1980
DOI: 10.1117/12.7972546
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Optical Feedback And Bistability: A Review

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1984
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Cited by 14 publications
(4 citation statements)
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“…SLM of such kind doesn't need high writing light intensities and can operate with the He-Ne laser light. 7,8,9 this device was used in optical schemes with 2-D feedback. In 10 realization of Fabry-Perrot interferometer containing complex nonlinear medium based on SLM was described.…”
Section: The Experimental Investigationmentioning
confidence: 99%
“…SLM of such kind doesn't need high writing light intensities and can operate with the He-Ne laser light. 7,8,9 this device was used in optical schemes with 2-D feedback. In 10 realization of Fabry-Perrot interferometer containing complex nonlinear medium based on SLM was described.…”
Section: The Experimental Investigationmentioning
confidence: 99%
“…Even a small change of control parameters causes some drastic changes of the pictures which demonstrate solutions. The experiment and its results were described in many papers and books, see for example [3,4]. In the first part of our work [5] (called Paper I), the experiment was described and the static (equilibrium) results were presented for particular control parameters.…”
Section: Introductionmentioning
confidence: 99%
“…The conventional electronic operational amplifier demonstrates similar behavior with the feedback loop. Various optical schemes with positive feedback such as laser, molecular cell inside Fabry-Perot resonator, hybrid schemes with birefringent materials [9] reveal the oscillatory or bistable behavior which also has analogs in electronics and mechanics (harmonic oscillators, triggers). Since the presence of the properly chosen feedback in dynamical system not only improves its performance but can also provide observation of new nonlinear phenomena, we have applied feedback operation concept to the sensor based on the effect of the non-steady-state photo-EMF.…”
mentioning
confidence: 99%
“…Here S is the electrode area, 0 is the average photoconductivity of the sample, L D is the diffusion length of photocarriers, E D =Kk B T/e is the diffusion field, M = 0 / 0 is the Maxwell relaxation time, is the dielectric constant, 0 is the free space permittivity, k B is the Boltzmann constant, and e is the elementary charge, J n ( ) is the Bessel function of the first kind of the n-th order. First let us consider the case of the real gain factor H=H r (8) Im(H r )=0 (9) This situation is typical for conventional analog wideband amplifiers. The phase conditions, i.e.…”
mentioning
confidence: 99%