1994
DOI: 10.1016/0030-4018(94)90714-5
|View full text |Cite
|
Sign up to set email alerts
|

Accessing high-mode oscillations in a delayed optical bistable system

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
2
0

Year Published

1994
1994
2017
2017

Publication Types

Select...
3
2

Relationship

3
2

Authors

Journals

citations
Cited by 8 publications
(2 citation statements)
references
References 11 publications
0
2
0
Order By: Relevance
“…The corresponding sampling frequency used as a control signal g(t) is 21 multiples of the fundamental frequency. In delay differential systems, we can design and generate arbitrary multi-valued waveforms (isomer signals) of higher periodic orders for the fundamental periodic oscillation by adding extra control circuits to the systems (Liu and Ohtsubo 1991;Liu et al 1994). In this example, the control signal is a very small perturbation to the chaotic oscillation and its amplitude is less than 3 % of the bias injection current.…”
Section: Chaos Control In Active Feedback Interferometersmentioning
confidence: 99%
“…The corresponding sampling frequency used as a control signal g(t) is 21 multiples of the fundamental frequency. In delay differential systems, we can design and generate arbitrary multi-valued waveforms (isomer signals) of higher periodic orders for the fundamental periodic oscillation by adding extra control circuits to the systems (Liu and Ohtsubo 1991;Liu et al 1994). In this example, the control signal is a very small perturbation to the chaotic oscillation and its amplitude is less than 3 % of the bias injection current.…”
Section: Chaos Control In Active Feedback Interferometersmentioning
confidence: 99%
“…(4)Here, H is a Heaviside function, c is the feedback gain, po is an offset to the output signal, a and b are the upper and 10wer thresholds of the window comparator, Ts=1lfs is the sampling period, and A=t2-tl is the gate width. The function f represents the system dynamics and is given by f Lp(t-tr)'r] =r-,c~p(t-tr){ 1+b cos [ ;4)(t-tr)~ ~)o] }(5) where r, /1 ' b, ;c, and ipo are system parameters.4~6)Figure 3shows the results of the OPF control of the chaotic attractor. The free running state inFig.…”
mentioning
confidence: 99%