• Title/Summary/Keyword: Optical bistability

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All Optical Logic Gate Based On Optical Bistability of DFB SOA (DFB SOA의 광쌍안정 특성을 이용한 전광논리구현)

  • Kim, Byung-Chae;Kim, Young-Il;Lee, Seok;Woo, Deok-Ha;Yoon, Tae-Hoon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.04b
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    • pp.112-113
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    • 2002
  • Optical bistability can be applied to the optical logic. optical signal processing and optical memory. We have measured the optical bistability of DFB-SOA and demonstrated all-optical OR logic gate using switching characteristics of DFB-SOA.

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GaAs/AlGaAs MQW waveguide phase modulator with optical bistability (광쌍안정을 갖는 GaAs/AlGaAs MQW 도파로형 위상 광변조기)

    • Korean Journal of Optics and Photonics
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    • v.7 no.3
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    • pp.280-286
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    • 1996
  • This paper describes operation mechanism of a novel optical waveguide phase modulator with optical bistability characteristics by self electro-optic effect. The fabricated device structure is an optical waveguide modulator, using a refractive index change by an applied electric field, parallel integrated with SEED with an electrical bistability. GaAs/AlGaAs MQW is used as the core layer of the waveguide modulator and the absorption layer of SEED. The absorbed optical power in SEED changes the diode voltage and controls the optical power propagating through the waveguide phase modulator. Optical bistability of waveguide phase modulator is experimentally obtained by using electrical bistability of SEED. Compared to other waveguide modulators, the proposed one has an asset that the lowest optical power is required to generate optical bistability.

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All-optical Flip-flop Operation Based on Polarization Bistability of Conventional-type 1.55-㎛ Wavelength Single-mode VCSELs

  • Lee, Seoung-Hun;Jung, Hae-Won;Kim, Kyong-Hon;Lee, Min-Hee
    • Journal of the Optical Society of Korea
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    • v.14 no.2
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    • pp.137-141
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    • 2010
  • We report, for the first time to our knowledge, observation of polarization bistability from 1.55-${\mu}m$ wavelength single-mode VCSELs of a conventional cylinder-shape under control of their driving current, and demonstration of all-optical flip-flop (AOFF) operations based on the bistability with optical set and reset pulse injection at a 50 MHz switching frequency. The injection pulse energy was less than 14 fJ. The average on-off contrast ratio of the flip-flopped signals was about 7 dB. These properties of the VCSELs will be potentially useful for future high-speed all-optical signal processing applications.

Low-threshold Optical Bistability Based on Bound States in the Continuum

  • Kim, Myunghwan;Kim, Sangin;Kim, Soeun
    • Current Optics and Photonics
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    • v.6 no.1
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    • pp.10-14
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    • 2022
  • Low-threshold optical bistability is essential for practical nonlinear optical applications. Many bistable optical devices based on high-quality-factor resonators have been proposed to reduce the threshold intensity. However, demonstrating high-quality-factor resonance requires complex fabrication techniques. In this work, we numerically demonstrate optical bistability with bound states in the continuum in a simple one-dimensional Si photonic crystal. The designed structure supports bound states in the continuum, producing an ultrahigh quality factor without tough fabrication conditions. The threshold intensity of the designed device is 150 MW/cm2 at the optical communication wavelength. This scheme may lead to a new class of nonlinear photonics.

All-optical Flip-flop based on Optical Beating and Bistability in an Injection-locked Fabry-Perot Laser Diode

  • Kim, Junsu;Lee, Hyuek Jae;Park, Chang-Soo
    • Journal of the Optical Society of Korea
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    • v.20 no.6
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    • pp.698-703
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    • 2016
  • We report a new all-optical flip-flop (AOFF) with a quite simple structure, using optical beating in an injection-locked Fabry-Perot laser diode (FP-LD) with optical bistability. While conventional AOFF methods using an injection-locked FP-LD require additional devices such as secondary FP-LDs or polarization controllers for reset operation, the proposed method can be implemented using only a single commercially available FP-LD with set and reset signals. The optical beating induces intensity fluctuations inside the FP-LD, and releases the locking state to the reset state. Even though we demonstrated the AOFF at 100 Mbit/s, we expect that its operation rate could extend to 10 Gbit/s, according to the limit of the FP-LD's frequency response.

A Study on the Optical Bistable Characteristic of a Multi-Section DFB-LD (다전극 DFB-LD의 광 쌍안정 특성에 관한 연구)

  • Kim, Geun-Cheol;Jeong, Yeong-Cheol
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.39 no.8
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    • pp.1-11
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    • 2002
  • A multi-section DFB-LD shows optical bistability subject to externally injected light signal, then it has potential applications such as wavelength conversion and optical logic gates. In this paper, we have studied the optical bistability in multi-section DFB-LD using split-step time-domain model. It is confirmed that the multi-section DFB-LD, which is excited inhomogeneously, shows bistability. The optical bistable characteristics are investigated when input light is injected into a absorptive region. Simulation results show that multi-section DFB-LD works as a flip-flop depending on the set-reset optical pulse which has a few ns in switching time and a few pj in switching energy, so that it can act as a optical logic device. Besides, if we change the carrier lifetime and the differential gain coefficient, it is expected that the response time of optical output signal can be reduced.

Optical bistability in the Fabry-Perot etalon which contains $As_2S_3$ space layer (비정질 $As_2S_3$를 중간층으로 Fabry-Perot 에탈론에서의 광쌍안정에 관한 연구)

  • 김강호;김석원;한성홍
    • Korean Journal of Optics and Photonics
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    • v.8 no.6
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    • pp.466-470
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    • 1997
  • We fabricated the asymmetric Fabry-Perot etalon which contains amorphous $As_2S_3$ as a spacer layer by using the method of optical multilayer coating and observed the optical bistability with the polarization. Optical thickness of the spacer layer is 2$\lambda$ at $Ar^+$ ($\lambda $=514.5 nm) laser wavelength. Optical bistability was observed at the intensities between 80~100 mW and the experiment shows us that the trends of bistable loop of the reflected and the transmitted lights are quite different depending on the state of polarization. This phenomena can be explained as the phase differences of each polarizations are different in the nonlinear Fabry-Perot etalon.

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