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Volumn 16, Issue 14, 2008, Pages 10596-10610

A proposal for highly tunable optical parametric oscillation in silicon micro-resonators

Author keywords

[No Author keywords available]

Indexed keywords

CRYSTAL RESONATORS; MICROELECTROMECHANICAL DEVICES;

EID: 47249162438     PISSN: None     EISSN: 10944087     Source Type: Journal    
DOI: 10.1364/OE.16.010596     Document Type: Article
Times cited : (74)

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    • Although the waveguide shown, in Fig. 1 is multimoded over a broad spectral range, higher-order modes have quite different mode profiles and dispersion properties compared with the fundamental quasi-TE mode. They are not likely to participate in the FWM process if the pump and signal, waves propagate predominantly in the fundamental quasi-TE mode
    • Although the waveguide shown, in Fig. 1 is multimoded over a broad spectral range, higher-order modes have quite different mode profiles and dispersion properties compared with the fundamental quasi-TE mode. They are not likely to participate in the FWM process if the pump and signal, waves propagate predominantly in the fundamental quasi-TE mode.
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    • The real and imaginary parts of χ(3) are related to Kerr nonlinearity and TPA, respectively [2, An accurate description of SPM, XPM, TPA, and FWM. requires complete information about χ(3, ωi;ωj,-ωk,wl, However, current experimental knowledge is only available for χ3, ωi;ωi, ωiωi, 11,12, As cross-TPA involves the simultaneous absorption of two photons at ωi and ωj, we approximate χ(3, ωi; ωj,-ωj,ωi) ≈ χ(3, ω̄-ω̄,ω̄) where ω̄, ωi, ωj)/)/2. Similarly, FWM involves the annihilation of two pump photons to create a signal and idler photon, and we approximate χ (3)ωs
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    • We fit each set of experimental data (1.2 - 2.2 μm) in Refs. [11, 12] with a fifth-order polynomial, and average them to obtain the silicon nonlinearity. TPA is zero and the Kerr nonlinearity is assumed to be constant for wavelength longer than 2.2 μm.
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    • For completeness, we have included all possible self- and cross-TPA. and induced free carriers from all the three waves and their combinations in the numerical results of this paper
    • For completeness, we have included all possible self- and cross-TPA. and induced free carriers from all the three waves and their combinations in the numerical results of this paper.
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    • In practice, a critical coupling over such a broad spectral region is difficult for a straight bus waveguide, but is possible by using a curved bus waveguide with a curvature similar to the resonator. See
    • In practice, a critical coupling over such a broad spectral region is difficult for a straight bus waveguide, but is possible by using a curved bus waveguide with a curvature similar to the resonator. See T. Carmon, S. Y. T. Wang, E. P. Ostby, and K. J. Vahala, "Wavelength-independent coupler from fiber to an on-chip cavity, demonstrated over an 850nm span," Opt. Express 15, 7677-7681 (2007).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.