Kerr effect

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This page is about the Kerr nonlinear optical effect. For the magneto-optic phenomenon of the same name, see magneto-optic Kerr effect.

The Kerr effect or the quadratic electro-optic effect (QEO effect) is a change in the refractive index of a material in response to an electric field. It is distinct from the Pockels effect in that the induced index change is directly proportional to the square of the electric field instead of to the magnitude of the field. All materials show a Kerr effect, but certain liquids display the effect more strongly than other materials do. The Kerr effect was discovered in 1875 by John Kerr, a Scottish physicist.

Two special cases of the Kerr effect are normally considered: the Kerr electro-optic effect, or DC Kerr effect, and the optical Kerr effect, or AC Kerr effect.

1 Kerr electro-optic effect
2 Optical Kerr effect
3 Theory
- 3.1 DC Kerr effect
- 3.2 AC Kerr effect
4 See also
5 External links

[edit] Kerr electro-optic effect

The Kerr electro-optic effect, or DC Kerr effect, is the special case in which the electric field is a slowly varying external field applied by, for instance, a voltage on electrodes across the material. Under the influence of the applied field, the material becomes birefringent, with different indexes of refraction for light polarized parallel to or perpendicular to the applied field. The difference in index of refraction, Δn, is given by

$\Delta n = \lambda K E^2\ ,$

where λ is the wavelength of the light, K is the Kerr constant, and E is the amplitude of the electric field. This difference in index of refraction causes the material to act like a waveplate when light is incident on it in a direction perpendicular to the electric field. If the material is placed between two "crossed" (perpendicular) linear polarizers, no light will be transmitted when the electric field is turned off, while nearly all of the light will be transmitted for some optimum value of the electric field. Higher values of the Kerr constant allow complete transmission to be achieved with a smaller applied electric field.

Some polar liquids, such as nitrotoluene (C₇H₇NO₂) and nitrobenzene (C₆H₅NO₂) exhibit very large Kerr constants. A glass cell filled with one of these liquids is called a Kerr cell. These are frequently used to modulate light, since the Kerr effect responds very quickly to changes in electric field. Light can be modulated with these devices at frequencies as high as 10 GHz. Because the Kerr effect is relatively weak, a typical Kerr cell may require voltages as high as 30 kV to achieve complete transparency. This is in contrast to Pockels cells, which can operate at much lower voltages. Another disadvantage of Kerr cells is that the best available material, nitrobenzene, is both poisonous and explosive. Some transparent crystals have also been used for Kerr modulation, although they have smaller Kerr constants.

[edit] Optical Kerr effect

The optical Kerr effect, or AC Kerr effect is the case in which the electric field is due to the light itself. This causes a variation in index of refraction which is proportional to the local irradiance of the light. This refractive index variation is responsible for the nonlinear optical effects of self focusing and self-phase modulation, and is the basis for Kerr-lens modelocking. This effect only becomes significant with very intense beams such as those from lasers.

[edit] Theory

[edit] DC Kerr effect

For a nonlinear material, the electric polarization field P will depend on the electric field E:

$\mathbf{P} = \varepsilon_0 \chi^{(1)} : \mathbf{E} + \varepsilon_0 \chi^{(2)} : \mathbf{E E} + \varepsilon_0 \chi^{(3)} : \mathbf{E E E} + \dots$

where ε₀ is the vacuum permittivity and χ⁽ⁿ⁾ is the n-th order component of the electric susceptibility of the medium. The ":" symbol represents the scalar product between matrices. We can write that relationship explicitly; the i-th component for the vector P can be expressed as:

$P_i = \varepsilon_0 \sum_{j=1}^{3} \chi^{(1)}_{i j} E_j + \varepsilon_0 \sum_{j=1}^{3} \sum_{k=1}^{3} \chi^{(2)}_{i j k} E_j E_k + \varepsilon_0 \sum_{j=1}^{3} \sum_{k=1}^{3} \sum_{l=1}^{3} \chi^{(3)}_{i j k l} E_j E_k E_l + \dots$

where $i = 1,2,3$ . It is often assumed that $P 1 = P x$ , i.e. the component parallel to x of the polarization field; $E 2 = E y$ and so on.

For a linear medium, only the first term of this equation is significant and the polarization varies linearly with the electric field.

