2/44 Foundation of nonlinear Optics II

  Рет қаралды 14,697

ISPNLO

ISPNLO

Күн бұрын

This lecture focuses on fundamentals in crystal and parametric optics. It aims at giving guidelines and tools for understanding the main concepts as well as the design, characterization and use of crystals for optical parametric generation. The following main aspects are detailed. •Constitutive relations and Maxwell equations. •Classification of the nonlinear interactions using the corpuscular approach: fusion and splitting involving three or four photons, spontaneous and stimulated processes. •Calculation of the electric susceptibility from the Lorentz model: perturbation approach leading to the definition of the different orders of the electric susceptibility, wavelength dispersion, intrinsic symmetries (Kleinman and ABDP), implications of spatial symmetry on the susceptibility tensors (Neumann principle). •Tensors algebra and calculation of the first, second and third order polarizations. •Modelling of the macroscopic nonlinearities of matter from the microscopic scale using the bond charge model and ab initio calculations, Miller index. •Basics in linear crystal optics: propagation equation, index surface, birefringence, double refraction, eigenmodes. •Amplitude equations in the nonlinear regime, Manley-Rowe relations. •Calculation of the effective coefficient based on the field tensor formalism. •Types and topology of collinear and non-collinear Birefringence Phase-Matching and Quasi-Phase-Matching in bulk media and whispering-gallery-mode resonators. •Integration of the amplitude equations and calculation of the conversion efficiencies associated with second harmonic generation (SHG), direct and cascaded third harmonic generation (THG), spontaneous parametric down-conversion (SPDC), optical parametric amplification (OPA), optical parametric generation (OPG), optical parametric oscillation (OPO). •Angular, spectral and thermal acceptances. •Spatial and temporal walk-off effects. •Techniques of characterization of nonlinear crystals: refractive indices, phase-matching and quasi-phase-matching loci, conversion efficiencies, magnitudes and relative signs of the nonlinear coefficients, acceptances. •The main nonlinear crystals for optical parametric generation, from ultraviolet to THz.

Пікірлер: 10
@Lephysicien1993
@Lephysicien1993 4 жыл бұрын
Very good lecture
@vstvgn4240
@vstvgn4240 Жыл бұрын
at 34:54, is there a typo for the expression of centrosymmetrical potential? The restoring force term should not contain order of even, rigtht?
@live4Cha
@live4Cha 5 жыл бұрын
Do you answer questions here prof Boulanger? Thnx
@daulandeyoung8884
@daulandeyoung8884 2 жыл бұрын
Where can I get these slides?
@PiyushRajPlatonic
@PiyushRajPlatonic 6 жыл бұрын
At about 30:45, the lecturer says that energy can be transferred without absorption. How is this possible?
@francescovitale6422
@francescovitale6422 5 жыл бұрын
I think that it is to be related to the time scale at which the elastic scattering process occurs: that is the absoprtion and "instantaneous" re-emission of radiation by the electrons, acting as dipoles at the microscopic level.
@live4Cha
@live4Cha 5 жыл бұрын
Piyush Raj i have same question its very confusing statement!
@live4Cha
@live4Cha 5 жыл бұрын
Francesco Vitale prof says “Energy can be transfered to matter without absorption”. I think this is a flat out wrong statement. The terms “Energy E” and “Absorption A” in optics can be linked to their mechanical definition with dE = F.dx and A = -dP/dx with P as power defined as time rate of energy exchange between two systems. These two definitions should show the interdependence of absorption and energy. What am i missing? Thnx
@jellyfish1679
@jellyfish1679 4 жыл бұрын
I know that this comment in quite old but just to give it a try. I think he just said absorption implying resonant absorption while here he is talking about parametric optics so non resonant absorpion (like scattering). Meaning that he is talking about a transfer of energy to matter that is much lower than the energy necessary to an electronic transition but only to a virtual state.
@Lephysicien1993
@Lephysicien1993 4 жыл бұрын
@@jellyfish1679 The transfer of energy is usually done by absorption and emission where the photon is absorbed or emitted by the electron. There is a set of phenomena called scattering where there is no absorption/emission but an interaction at a distance (mediated by a virtual photon), however that's a more specific case. So, If matter is "a perfect reflector" the energy will not be changed except to change the direction in which it is moving (in fact even for the case of scattering, the electron absorbs the photon and re-emitted another photon with the same frequency with a random direction...)
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