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Therefore, for a model of fission yeast, Cdc25 is essential, whereas the homologue Mih1 in budding yeast is not [13].
The overall results obtained from our model are in accordance with the existing ODE model of fission yeast [10].
A Boolean model of fission yeast was published recently [21], also based on Sveiczer, et al., 2000 but that was similar to the model we constructed.
In the Boolean model of fission yeast [31] the attractor size predicted by the specific network is compared with that predicted by randomly connected networks with the same number of inhibiting and activating links, self-degrading and self-activating links and the same activation thresholds.
Although only spatial regulation was reflected in the present model of fission yeast, other cells, such as frog eggs, may also have similar ways of transferring spatial information directly, but this has not been experimentally established.
We propose a model of fission yeast inner kinetochore structure in which the variable linkers between irregularly placed CENP-A nucleosomes are occupied by CENP-T-containing particles, at least some of which are CENP TWSX particles in close proximity to CENP-A nucleosomes bound by CENP-C.
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This paper focuses on the modelling of fission gas release in mixed oxide fuel.
Implications are discussed in terms of directions of research for the improved modeling of fission gas behavior for engineering purposes.
The updated models of fission gas release, fuel core swelling, and rod deformation are incorporated into the correspondence routines in MACSIS MOD1.
In this paper, a simple approach to modeling of fission gas trapping is employed which reveals a potential correlation between the position of the rod within the fuel assembly (and therefore the degree of circumferential burnup non-uniformity) and the degree of fission gas trapping.
The objective of the development of the code system KESS is simulating the processes of core melting, relocation of core material to the lower head of the reactor pressure vessel (RPV) and its further heatup, modelling of fission product release and coolability of the core material.
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model of cleavage
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