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The first bound gives the minimal velocity 1 / c below which the stationary state might be unstable, in this case, even for smaller speed, the state is stable as one can see from the CV boundary.
From Eqs. (7) and (8), it follows that the stability of the splay state can be inferred, for arbitrary coupling strength, from the sign of F ( 1 ) − F ( 0 ) : in excitatory (inhibitory) networks, the state is stable whenever F ( 0 ) > F ( 1 ) ( F ( 0 ) < F ( 1 ) ).
If the state is stable then it must also be true that the initial numbers of LTP, STP and ND cells are the same for every passage.
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If the unperturbed state was reached again we concluded that the state was stable.
Numerical examples seem to indicate that at most two of the states are stable.
The transition occurs in less than 25 nanoseconds, the limit of what the team could detect; the states are stable even when the power is off and can be switched back and forth repeatedly.
According to the mean field approximation the spontaneous state is stable for the first two values of λ̅ and unstable for the third.
At this minimum fluidization velocity, the fluidization state is stable and the bed height remains constant over the whole simulation time.
For SWCNTs with diameter below the first threshold diameter, the circular state is stable.
It can be also seen that the fluidization state is stable and the expansion ratio remains constant.
Resuscitation attempts did not lead to a higher recovery of colony forming units indicating the VBNC state is stable under the conditions tested.
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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