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9 Nonlinear Optics
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Nonlinear susceptibility tensor
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The Physical origin of optical nonlinearities
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Oscillator model:
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Non-resonant nonlinearities
Second-order nonlinearities ((2)) -- Nonlinear frequency mixing
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= 2 - 21= 0 k = k2 -2k 1 = 0 Phase matching
Optical frequency conversion (Second Harmonic generation) Energy conservation Momentum conservation k = 2 - 21= 0 k = k2 -2k 1 = 0 Birefringence Phase Match (BPM)
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QPM Condition: k=(k2-2k )-Gm=0
Ln Lp dij Lp+Ln X Y Z X QPM Condition: k=(k2-2k )-Gm=0
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Overview of third-order phenomena
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The optical Kerr effect and the nonlinear rafractive index
Frequency tripling Phase match problem The optical Kerr effect and the nonlinear rafractive index ( degeneate four-wave mixing) No phase match problem (K: Kerr constant)
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Stimulated Raman scattering
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Resonant nonlinearities
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Saturable absorber Resonant nonlinerarities are third-order nonlinear
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Resonant nonlinearities in semiconductors
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