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Optics Express

Lossless optical modulation in a silicon waveguide using stimulated Raman scattering

Richard Jones, Ansheng Liu, Haisheng Rong, Mario J. Paniccia, Oded M. Cohen, Dani Hak

Published Jan 1, 2005• 78 citations
Publisher

Abstract

In this paper we describe a new modulation scheme using stimulated Raman scattering in conjunction with a reverse biased p-i-n diode embedded in a silicon waveguide. We show optical modulation of a weak probe beam by modulating the reverse bias voltage of the silicon waveguide excited by a strong pump beam. The probe beam modulation is due to the two-photon absorption-induced carrier density modulation in the waveguide. By tuning the probe wavelength to the Stokes wavelength, we demonstrate for the first time a lossless optical modulator in silicon with modulation speeds up to 80-MHz.

DOI
10.1364/opex.13.001716

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In this paper we describe a new modulation scheme using stimulated Raman scattering in conjunction with a reverse biased p-i-n diode embedded in a silicon waveguide. We show optical modulation of a weak probe beam by modulating the reverse bias voltage of the silicon waveguide excited by a strong pump beam. The probe beam modulation is due to the two-photon absorption-induced carrier density modulation in the waveguide. By tuning the probe wavelength to the Stokes wavelength, we demonstrate for the first time a lossless optical modulator in silicon with modulation speeds up to 80-MHz.
We analytically demonstrate the slow down factor enhancement of slow light induced by stimulated Raman scattering in a silicon-on insulator waveguide with a p-i-n Structure. An analytical model is derived for group delay simulation by taking into account of propagation loss and free carrier absorption. It is shown that applying a variable reverse bias voltage to the waveguide decreases the FCA and thus the maximum group delay can be enhanced. Tunable delay time is achievable through applying different bias voltages.
This paper presents a new model for an absorptive-dispersive optical bit memory using stimulated Raman scattering slow-light (SRS). The structure of our model is developed in a low loss silicon-on-insulator (SOI) waveguide based on Stimulated Raman Scattering (SRS). Waveguide has two parts, Raman cell and feedback pass. This model functions as a memory bit and can store an optical pulse by generating a pulse train in the output. Also by using a p-i-n diode structure in Raman cell, the delay time between OB output pulses can be tuned through changing the bias voltage.
A frequency-unshifted and backward stimulated scattering can be efficiently generated in one-photon-absorption free but two-photon absorbing materials. Using a number of novel two-photon absorbing dye solutions as the scattering media and nanosecond pulsed laser as the pump beams, a highly directional backward stimulated scattering at the exact pump wavelength can be readily observed once the pump intensity is higher than a certain threshold level. The spectral and spatial structures as well as the temporal behavior and optical phase-conjugation property of this new type of backward stimulated scattering have been experimentally studied. This stimulated scattering phenomenon can be explained by using a model of two-photon-excitation enhanced standing-wave Bragg grating initially formed by the strong forward pump beam and much weaker backward Rayleigh scattering beam; the partial reflection of the pump beam from this grating provides an positive feedback to the initial backward Rayleigh scattering beam without suffering linear attenuation influence. Comparing to other known stimulated (Raman, Brillouin, Rayleigh-wing, and Kerr) scattering effects, the stimulated Rayleigh-Bragg scattering exhibits the advantages of no frequency-shift, low pump threshold, and low spectral linewidth requirement.