2020
DOI: 10.1103/physrevlett.125.134102
|View full text |Cite
|
Sign up to set email alerts
|

Testing Critical Slowing Down as a Bifurcation Indicator in a Low-Dissipation Dynamical System

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
10
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
7
2

Relationship

0
9

Authors

Journals

citations
Cited by 18 publications
(10 citation statements)
references
References 25 publications
0
10
0
Order By: Relevance
“…Although I(t) surpasses J tr , it does so for a short time and, since the nanoLD relaxation time is too long when J is close to o under J tr , the nanoLD is unable to respond properly to real-time changes in I(t). This phenomenon is known as critical slowing down and has been observed in theoretical and experimental problems involving a transcritical bifurcation [46][47][48][49]. As the bifurcation is swept over, the system remains in the now unstable zero state, transitioning to the nonzero state when the control parameter is well above the critical point, regardless of its change rate.…”
Section: Rtd Biased In the Second Pdc Regionmentioning
confidence: 95%
See 1 more Smart Citation
“…Although I(t) surpasses J tr , it does so for a short time and, since the nanoLD relaxation time is too long when J is close to o under J tr , the nanoLD is unable to respond properly to real-time changes in I(t). This phenomenon is known as critical slowing down and has been observed in theoretical and experimental problems involving a transcritical bifurcation [46][47][48][49]. As the bifurcation is swept over, the system remains in the now unstable zero state, transitioning to the nonzero state when the control parameter is well above the critical point, regardless of its change rate.…”
Section: Rtd Biased In the Second Pdc Regionmentioning
confidence: 95%
“…An optimal bias current to momentarily turn the nanoLD on and produce a short yet high optical pulse is found to be J = 214 µA (panel c), with a relatively long response delay (about 150 ps) as the only drawback, consequence of the critical slowing down that is more notorious since the nanoLD is driven way over the threshold. When the current is lowered, there is no critical slowing down [46,47], and the nanoLD turns off faster than it turned on, thus its short duration (roughly 0.5 ns). For a sufficiently high bias current (over 250 µA), the total current J + I(t) is always above J tr and thus the nanoLD is permanently emitting.…”
Section: Rtd Biased In the Second Pdc Regionmentioning
confidence: 99%
“…In terms of dynamical systems, such transitions may result from a time-varying parameter that crosses a bifurcation point. In this context, lasers have been used as "toy models" because they allow to perform controlled experiments, to test the capability of new time series analysis tools for providing reliable indicators alerting of incoming bifurcations (e.g., Masoller et al, 2015;Marconi et al, 2020, where the abrupt switching of the polarization of the emitted light and the crossing of the laser threshold were used to analyze the suitability of a well-known indicator-critical slowing down-to provide reliable warning of the dynamical transition).…”
Section: Photonic Neuronsmentioning
confidence: 99%
“…The exit from the blockade regime is also sensitive to the chosen value of H + /H − and the scan parameters. Generally, nonlinear dynamics under conditions when a parameter is swept across the bifurcation points is an area of research attracting attention in optics and beyond (see, e.g., [24,25] and references therein). The reverse, i.e., ε-positive to ε-negative, scan shows the much narrower range of the soliton-blockade in the plus field, and no solitons in the minus field (see the right column in Figure 6).…”
Section: Controlling Solitons By Tuning the Cw-component: Direct And ...mentioning
confidence: 99%