Raman gain in silicon photonic wires depends on the relative propagation directions of the pump and Stokes waves due to strong longitudinal mode-field components. Here we show that this Raman-induced nonreciprocity can be varied in a wide range by changing the orientation of the waveguide with respect to the crystallographic axes. In a ⟨001⟩ orientation, the nonreciprocity reaches its maximum which is larger by more than two orders of magnitude as compared to the traditional ⟨011⟩ orientation. The waveguide is then practically Raman-inactive for copropagation, while the contradirectional Stokes wave may experience significant Raman gain.
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Krause et al. (2009) studied this question.
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