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Nonlinear Optics

T. Kippenberg (2006). Nonlinear Optics. Tobias J. Kippenberg tjk@mpq.mpg.de T.W. H ä nsch Division. Lecture 3. T. Kippenberg (2006). Lecture 3: Review. 2. 2. RHS: Source term. Simplest relationship between E and P is a linear one:. Assuming a plane wave we arrive at the new k-vector.

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Nonlinear Optics

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  1. T. Kippenberg (2006) Nonlinear Optics Tobias J. Kippenberg tjk@mpq.mpg.de T.W. Hänsch Division Lecture 3

  2. T. Kippenberg (2006) Lecture 3: Review 2 2 RHS: Source term. Simplest relationship between E and P is a linear one: Assuming a plane wave we arrive at the new k-vector Lecture 3

  3. T. Kippenberg (2006) Lecture 3: Review of the refractive index and absorption Refractive index Absorption or gain coefficient. Lecture 3

  4. T. Kippenberg (2006) Lecture 3: Review of the Polarization for a two level system The polarization is the Dipole moment per unit volume, where the total dipole moment is: The time dependence of the dipole operator is determined by the Coherences: Lecture 3

  5. T. Kippenberg (2006) Lecture 4: Preview Combine Quantum Mechanics and Classical Electrodynamics 2 2 Electrodynamics Polarization acts as a source term. Quantum Mechanics Goal: Find the relation between E and P Lecture 3

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