For materials exhibiting a non-negligible Kerr effect, the third, χ⁽³⁾ term is significant, with the even-order terms typically dropping out due to inversion symmetry of the Kerr medium. Consider the net electric field E produced by a light wave of frequency ω together with an external electric field E₀:

$\mathbf{E} = \mathbf{E}_0 + \mathbf{E}_\omega \cos(\omega t),$

where E_ω is the vector amplitude of the wave.

Combining these two equations produces a complex expression for P. For the DC Kerr effect, we can neglect all except the linear terms and those in $\chi^{(3)}|\mathbf{E}_0|^2 \mathbf{E}_\omega$ :

$\mathbf{P} \simeq \varepsilon_0 \left( \chi^{(1)} + 3 \chi^{(3)} |\mathbf{E}_0|^2 \right) \mathbf{E}_\omega \cos(\omega t),$

which is similar to the linear relationship between polarization and an electric field of a wave, with an additional non-linear susceptibility term proportional to the square of the amplitude of the external field.

For non-symmetric media (e.g. liquids), this induced change of susceptibility produces a change in refractive index in the direction of the electric field:

$\Delta n = \lambda_0 K |\mathbf{E}_0|^2,$

where λ₀ is the vacuum wavelength and K is the Kerr constant for the medium. The applied field induces birefringence in the medium in the direction of the field. A Kerr cell with a transverse field can thus act as a switchable wave plate, rotating the plane of polarization of a wave travelling through it. In combination with polarizers, it can be used as a shutter or modulator.

The values of K depend on the medium and are about 9.4×10^-14 m V^-2 for water, and 4.4×10^-12 m V^-2 for nitrobenzene.

For crystals, the susceptibility of the medium will in general be a tensor, and the Kerr effect produces a modification of this tensor.

[edit] AC Kerr effect

In the optical or AC Kerr effect, an intense beam of light in a medium can itself provide the modulating electric field, without the need for an external field to be applied. In this case, the electric field is given by:

$\mathbf{E} = \mathbf{E}_\omega \cos(\omega t),$

where E_ω is the amplitude of the wave as before.

Combining this with the equation for the polarization, and taking only linear terms and those in χ⁽³⁾|E_ω|³:

$\mathbf{P} \simeq \varepsilon_0 \left( \chi^{(1)} + \frac{3}{4} \chi^{(3)} |\mathbf{E}_\omega|^2 \right) \mathbf{E}_\omega \cos(\omega t).$

As before, this looks like a linear susceptibility with an additional non-linear term:

$\chi = \chi_{\mathrm{LIN}} + \chi_{\mathrm{NL}} = \chi^{(1)} + \frac{3\chi^{(3)}}{4} |\mathbf{E}_\omega|^2,$

and since:

$n = (1 + \chi)^{1/2} = \left( 1+\chi_{\mathrm{LIN}} + \chi_{\mathrm{NL}} \right)^{1/2} \simeq n_0 \left( 1 + \frac{1}{2 {n_0}^2} \chi_{\mathrm{NL}} \right)$

where n₀=(1+χ_LIN)^1/2 is the linear refractive index. Using a Taylor expansion since χ_NL << n₀², this give an intensity dependent refractive index (IDRI) of:

$n = n_0 + \frac{3\chi^{(3)}}{8 n_0} |\mathbf{E}_{\omega}|^2 = n_0 + n_2 I$

where n₂ is the second-order nonlinear refractive index, and I is the intensity of the wave. The refractive index change is thus proportional to the intensity of the light travelling through the medium.

The values of n₂ are relatively small for most materials, on the order of 10^-20 m² W^-1 for typical glasses. Therefore beam intensities (irradiances) on the order of 1 GW cm^-2 (such as those produced by lasers) are necessary to produce significant variations in refractive index via the AC Kerr effect.

The optical Kerr effect manifests itself temporally as self-phase modulation, a self-induced phase- and frequency-shift of a pulse of light as it travels through a medium. This process, along with dispersion, can produce optical solitons.

Spatially, an intense beam of light in a medium will produce a change in the medium's refractive index that mimics the transverse intensity pattern of the beam. For example, a Gaussian beam results in a Gaussian refractive index profile, similar to that of a gradient-index lens. This causes the beam to focus itself, a phenomenon known as self-focusing.

This article contains material from the Federal Standard 1037C, which, as a work of the United States Government, is in the public domain.