Polarization density

Electromagnetism
Electrostatics

In classical electromagnetism, polarization density (or electric polarization, or simply polarization) is the vector field that expresses the density of permanent or induced electric dipole moments in a dielectric material. When a dielectric is placed in an external electric field, its molecules gain electric dipole moment and the dielectric is said to be polarized. The electric dipole moment induced per unit volume of the dielectric material is called the electric polarization of the dielectric. Polarization density also describes how a material responds to an applied electric field as well as the way the material changes the electric field, and can be used to calculate the forces that result from those interactions. It can be compared to magnetization, which is the measure of the corresponding response of a material to an magnetic field in magnetism. The SI unit of measure is coulombs per square metre, and polarization density is represented by a vector P.

Contents

Polarization density in Maxwell's equations

The behavior of electric fields (E and D), magnetic fields (B, H), charge density (ρ) and current density (J) are described by Maxwell's equations. The role of the polarization density P is described below.

Relations between E, D and P

The polarization density P defines the electric displacement field D as [1]

\mathbf{D} = \varepsilon_0\mathbf{E} %2B \mathbf{P}

which is convenient for various calculations. Here ε0 is the electric permittivity.

A relation between P and E exists in many materials, as described later in the article.

Bound charge

Electric polarization corresponds to a rearrangement of the bound electrons in the material, which creates an additional charge density, known as the bound charge density ρb:

\rho_b = -\nabla\cdot\mathbf{P}

so that the total charge density that enters Maxwell's equation for the divergence of E is given by

\rho = \rho_f %2B \rho_b \,

where ρf is the free charge density given by the divergence of D.

At the surface of the polarized material, the bound charge appears as a surface charge density

\sigma_b = \mathbf{P}\cdot\mathbf{\hat n}_\mathrm{out} \,

where \mathbf{\hat n}_\mathrm{out}\, is the normal vector. If P is uniform inside the material, this surface charge is the only bound charge.

When the polarization density changes with time, the time-dependent bound-charge density creates a polarization current density of

\mathbf{J}_p = \frac{\partial \mathbf{P}}{\partial t}

so that the total current density that enters Maxwell's equations is given by

\mathbf{J} = \mathbf{J}_f %2B \nabla\times\mathbf{M} %2B \frac{\partial\mathbf{P}}{\partial t}

where Jf is the free-charge current density, and the second term is the magnetization current density (also called the bound current density), a contribution from atomic-scale magnetic dipoles (when they are present).

Relation between P and E in various materials

In a homogeneous linear and isotropic dielectric medium, the polarization is aligned with and proportional to the electric field E:

{\mathbf P}=\varepsilon_0\chi{\mathbf E},

where ε0 is the electric constant, and χ is the electric susceptibility of the medium.

In an anisotropic material, the polarization and the field are not necessarily in the same direction. Then, the ith component of the polarization is related to the jth component of the electric field according to:

P_i = \sum_j \epsilon_0 \chi_{ij} E_j , \,\!

where ε0 is the electric constant, and χij, is the electric susceptibility tensor of the medium. This relation shows, for example, that a material can polarize in the x direction by applying a field in the z direction, and so on. The case of an anisotropic dielectric medium is described by the field of crystal optics.

As in most electromagnetism, this relation deals with macroscopic averages of the fields and dipole density, so that one has a continuum approximation of the dielectric materials that neglects atomic-scale behaviors. The polarizability of individual particles in the medium can be related to the average susceptibility and polarization density by the Clausius-Mossotti relation.

In general, the susceptibility is a function of the frequency ω of the applied field. When the field is an arbitrary function of time t, the polarization is a convolution of the Fourier transform of χ(ω) with the E(t). This reflects the fact that the dipoles in the material cannot respond instantaneously to the applied field, and causality considerations lead to the Kramers–Kronig relations.

