Electric susceptibility explained

In electricity (electromagnetism), the electric susceptibility (

\chi _{e} ; Latin: susceptibilis "receptive") is a dimensionless proportionality constant that indicates the degree of polarization of a dielectric material in response to an applied electric field. The greater the electric susceptibility, the greater the ability of a material to polarize in response to the field, and thereby reduce the total electric field inside the material (and store energy). It is in this way that the electric susceptibility influences the electric permittivity of the material and thus influences many other phenomena in that medium, from the capacitance of capacitors to the speed of light.^{[1] [2]}

Definition for linear dielectrics

If a dielectric material is a linear dielectric, then electric susceptibility is defined as the constant of proportionality (which may be a tensor) relating an electric field E to the induced dielectric polarization density P such that^{[3] [4]} $$\backslash mathbf\; P\; =\backslash varepsilon\_0\; \backslash chi\_,$$where

P is the polarization density;\varepsilon _{0} is the electric permittivity of free space (electric constant);\chi _{e} is the electric susceptibility;E is the electric field.

In materials where susceptibility is anisotropic (different depending on direction), susceptibility is represented as a tensor known as the susceptibility tensor. Many linear dielectrics are isotropic, but it is possible nevertheless for a material to display behavior that is both linear and anisotropic, or for a material to be non-linear but isotropic. Anisotropic but linear susceptibility is common in many crystals.^[3]

The susceptibility is related to its relative permittivity (dielectric constant)

\varepsilon _{rm{r} } by$$\backslash chi\_\backslash \; =\; \backslash varepsilon\_\; -\; 1$$so in the case of a vacuum,$$\backslash chi\_\backslash \; =\; 0.$$

At the same time, the electric displacement D is related to the polarization density P by the following relation:^[3] $$\backslash mathbf\; \backslash \; =\; \backslash \; \backslash varepsilon\_0\backslash mathbf\; +\; \backslash mathbf\; \backslash \; =\; \backslash \; \backslash varepsilon\_0\; (1+\backslash chi\_)\; \backslash mathbf\; \backslash \; =\; \backslash \; \backslash varepsilon\_\; \backslash varepsilon\_0\; \backslash mathbf\; \backslash \; =\; \backslash \; \backslash varepsilon\backslash mathbf$$where

\varepsilon = \varepsilon _{r} \varepsilon _{0} \varepsilon _{r} = 1+ \chi _{e}

Molecular polarizability

See main article: Polarizability. A similar parameter exists to relate the magnitude of the induced dipole moment p of an individual molecule to the local electric field E that induced the dipole. This parameter is the molecular polarizability (α), and the dipole moment resulting from the local electric field E_local is given by:$$\backslash mathbf\; =\; \backslash varepsilon\_0\backslash alpha\; \backslash mathbf$$

This introduces a complication however, as locally the field can differ significantly from the overall applied field. We have:$$\backslash mathbf\; =\; N\; \backslash mathbf\; =\; N\; \backslash varepsilon\_0\; \backslash alpha\; \backslash mathbf\_\backslash text,$$where P is the polarization per unit volume, and N is the number of molecules per unit volume contributing to the polarization. Thus, if the local electric field is parallel to the ambient electric field, we have:$$\backslash chi\_\; \backslash mathbf\; =\; N\; \backslash alpha\; \backslash mathbf\_$$

Thus only if the local field equals the ambient field can we write:$$\backslash chi\_\; =\; N\; \backslash alpha.$$

Otherwise, one should find a relation between the local and the macroscopic field. In some materials, the Clausius–Mossotti relation holds and reads$$\backslash frac\; =\; \backslash frac.$$

Ambiguity in the definition

The definition of the molecular polarizability depends on the author. In the above definition,$$\backslash mathbf=\backslash varepsilon\_0\backslash alpha\; \backslash mathbf,$$

p and E are in SI units and the molecular polarizability \alpha has the dimension of a volume (m³). Another definition^[5] would be to keep SI units and to integrate \varepsilon _{0} into \alpha :

$$\backslash mathbf=\backslash alpha\; \backslash mathbf.$$

In this second definition, the polarizability would have the SI unit of C.m²/V. Yet another definition exists^[5] where

p and E are expressed in the cgs system and \alpha is still defined as$$\backslash mathbf=\backslash alpha\; \backslash mathbf.$$

Using the cgs units gives

\alpha the dimension of a volume, as in the first definition, but with a value that is 4 \pi lower.

