Transverse and Quantum Effects in Superfluorescence; Pump Dynamics for Three-Level Superfluoresence; An Algorithm for Transverse, Full Transient Effects in Optical Bistability in a Fabry-Perot Cavity.

1983 ◽  
Author(s):  
F. P. Mattar
Keyword(s):  
Optical Bistability ◽  
Quantum Effects ◽  
Transient Effects ◽  
Fabry Perot

Transverse optical bistability and formation of transverse structures in a sodium-filled Fabry-Pérot resonator

1992 ◽  
Vol 45 (7) ◽  
pp. R4237-R4240 ◽  
Author(s):  
J. Nalik ◽  
L. M. Hoffer ◽  
G. L. Lippi ◽  
Ch. Vorgerd ◽  
W. Lange
Keyword(s):  
Optical Bistability ◽  
Transverse Optical ◽  
Fabry Perot

Optical bistable switching in pyran dye-doped polymers

2014 ◽  
Vol 23 (02) ◽  
pp. 1450018 ◽  
Author(s):  
Purnima ◽  
Devendra Mohan
Keyword(s):  
Solid State ◽  
Communication Systems ◽  
Optical Bistability ◽  
Nonlinear Refraction ◽  
Nonlinear Behavior ◽  
Single Mode ◽  
Third Order ◽  
Bistable Switching ◽  
Fabry Perot ◽  
Doped Polymers

In the present frame of work, optical bistability using a Fabry–Perot (FP) cavity containing 4-dicyanomethylene-2-methyl-6-p-dimethylaminostyryl-4H-pyran (DCM) dye entrapped in poly-methylmethacrylate (PMMA) matrix is experimentally investigated. Optical nonlinear behavior of solid-state samples is studied using a single-mode Q-switched nanosecond Nd:YAG laser operating at 532 nm. Various optical nonlinear parameters such as nonlinear refractive index (n2) and third-order susceptibility (χ3) of the material are numerically estimated from bistability loops. The origin of optically bistable behavior is attributed to photoisomerization-assisted nonlinear refraction phenomenon. It is observed that nonlinear refraction dominates over nonlinear absorption in giving rise to the optical bistability. The study shows that DCM dye entrapped in solid-state matrices are promising candidate for polymer-based optical switches, data processing, and communication systems.

Observation of bifurcation to chaos in a passive all-optical Fabry-Perot resonator: a high-frequency optical modulator

1984 ◽  
Vol 313 (1525) ◽  
pp. 405-409
Keyword(s):  
Excellent Agreement ◽  
High Frequency ◽  
Optical Bistability ◽  
Time Dependent ◽  
Optical Modulator ◽  
Round Trip Time ◽  
Round Trip ◽  
Trip Time ◽  
Fabry Perot ◽  
All Optical

We report the first observations of bifurcation routes to chaos in an all-optical resonator. Generation of associated deep and sustained Ikeda oscillation of the smooth CO 2 laser input pulses at twice the round-trip time of the Fabry-Perot resonator provides a high-frequency ( ca .0.1 GHz) passive optical modulator device. Results are in excellent agreement with our adaption of optical bistability theory to the time-dependent regime

Large non‐biased all‐optical bistability in an electroabsorption modulator using p‐i‐n‐i‐p diode and asymmetric Fabry–Perot cavity structure

1996 ◽  
Vol 68 (23) ◽  
pp. 3216-3217 ◽  
Author(s):  
O. K. Kwon ◽  
K. Kim ◽  
K. S. Hyun ◽  
J. H. Baek ◽  
B. Lee ◽  
...  
Keyword(s):  
Optical Bistability ◽  
Electroabsorption Modulator ◽  
Cavity Structure ◽  
Fabry Perot ◽  
All Optical

Optical Bistability by Using a Tunable Fibre Laser with Fibre Fabry–Perot

2004 ◽  
Vol 21 (11) ◽  
pp. 2201-2204 ◽  
Author(s):  
L Guo-Hui ◽  
Ye Hong-An ◽  
Li Jun-Qing ◽  
Sun Xiu-Dong ◽  
Zhang Xin-Ming
Keyword(s):  
Optical Bistability ◽  
Fibre Laser ◽  
Fabry Perot

Optical Bistability from Ferroelectric Fabry-Perot Interferometer

2007 ◽  
Vol 355 (1) ◽  
pp. 140-144 ◽  
Author(s):  
Abdel-Baset M. A. Ibrahim ◽  
D. R. Tilley ◽  
Junaidah Osman
Keyword(s):  
Optical Bistability ◽  
Fabry Perot
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