The classical electron radius, also known as the Compton radius or the Thomson scattering length is based on a classical (i.e., non-quantum) relativistic model of the electron. Its value is calculated as

$r\_\backslash mathrm\{e\}=\backslash frac\{1\}\{4\backslash pi\backslash epsilon\_0\}\backslash frac\{e^2\}\{mc^2\}\; =\; 2.817940325(28)\backslash times\; 10^\{-15\}\; \backslash mathrm\{m\}$

where e and m are the electric charge and the mass of the electron, c is the speed of light, and ε₀ is the permittivity of free space. Using classical electrostatics, the amount of energy required to assemble a sphere of constant charge density, of radius r_e and charge e is approximately

$E=\backslash frac\{1\}\{4\backslash pi\backslash epsilon\_0\}\backslash frac\{e^2\}\{r\_\backslash mathrm\{e\}\}$.

If this is equated to the relativistic energy of the electron (E = mc²) and solved for r_e, the above result is obtained.

In simple terms, the classical electron radius is roughly the size the electron would need to have for its mass to be completely due to its electrostatic potential energy - not taking quantum mechanics into account. We now know that quantum mechanics, indeed quantum field theory, is needed to understand the behavior of electrons at such short distance scales, thus the classical electron radius is no longer regarded as the actual size of an electron. In fact, modern particle physics experiments indicate that the electron is a point particle, i.e. it has no size and its radius is zero. Still, the classical electron radius is used in modern classical-limit theories involving the electron, such as non-relativistic Thomson scattering. Also, the classical electron radius is roughly the length scale at which renormalization becomes important in quantum electrodynamics.

The classical electron radius is one of a trio of related units of length, the other two being the Bohr radius $a\_0$ and the Compton wavelength of the electron $\backslash lambda\_e$. The classical electron radius is built from the electron mass $m\_e$, the speed of light $c$ and the electron charge $e$. The Bohr radius is built from $m\_e$, $e$ and Planck's constant $h$. The Compton wavelength is built from $m\_e$, $h$ and $c$. Any one of these three lengths can be written in terms of any other using the fine structure constant $\backslash alpha$:

$r\_e\; =\; \{\backslash alpha\; \backslash lambda\_e\; \backslash over\; 2\backslash pi\}\; =\; \backslash alpha^2\; a\_0$

Extrapolating from the initial equation, any mass $m\_0$ can be imagined to have an 'electromagnetic radius' similar to the electron's classical radius.

$r=\backslash frac\{k\_\{C\}e^2\}\{m\_0\; c^2\}=\backslash frac\{\backslash alpha\backslash hbar\}\{m\_0\; c\}$

where $k\_C$ is Coulomb's constant, $\backslash alpha$ is the fine structure constant and $\backslash hbar$ is Planck's constant. Such a radius does not exist as a physical entity but it is sometimes useful in theoretical calculations.

References

• CODATA value for the classical electron radius at NIST.
• Arthur N. Cox, Ed. "Allen's Astrophysical Quantities", 4th Ed, Springer, 1999.

External links

• Length Scales in Physics: the Classical Electron Radius

Physical constants | Atomic physics

Klassischer Elektronenradius