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For late time, thermally activated quantities such as the dislocation mobility and nucleation rate set the timescale and control the algebraic behavior, respectively.
Also, observations such as cosmic background radiation [10, 11] and large-scale structure [12] provide an indirect evidence for late time acceleration.
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Since for late time-points the error estimates (Brier scores) are based on a small number of observations (generally with few/no events) and are therefore unreliable, the researcher may prefer to evaluate Brier score-based quantities up to a specific time, which would ideally have a clear clinical meaning.
In addition to finding nearby SLSNe that allows for late-time follow-up, PTF is also great for finding all kinds of rare transients.
In total we had 4 datasets that were used for the early time point, and 7 datasets that were used for the late time point (tables 1 and 2).
The solution obtained shows the transient behavior in detail, until the consistent collapse to known profiles for the late time periods.
In addition, two dimensionless shape factors are obtained for the late time, which depend on the injection flow rate and the distance of the rock matrix from the injection point.
The same SPECT protocol was used as described for the late time points in the kinetics experiment.
For the late time point, the lower signal-to-noise ratio made it beneficial to increase the number of angles per subset.
The direct comparison of the runs following control (rn04) and stress induction (rn06) for the late time bin was significant with T 33) = 1.92; p = .032.032
This is partially due to the fact that some of the patients from the ABCSG6 and ABCSG8 trials were censored for the late time interval, because they were treated with extended adjuvant therapy (ABCSG6a, ABCSG16).
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