Impact of reduced or equal unbound nucleation rate.
<p>Median over 100 independent simulation runs of the order parameter <i>S</i><sub>2</sub> (A,B) as function of the control parameter <i>G</i> at s (8 h, 20 min), and (C) as a function of time for LDD, GDD, and ISO nucleation modes as in <a href="htt...
Wedi'i Gadw mewn:
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| Awduron Eraill: | |
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2025
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| Tagiau: |
Ychwanegu Tag
Dim Tagiau, Byddwch y cyntaf i dagio'r cofnod hwn!
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| Crynodeb: | <p>Median over 100 independent simulation runs of the order parameter <i>S</i><sub>2</sub> (A,B) as function of the control parameter <i>G</i> at s (8 h, 20 min), and (C) as a function of time for LDD, GDD, and ISO nucleation modes as in <a href="http://www.ploscompbiol.org/article/info:doi/10.1371/journal.pcbi.1013282#pcbi.1013282.g003" target="_blank">Fig 3</a> and <a href="http://www.ploscompbiol.org/article/info:doi/10.1371/journal.pcbi.1013282#pcbi.1013282.s001" target="_blank">S1 Fig</a>, supplemented by LDD with equal rates for bound and unbound nucleation (LDD equal rates), and GDD with an unbound nucleation rate that is 8.3% of the bound rate (GDD unbound reduced), on a square periodic geometry with sizes m and m. (C) In these simulations, in the case of LDD with equal rates <i>r</i><sub><i>c</i></sub> = 0.0025 s<sup>−1</sup>, in the case of GDD with unequal rates <i>r</i><sub><i>c</i></sub> = 0.00325 s<sup>−1</sup>. Error bars represent the 10th and 90th percentile.</p> <p>(EPS)</p> |
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