Nonlinear susceptibility

In many materials the polarizability starts to saturate at high values of electric field. This saturation can be modelled by a nonlinear susceptibility. These susceptibilities are important in nonlinear optics and lead to effects such as second-harmonic generation (such as used to convert infrared light into visible light, in green laser pointers).

The standard definition of nonlinear susceptibilities in SI units is via a Taylor expansion of the polarization's reaction to electric field:^[6] $$P\; =\; P\_0\; +\; \backslash varepsilon\_0\; \backslash chi^\; E\; +\; \backslash varepsilon\_0\; \backslash chi^\; E^2\; +\; \backslash varepsilon\_0\; \backslash chi^\; E^3\; +\; \backslash cdots.$$(Except in ferroelectric materials, the built-in polarization is zero,

P _{0} = 0 .)The first susceptibility term, \chi ^{(1)} , corresponds to the linear susceptibility described above. While this first term is dimensionless, the subsequent nonlinear susceptibilities \chi ^{(n)} have units of .

The nonlinear susceptibilities can be generalized to anisotropic materials in which the susceptibility is not uniform in every direction. In these materials, each susceptibility

\chi ^{(n)} becomes an -degree tensor.

Dispersion and causality

In general, a material cannot polarize instantaneously in response to an applied field, and so the more general formulation as a function of time is$$\backslash mathbf(t)\; =\; \backslash varepsilon\_0\; \backslash int\_^t\; \backslash chi\_(t-t\text{'})\; \backslash mathbf(t\text{'})\backslash ,\; \backslash mathrm\; dt\text{'}.$$

That is, the polarization is a convolution of the electric field at previous times with time-dependent susceptibility given by

\chi _{e} (\Delta t) . The upper limit of this integral can be extended to infinity as well if one defines \chi _{e} (\Delta t) = 0 for \Delta t < 0 . An instantaneous response corresponds to Dirac delta function susceptibility \chi _{e} (\Delta t) = \chi _{e} \delta(\Delta t) .

It is more convenient in a linear system to take the Fourier transform and write this relationship as a function of frequency. Due to the convolution theorem, the integral becomes a product,$$\backslash mathbf(\backslash omega)\; =\; \backslash varepsilon\_0\; \backslash chi\_(\backslash omega)\; \backslash mathbf(\backslash omega).$$

This has a similar form to the Clausius–Mossotti relation:$$\backslash mathbf(\backslash mathbf)\; =\; \backslash varepsilon\_0\backslash frac\backslash mathbf(\backslash mathbf)\; =\; \backslash varepsilon\_0\backslash chi\_\backslash text(\backslash mathbf)\backslash mathbf(\backslash mathbf)$$

This frequency dependence of the susceptibility leads to frequency dependence of the permittivity. The shape of the susceptibility with respect to frequency characterizes the dispersion properties of the material.

Moreover, the fact that the polarization can only depend on the electric field at previous times (i.e.

\chi _{e} (\Delta t) = 0 for \Delta t < 0 ), a consequence of causality, imposes Kramers–Kronig constraints on the susceptibility \chi _{e} ( 0 ) .

See also

• Application of tensor theory in physics
• Magnetic susceptibility
• Maxwell's equations
• Clausius–Mossotti relation
• Linear response function
• Green–Kubo relations

Notes and References

1. Encyclopedia: Electric susceptibility . Encyclopædia Britannica.
2. Book: Cardarelli , François . Materials Handbook: A Concise Desktop Reference . . 2nd . 2000–2008 . London . 524 (Section 8.1.16) . 10.1007/978-1-84628-669-8 . 978-1-84628-668-1 .
3. Book: Griffiths . David J . Introduction to Electrodynamics . 2017 . Cambridge University Press . 181–190 . 4.
4. Book: Freeman. Richard. Essentials of Electricity and Magnetism. 2019. Electromagnetic Radiation. Oxford University Press. 10.1093/oso/9780198726500.003.0001. 978-0-19-872650-0. King. James. Lafyatis. Gregory.
5. Book: CRC Handbook of Chemistry and Physics. CRC. 10–163. 84. 2016-08-19. https://web.archive.org/web/20161006104503/http://www.znu.ac.ir/data/members/rasoulifard_mohammad/crc.pdf. 2016-10-06 . dead.
6. Book: 10.1017/CBO9781139167994. The Elements of Nonlinear Optics. 1990. Butcher. Paul N.. Cotter. David. 9781139167994. Cambridge University Press.