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It is shown that this mode is stable over the wide range of the excitation frequency.
However, our (first ever) Bloch wave stability analysis of the post-bifurcated equilibrium paths shows that the flower mode is stable for all sufficiently short wavelength perturbations.
In any case, this mode is stable.
Molecular dynamics simulations show that this minor-groove binding mode is stable on a nanosecond scale.
From the range of solid curves, we have the summary of parametric space where a specific mode is stable: The stripes mode is stable when μs- < μ < μs+; the hexagonal mode is stable (H π and H0) when μ < μh- or μ > μh+.
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The average spontaneous frequency recorded in the whole-cell mode was stable at 9±8 Hz during the entire 5 minutes of recording (Fig. 3B).
The functional modes are stable and constant during this period.
If different SSB modes are stable and interconvertible, discrete transitions in the extension would have been expected in the stretching-relaxing experiment.
For U = 0, W = 0, it has been found that the model is gravitationally unstable in the domain ( 0 < x < 1.0667 for m = 0 mode) while it is stable in the domains ( 1.0667 ≤ x ≤ ∞ for m = 0 mode) and ( 0 ≤ x ≤ ∞ for m ≥ 1 modes).
The theoretical analysis and simulation results show that the adaptive quasi-sliding mode control system is stable and convergent.
Whereas the low-energy Goldstone (phase) mode is always stable, additional symmetries are required to prevent the Higgs (amplitude) mode from rapidly decaying into low-energy excitations.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com