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The initial term explains for indium atoms that first impact the diffusion loop of thickness λ S (called beneath of the effective diffusion length exterior) at the proportion χ S J cos α and after a while shifted to the drop along the sidewalls, with χ S as the pyrolysis effectiveness of TMIn at the superficial surface of substrate.
The first procedure (the reaction loop) operated on a larger timescale than the second (the diffusion loop).
The sampling of new displacement in the diffusion loop was cheap, but the escape rate of the Ca2+ ions leaving the cleft by the absorbing boundary ∂ΩD, was underestimated (41).
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The low frequency loop can take different forms as a convective-diffusion loop, a first order semi-circle or a mixed graph.
To study the impact of diffusion-based loop formation on the conformational properties isolated from effects of the presence of other chromosomes, we simulate single chromosomes in a dilute solution.
This corresponds to the reptation controlled surface self-diffusion of loop-train adsorbed chains with the contour length fluctuation (CLF) and the chain constraint release (CR) contributions.
However, a diffusion-mediated looping mechanism of LCR-gene contact is not ruled out by our results.
Thus, dynamic diffusion-based looping, i.e. gene co-localization, provides a consistent framework for chromatin organization in eukaryotic interphase nuclei.
At the same time, EIS demonstrated formation of a low frequency loop due to diffusion limitations.
The high frequency response characterized the charge transfer process and the low frequency loop identified the diffusion process of oxygen.
In this paper, we derive an analytical expression of a 2D convecto-diffusive impedance taking into account convection along the channel direction, which makes it possible to determine the extent to which the low frequency loop results from diffusion losses in the direction perpendicular to the MEA or from convective phenomena occurring along the channel direction.
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