Crystal optics

Crystal optics is the branch of optics that describes the behaviour of light in anisotropic media, that is, media (such as crystals) in which light behaves differently depending on which direction the light is propagating. Crystals are often naturally anisotropic, and in some media (such as liquid crystals it is possible to induce anisotropy by applying e.g. an external electric field.

Typical transparent media such as glasses are isotropic, which means that light behaves the same way no matter which direction it is travelling in the medium. In terms of Maxwell's equations in a dielectric, this gives a relationship between the electric displacement field[?] D and the electric field E:

D = ε₀E + P ,

where ε₀ is the permittivity of free space and P is the electric polarisation (the vector field corresponding to electric dipole moments present in the medium). Physically, the polarisation field can be regarded as the response of the medium to the electric field of the light.

In an isotropic and linear medium, this polarisation field P is proportional to and parallel to the electric field E:

P = ε₀χE ,

where χ is the electric susceptibility[?] of the medium. The relation between D and E is thus:

D = ε₀E + ε₀χE = ε₀(1+χ)E .

The value (1+χ) is called the relative permittivity of the medium, and is related to the refractive index n:

n = (1+χ)^1/2 = (ε_r)^1/2 .

In an anisotropic medium, such as a crystal, the polarisation field P is not necessarily aligned with the electric field of the light E. In a physical picture, this can be thought of as the dipoles induced in the medium by the electric field having certain prefered directions, related to the physical structure of the crystal. This can be written as:

P = ε₀ χ×E .

Here χ is not a number as before but a tensor of rank 2, the electric susceptibility tensor. In terms of components in 3 dimensions:

<math>\begin{pmatrix} P_x \\ P_y \\ P_z \end{pmatrix} = \epsilon_0 \begin{pmatrix} \chi_{xx} & \chi_{xy} & \chi_{xz} \\ \chi_{yx} & \chi_{yy} & \chi_{yz} \\ \chi_{zx} & \chi_{zy} & \chi_{zz} \end{pmatrix} \begin{pmatrix} E_x \\ E_y \\ E_z \end{pmatrix} </math>

or using the summation convention:

P_i = ε₀ χ_ij E_j .

Since χ is a tensor, P is not necessarily colinear with E.

From thermodynamics arguments it can be shown that χ_ij = χ_ji, i.e. the χ tensor is symmetric. In accordance with the spectral theorem, it is thus possible to diagonalise the tensor by choosing the appropriate set of cooridinate axes, zeroing all components of the tensor except χ_xx, χ_yy and χ_zz. This gives the set of relations:

P_x = ε₀ χ_xx E_x

P_y = ε₀ χ_yy E_y

P_z = ε₀ χ_zz E_z

The directions x, y and z are in this case known as the principal axes of the medium.

It follows that D and E are also related by a tensor:

D = ε₀E + P = ε₀E + ε₀ χ×E = ε₀ (1+χ)×E = ε₀ ε×E .

Here ε is know as the relative permittivity tensor or dielectric tensor. Consequently, the refractive index of the medium must also be a tensor. Consider a light wave propagating along the z principal axis polarised such the electric field of the wave is parallel to the x-axis. The wave experiences a susceptability χ_xx and a permittivity ε_xx. The refractive index is thus:

n_xx = (1 + χ_xx)^1/2 = (ε_xx)^1/2 .

For a wave polarised in the y direction:

n_yy = (1 + χ_yy)^1/2 = (ε_yy)^1/2 .

Thus these waves will see two different refractive indices and travel at different speeds. This phenomenon is known as birefringence and occurs in some common crystals such as calcite and quartz.

If χ_xx = χ_yy ≠ χ_zz, the crystal is known as uniaxial. If χ_xx ≠ χ_yy and χ_xx ≠ χ_zz the crystal is called biaxial. A uniaxial crystal exhibits two refractive indicies, an "ordinary" index (n_o) for light polarised in the x or y directions, and an "extraordinary" index (n_e) for polarisation in the z direction. Light polarised at some angle to the axes will experience a different phase velocity for different polarization components, and cannot be described by a single index of refraction. This is often depicted as an index ellipsoid[?].

Certain nonlinear optical phenomena such as the electro-optic effect cause a variation of a medium's permittivity tensor when an external electric field is applied, proportional (to lowest order) to the strength of the field. This causes a rotation of the principal axes of the medium and alters the behaviour of light travelling through it; the effect can be used to produce light modulators.

In response to a magnetic field, some materials can have a dielectric tensor that is complex-Hermitian; this is called a gyro-magnetic or magneto-optic effect. In this case, the principle axes are complex-valued vectors, corresponding to elliptically polarized light, and time-reversal symmetry can be broken. This can be used to design optical isolators, for example.

(A dielectric tensor that is not Hermitian gives rise to complex eigenvalues, which corresponds to a material with gain or absorption at a particular frequency.)