If the polarization P is not linearly proportional to the electric field E, the medium is termed nonlinear and is described by the field of nonlinear optics. To a good approximation (for sufficiently weak fields, assuming no permanent dipole moments are present), P is usually given by a Taylor series in E whose coefficients are the nonlinear susceptibilities:

P_i / \epsilon_0 = \sum_j \chi^{(1)}_{ij} E_j %2B \sum_{jk} \chi_{ijk}^{(2)} E_j E_k %2B \sum_{jk\ell} \chi_{ijk\ell}^{(3)} E_j E_k E_\ell %2B \cdots \!

where \chi^{(1)} is the linear susceptibility, \chi^{(2)} is the second-order susceptibility (describing phenomena such as the Pockels effect, optical rectification and second-harmonic generation), and \chi^{(3)} is the third-order susceptibility (describing third-order effects such as the Kerr effect and electric field-induced optical rectification).

In ferroelectric materials, there is no one-to-one correspondence between P and E at all because of hysteresis.

Polarization ambiguity

The polarization inside a solid is not, in general, uniquely defined: It depends on which electrons are paired up with which nuclei.[3] (See figure.) In other words, two people, Alice and Bob, looking at the same solid, may calculate different values of P, and neither of them will be wrong. Alice and Bob will agree on the macroscopic electric field E in the solid, but disagree on the value of the displacement field \mathbf{D}=\varepsilon_0 \mathbf{E}%2B\mathbf{P}. They will both find that Gauss's law is correct (\nabla\cdot\mathbf{D}= \rho_{\text{free}}), but they will disagree on the value of \rho_{\text{free}} at the surfaces of the crystal. For example, if Alice believes the bulk solid to consist of dipoles with positive ions above and negative ions below, but the real crystal has negative ions as the topmost surface, then Alice will say that there is a negative free charge at the topmost surface. (She would categorize this as a type of surface reconstruction).

On the other hand, even though the value of P is not uniquely defined in a bulk solid, gradual changes in P are uniquely defined.[3] If the crystal is gradually changed from one structure to another, there will be a current inside each unit cell, due to the motion of nuclei and electrons. This current results in a macroscopic transfer of charge from one side of the crystal to the other, and therefore it can be measured with an ammeter (like any other current) when wires are attached to the opposite sides of the crystal. The time-integral of the current is proportional to the change in P. The current can be calculated in computer simulations (such as density functional theory); the formula for the integrated current turns out to be a type of Berry's phase.[3]

The non-uniqueness of P is not problematic, because every measurable consequence of P is in fact a consequence of a continuous change in P.[3] For example, when a material is put in an electric field E, which ramps up from zero to a finite value, the material's electronic and ionic positions slightly shift. This changes P, and the result is electric susceptibility (and hence permittivity). As another example, when some crystals are heated, their electronic and ionic positions slightly shift, changing P. The result is pyroelectricity. In all cases, the properties of interest are associated with a change in P.

Even though the polarization is in principle non-unique, in practice it is often (not always) defined by convention in a specific, unique way. For example, in a perfectly centrosymmetric crystal, P is usually defined by convention to be exactly zero. As another example, in a ferroelectric crystal, there is typically a centrosymmetric configuration above the Curie temperature, and P is defined there by convention to be zero. As the crystal is cooled below the Curie temperature, it shifts gradually into a more and more non-centrosymmetric configuration. Since gradual changes in P are uniquely defined, this convention gives a unique value of P for the ferroelectric crystal, even below its Curie temperature.

Lorentzian Model

See also

References and notes

  1. ^ Saleh, B.E.A.; Teich, M.C. (2007). Fundamentals of Photonics. Hoboken, NJ: Wiley. pp. 154. ISBN 9780471358329. 
  2. ^ Based upon equations from Andrew Gray (1888). The theory and practice of absolute measurements in electricity and magnetism. Macmillan & Co.. pp. 126–127. http://books.google.com/?id=jb0KAAAAIAAJ&pg=PA127. , which refers to papers by Sir W. Thomson.
  3. ^ a b c d Resta, Raffaele (1994). "Macroscopic polarization in crystalline dielectrics: the geometric phase approach". Rev. Mod. Phys. 66: 899. doi:10.1103/RevModPhys.66.899. http://inside.mines.edu/~zhiwu/research/papers/E04_berry2.pdf.  See also: D Vanderbilt, Berry phases and Curvatures in Electronic Structure Theory, an introductory-level powerpoint.