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Volumn 21, Issue 9, 1985, Pages 1462-1476

The Quantum Well Self-Electrooptic Effect Device: Optoelectronic Bistability and Oscillation, and Self-Linearized Modulation

Author keywords

[No Author keywords available]

Indexed keywords

ELECTROOPTICAL EFFECTS;

EID: 0022115408     PISSN: 00189197     EISSN: 15581713     Source Type: Journal    
DOI: 10.1109/JQE.1985.1072821     Document Type: Article
Times cited : (498)

References (24)
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    • D. A. B. Miller, D. S. Chemla, D. J. Eilenberger, P. W. Smith, A. C. Gossard, and W. T. Tsang, “Large room-temperature optical nonlinearity in GaAs/Ga 1-x Al x As multiple quantum well structures,” Appl. Phys. Lett., vol. 41, pp. 679–681, 1982.
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  • 5
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    • D. S. Chemla, D. A. B. Miller, P. W. Smith, A. C. Gossard, and W. Wiegmann, “Room temperature excitonic nonlinear absorption and refraction in GaAs/A1GaAs multiple quantum well structures,” IEEE J, Quantum Electron., vol. QE-20, pp. 265–275, 1984.
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    • For a discussion of the Franz-Keldysh effect and the broadening of exciton resonances with field see J. D. Dow and D. Redfield, “Electroabsorption in semiconductors: The excitonic absorption edge,” Phys. Rev., vol. B1, pp. 3358–3371, 1970.
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    • D. A. B. Miller, D. S. Chemla, T. C. Damen, T. H. Wood, C. A. Burrus, A. C. Gossard, and W. Wiegmann, “Optical level shifter and self-linearized optical modulator using a quantum-well self-electrooptic effect device,” Optics Lett., vol. 9, pp. 567–569, 1984.
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    • Miller, D.A.B.1    Chemla, D.S.2    Damen, T.C.3    Wood, T.H.4    Burrus, C.A.5    Gossard, A.C.6    Wiegmann, W.7
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    • Perhaps the closest precedent to the SEED devices is in the interesting work that has been performed on devices using the Franz-Keldysh effect in diodes [15]-[17]. One configuration utilizes the diode in a resonator; this has been considered both theoretically [15] and experimentally [16]. As in the SEED devices reported here, the modulator and photodiode are the same p-n junction. The Franz-Keldysh effect can however only usefully give an increase in absorption with increasing voltage; consequently, the mechanism of bistability from increasing absorption (with decreasing voltage) used in the SEED device (see Section III) is not available and instead a resonator is used as in conventional absorptive bistability to achieve bistability with decreasing absorption. The Franz-Keldysh bistability is therefore a hybrid implementation of conventional absorption bistability. Another configuration using the Franz-Nadysh effect, with an additional separate photodiode for detection and an external transistor to give the gain for bistability, has also recently been reported [17]. Because of the transistor, the cavity is not necessary, and, as in the SEED devices reported here. coherent light is no longer required.
    • Perhaps the closest precedent to the SEED devices is in the interesting work that has been performed on devices using the Franz-Keldysh effect in diodes [15]-[17]. One configuration utilizes the diode in a resonator; this has been considered both theoretically [15] and experimentally [16]. As in the SEED devices reported here, the modulator and photodiode are the same p-n junction. The Franz-Keldysh effect can however only usefully give an increase in absorption with increasing voltage; consequently, the mechanism of bistability from increasing absorption (with decreasing voltage) used in the SEED device (see Section III) is not available and instead a resonator is used as in conventional absorptive bistability to achieve bistability with decreasing absorption. The Franz-Keldysh bistability is therefore a hybrid implementation of conventional absorption bistability. Another configuration using the Franz-Nadysh effect, with an additional separate photodiode for detection and an external transistor to give the gain for bistability, has also recently been reported [17]. Because of the transistor, the cavity is not necessary, and, as in the SEED devices reported here. coherent light is no longer required.
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    • B. S. Ryvkin and M. N. Stepanova, “Bistable optical characteristics of a resonator photocell with two-step optical transitions,” Soy. Tech. Phys. Lett., vol. 8. pp. 413–414, 1982 (translation of Pis ‘ma Zh, Fiz., vol. 8, pp. 951–954, 1982).
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    • Nemenov, M.I.1    Ryvkin, B.S.2    Stepanova, M.N.3
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.