Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Applied Optics

Kerr bistability in a 3 × 3 coupler optical fiber ring resonator

Y. H. Ja

Published Sep 20, 1993• 21 citations
Publisher

Abstract

We present a theoretical study of bistability in an optical fiber ring resonator connected to a 3 × 3 fiber coupler. The bistability is caused by the Kerr effect when the ring resonator is working in the nonlinear regime. The dependence of the bistability on various parameters of the fiber and the coupler is investigated.
DOI
10.1364/ao.32.005310

Related papers

Kerr bistability in an optical fiber ring resonator with a 3 × 3 planar fiber coupler

Y. H. Ja

A theoretical study of bistability caused by the optical Kerr effect in a type 1 optical fiber ring resonator connected to a 3 × 3 planar coupler is presented. The dependence of the bistability on various parameters of the fiber and the coupler is investigated. A comparison between the bistable characteristics of this ring resonator and those of a fiber ring resonator with a 3 × 3 equilateral triangular (nonplanar) fiber coupler is made.

Applied Optics•Oct 20, 1994•0 citations

Kerr bistability in optical fiber loop resonators with a 3 × 3 fiber coupler

Y. H. Ja

Abstract A theoretical study of bistability caused by the Kerr effect in two types of optical fiber loop resonators connected to a 3 × 3 coupler is carried out. The dependence of the bistability on various parameters of the fiber and the coupler is investigated and presented as graphs. The bistability offers the possibility of using these fiber loop resonators as optical logic gates, memories, switches, and differential amplifiers. © 1993 John Wiley & sons, Inc.

Microwave and Optical Technology Letters•Apr 1, 1993•4 citations

Multiple bistability in an optical-fiber double-ring resonator utilizing the Kerr effect

Y.H. Ju

We present a theoretical study of multiple bistability in an optical-fiber double-ring resonator. The multiple bistability is caused by the optical Kerr effect, which modulates the refractive index of the fiber. The dependence of the multiple bistability on various parameters of the fibers and the couplers is investigated.>

IEEE Journal of Quantum Electronics•Feb 1, 1994•26 citations

Optical bistability in a two-coupler fiber ring resonator by using degenerate two-wave mixing

Y. H. Ja

A theoretical study of bistability in a two-coupler optical fiber ring resonator is presented. The bistability is caused mainly by the degenerate two-wave mixing in which the circulating intensity of the fiber ring depends on the intensity ratio of the signal to the pump beams. The dependence of the bistability on various parameters of the fibers and the couplers is investigated.

Optics Letters•Oct 1, 1992•9 citations

Optical bistability in a one planar 3 × 3 coupler fiber‐ring resonator with degenerate two‐wave mixing

Y. H. Ja

Abstract A theoretical study of optical bistability in a Type 1 one (planar 3 × 3) coupler fiber‐ring resonator with an all‐fiber scheme, Scheme B, of degenerate two‐wave mixing (DTWM) is presented. The bistability is caused by the DTWM, the inherent positive feedback in the fiber‐ring resonator and the nonlinear dependence of the circulating intensity of the fiber‐ring resonator on the DTWM gain. The relations between the bistability and various parameters of the fibers and the planar 3 × 3 coupler are inuestigated. A comparison between the bistability in such a jiber‐ring resonator and that using an equilateral triangular 3 × 3 fiber coupler is also made. © 1994 John Wiley & Sons, Inc.

Microwave and Optical Technology Letters•Dec 5, 1994•0 citations

COUPLER-LOSS AND COUPLING-COEFFICIENT DEPENDENCE OF BISTABILITY AND INSTABILITY IN A FIBER RING RESONATOR: NONLINEAR BEHAVIORS

Preecha P. Yupapin, P. Saeung, W. Suwancharoen

In this paper we demonstrate the dynamic simulation of light traveling in a nonlinear fiber optic ring resonator (FORR) with a single coupler. The mathematical relations describing the nonlinear characteristics of the FORR are derived from light transmission theory in linear optical systems. Optical nonlinear phenomena such as bifurcation and chaos are investigated for optical bistability and the Ikeda instability. It is found that for the Ikeda instability of light inside a FORR, the ring-cavity lifetime is much longer than the Kerr-effect response time of the fiber ring. Transmission curves of bistability and instability are shown as a function of the coupler insertion losses (γ) and the coupling coefficients (κ).

Journal of Nonlinear Optical Physics & Materials•Mar 1, 2007•13 citations
Abstract A theoretical study of optical bistability in a Type 1 one (planar 3 × 3) coupler fiber‐ring resonator with an all‐fiber scheme, Scheme B, of degenerate two‐wave mixing (DTWM) is presented. The bistability is caused by the DTWM, the inherent positive feedback in the fiber‐ring resonator and the nonlinear dependence of the circulating intensity of the fiber‐ring resonator on the DTWM gain. The relations between the bistability and various parameters of the fibers and the planar 3 × 3 coupler are inuestigated. A comparison between the bistability in such a jiber‐ring resonator and that using an equilateral triangular 3 × 3 fiber coupler is also made. © 1994 John Wiley & Sons, Inc.
In this paper we demonstrate the dynamic simulation of light traveling in a nonlinear fiber optic ring resonator (FORR) with a single coupler. The mathematical relations describing the nonlinear characteristics of the FORR are derived from light transmission theory in linear optical systems. Optical nonlinear phenomena such as bifurcation and chaos are investigated for optical bistability and the Ikeda instability. It is found that for the Ikeda instability of light inside a FORR, the ring-cavity lifetime is much longer than the Kerr-effect response time of the fiber ring. Transmission curves of bistability and instability are shown as a function of the coupler insertion losses (γ) and the coupling coefficients (κ).