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The difference in the simulated (Figure 4b) and experimental (Figure 4c) values is attributed to the deviation in the nature of ideal graphene layer used in simulation in comparison to that in the experiment.
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In the initial stage of the bias stress process the standard deviations from the mean values tend to be larger, which is mainly attributed to the difference in the fabrication process of all these OFETs.
Similar deviations of GH3 observed in other studies[ 20, 22] were attributed to the difference in construction of GH3, which measures health relative to other people, and the construction of GH1 and GH5, which measure absolute health.
The decrease of the standard deviation in the CI results is attributed to the increase in the effective number of samples due to resampling using bootstrap principles.
This deviation is reasonably attributed to the nominal difference in 'J' values under those two respective cases.
These deviations are attributed to the distribution of the fluid velocity in the tube.
The deviation in size as compared to DLS data is attributed to the distortion of the micelles upon deposition and subsequent drying as well as to the choice of the AFM tip.
These deviations can be attributed to the changes in machine tool dynamics under cutting conditions which are difficult to measure.
The greater deviation in the analytic model was attributed to the difficulty in estimation of a representative saturated thickness in an unconfined aquifer.
The arabinan recovery is inflated (115% mass) and this is attributed to the large standard deviation of arabinose measurements in the liquid fraction as discussed earlier.
The relative deviations are more significant, that is, >15% in some cases, which can be attributed to the change in load to the ICBs.
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