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Kleinman symmetry, named after American
physicist A physicist is a scientist who specializes in the field of physics, which encompasses the interactions of matter and energy at all length and time scales in the physical universe. Physicists generally are interested in the root or ultimate cau ...
D.A. Kleinman, gives a method of reducing the number of distinct
coefficients In mathematics, a coefficient is a multiplicative factor involved in some term of a polynomial, a series, or any other type of expression. It may be a number without units, in which case it is known as a numerical factor. It may also be a ...
in the rank-3 second order
nonlinear optical Nonlinear optics (NLO) is the branch of optics that describes the behaviour of light in nonlinear media, that is, media in which the polarization density P responds non-linearly to the electric field E of the light. The non-linearity is typicall ...
susceptibility when the applied frequencies are much smaller than any resonant frequencies.


Formulation

Assuming an instantaneous response we can consider the second order polarisation to be given by P(t) = \epsilon_0 \chi^E^2(t) for E the applied
field Field may refer to: Expanses of open ground * Field (agriculture), an area of land used for agricultural purposes * Airfield, an aerodrome that lacks the infrastructure of an airport * Battlefield * Lawn, an area of mowed grass * Meadow, a grass ...
onto a nonlinear medium. For a lossless medium with spatial indices i,j,k we already have full permutation symmetry, where the spatial indices and frequencies are permuted simultaneously according to \chi_^(\omega_3;\omega_1+\omega_2) = \chi_^(\omega_1;-\omega_2+\omega_3) = \chi_^(\omega_2;\omega_3-\omega_1) = \chi_^(\omega_3;\omega_2+\omega_1) = \chi_^(\omega_2;-\omega_1+\omega_3) = \chi_^(\omega_1;\omega_3-\omega_2) In the regime where all frequencies \omega_i \ll \omega_0 for resonance \omega_0 then this response must be independent of the applied frequencies, i.e. the susceptibility should be dispersionless, and so we can permute the spatial indices without also permuting the frequency arguments. This is the Kleinman symmetry condition.


In second harmonic generation

Kleinman symmetry in general is too strong a condition to impose, however it is useful for certain cases like in second harmonic generation (SHG). Here, it is always possible to permute the last two indices, meaning it is convenient to use the contracted notation d_ = \frac\chi^_(\omega_3;\omega_1,\omega_2) which is a 3x6 rank-2 tensor where the index l is related to combinations of indices as shown in the figure. This notation is used in section VII of Kleinman's original work on the subject in 1962. Note that for processes other than SHG there may be further, or fewer reduction of the number of terms required to fully describe the second order polarisation response.


See also

*
Nonlinear optics Nonlinear optics (NLO) is the branch of optics that describes the behaviour of light in Nonlinearity, nonlinear media, that is, media in which the polarization density P responds non-linearly to the electric field E of the light. The non-linearity ...
*
Second-harmonic generation Second-harmonic generation (SHG), also known as frequency doubling, is the lowest-order wave-wave nonlinear interaction that occurs in various systems, including optical, radio, atmospheric, and magnetohydrodynamic systems. As a prototype behav ...
*
Crystal symmetry In crystallography, crystal structure is a description of ordered arrangement of atoms, ions, or molecules in a crystalline material. Ordered structures occur from intrinsic nature of constituent particles to form symmetric patterns that repeat ...


References

Nonlinear optics Second-harmonic generation {{optics-stub