Miller's rule (optics) explained

In optics, Miller's rule is an empirical rule which gives an estimate of the order of magnitude of the nonlinear coefficient.[1]

More formally, it states that the coefficient of the second order electric susceptibility response (

\chi2

) is proportional to the product of the first-order susceptibilities (

\chi1

) at the three frequencies which

\chi2

is dependent upon.[2] The proportionality coefficient is known as Miller's coefficient

\delta

.

Definition

The first order susceptibility response is given by:\chi_1(\omega) = \frac \frac

where:

\omega

is the frequency of oscillation of the electric field;

\chi1

is the first order electric susceptibility, as a function of

\omega

;

\varepsilon0

is the electric permittivity of free space;

\tau

is the free carrier relaxation time;

For simplicity, we can define

D(\omega)

, and hence rewrite

\chi1

:D(\omega) = \omega_0^2 - \omega^2 - \tfrac \chi_1(\omega) = \frac \frac

The second order susceptibility response is given by:\chi_2(2\omega) = \frac \frac where

\zeta2

is the first anharmonicity coefficient.It is easy to show that we can thus express

\chi2

in terms of a product of

\chi1

\chi_2(2\omega) = \frac \chi_1(\omega) \chi_1(\omega) \chi_1(2\omega)

The constant of proportionality between

\chi2

and the product of

\chi1

at three different frequencies is Miller's coefficient: \delta = \frac

Notes and References

  1. Miller . R. C. . Optical second harmonic generation in piezoelectric crystals . Applied Physics Letters . 5 . 1 . 17–19 . 1964 . 10.1063/1.1754022 .
  2. Book: Boyd , Robert . Nonlinear Optics . Academic Press . 2008 . 978-0123694706 .