the measured values of reflectance with K-M theoretical values.
16 ) were on the same order of magnitude as the theoretical values.
17 ios for X-chromosome probes within 6% of the theoretical values (0.5 for XY/XX, 1.0 for XX/XX, 1.4 fo
18 ding reversible capacity almost equal to the theoretical value (260 mA h g(-1); >257 mA h g(-1) for A
19 urface area (>2600 m(2)/g) very close to its theoretical value (2830 m(2)/g).
20 mAh g(-1) - nearly 2x higher than graphite's theoretical value (372 mAh g(-1)).
21 c capacity of 438 mAh g(-1), approaching the theoretical value (443 mAh g(-1)), a long cyclability an
22 uction via evanescent modes, approaching the theoretical value 4e(2)/pih (where e is the electron cha
23 y of applications, with a slope close to the theoretical value (59.2/z mV).
24 ere exhibits a reversible capacity above its theoretical value (924 mAh g(-1) at 1.12 C), enhanced ra
25              NMR studies and comparison with theoretical values allowed the assignment of the stereoc
26 > is found to deviate significantly from the theoretical value and high correlation between the orien
27 e mean deviation = +/-0.39 kcal mol(-)(1) vs theoretical values and +/-0.52 vs experimental) from thr
28 i(17) cluster are in good agreement with the theoretical values and show a blue shift of approximatel
29 , 40 726.2 Da) is in good agreement with the theoretical value, and a 16 Da mass shift is easily obse
30 action revealed a stoichiometry close to the theoretical value, and adding L-arginine not only initia
31 -1) for the first cycle, more than twice its theoretical value, and maintains its initial capacity af
32 was found to be reliable as the measured and theoretical values based on the ideal gas law were compa
33 ents for length of vessels also diverge from theoretical values, but those for radius show stronger a
34 tely estimate Mn in this study, differing to theoretical values by only 5.2%.
35 /-0.03 S) and are in good agreement with the theoretical value calculated from the crystal structure
36          These distances are consistent with theoretical values calculated from a helical bundle mode
37  of 19-NA glucuronide compared well with the theoretical values (calculated from the conversion of 19
38 teries is limited to a small fraction of its theoretical value due to the build-up of insulating lith
39 he C fragment are in good agreement with the theoretical values expected for fully solvated chains (c
40 h human and P. falciparum PNP agree with the theoretical value for a 1'-(14)C equilibrium isotope eff
41 which agree with our experiments, as well as theoretical value for an atomic analog of electrical ind
42 immune responses for disease therapy, and of theoretical value for determining what aspects of IL-10
43 c methods used in this study provide data of theoretical value for the circumscription of generic and
44 the results are compared to experimental and theoretical values for GaN.
45                                              Theoretical values for nu(3) range from 1.8 to 2.4; thus
46 n lengths on the resulting surfaces approach theoretical values for perfectly flat films.
47                      We have also calculated theoretical values for the capacitance and resistance, w
48 ive energy into residue contributions yields theoretical values for the oligomeric propensity of diff
49 nomial distribution in Sr(2+) solutions gave theoretical values for the third moment of the mean whic
50 CC values were analyzed with assistance from theoretical values obtained from density functional theo
51 the reaction, 0.8 +/- 0.1, is similar to the theoretical value of 1, whereas significantly less produ
52 ent MnO2 of 1,145 F/g, which is close to the theoretical value of 1,380 F/g.
53 ntioselectivity of 2-butanone reduction to a theoretical value of 100% (S)-2-butanol.
54 clay-Fe(II) produced per mol U(VI) produced (theoretical value of 2.0).
55 ies, the La-La distance is comparable to the theoretical value of a La-La covalent bond and is shorte
56                                  Despite the theoretical value of characterizing both intrinsic and e
57 of 0.85 nm and 1.15 nm whereas the predicted theoretical value of SHD radius for NdGaO3 is ~1.01 nm.
58            The former is consistent with the theoretical value of ~3.5-5.0 eV.
59 d discrepancies between the experimental and theoretical values of carrier mobility.
60 y 150% and approximately 60% higher than the theoretical values of defect-free UiO-66 crystal, respec
61                                              Theoretical values of metric parameters and activation e
62 basis of this comparison of experimental and theoretical values of spin relaxation enhancement effect
63 Excellent agreement between experimental and theoretical values of the molecular flux was obtained us
64 muM the binding capacity was only 50% of the theoretical value or even less.
65 le and the N-terminal helix agreed well with theoretical values predicted for a protein the size and
66 values are in relatively good agreement with theoretical values, providing the way for rational desig
67 asurements of the diffusion of apoMb confirm theoretical values showing a approximately 40% increase
68 he flux rate per pore is much smaller than a theoretical value that assumes no friction for the dye m
69 ic PDAA with [mmmm] > 99%, M(n) matching the theoretical value (thus a quantitative initiation effici
70 d mass accuracies, i.e., within 2 mDa of the theoretical value, were obtained in MS and MS/MS operati
71 ranged from -7.0 to 11.3% deviation from the theoretical values with five duplicate assays.
72 ra of all botryococcenes to compare computed theoretical values with those observed.
73 r these complexes were consistent with their theoretical values within 0.01% mass accuracy.

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