# Exact analytical expression for the synchrotron radiation spectrum in the Gaussian turbulent magnetic field

## TL;DR

This paper derives an exact analytical formula for the synchrotron radiation spectrum in Gaussian turbulent magnetic fields and explores its implications for different electron energy distributions.

## Contribution

It provides the first exact analytical expression for synchrotron spectra in turbulent fields and extends it to approximate spectra with high-energy cut-offs.

## Key findings

- Exact spectrum formula for isotropic mono-energetic electrons in Gaussian turbulence
- Derived approximate spectra for power-law electron distributions with high-energy cut-offs
- Calculated coefficient functions for power-law distributions without cut-offs

## Abstract

We demonstrate that the exact solution for the spectrum of synchrotron radiation from an isotropic population of mono-energetic electrons in turbulent magnetic field with Gaussian distribution of local field strengths can be expressed in the simple analytic form: $\left( \frac{{\rm d} \dot{N}}{{\rm d} \omega} \right)_t = \frac{\alpha}{3} \frac{1}{\gamma^2} \left( 1 + \frac{1}{x^{2/3}} \right) \exp \left( - 2 x^{2/3} \right)$, where $x = \frac{\omega}{\omega_0}\, ; \omega_0 = \frac{4}{3} \gamma^2 \frac{eB_0}{m_e c}\, .$ We use this expression to find approximate synchrotron spectra for power-law electron distributions with $\propto \exp\left( -\left[ \gamma/\gamma_0 \right]^\beta\right)$ type high-energy cut-off; the resulting synchrotron spectrum has the exponential cut-off factor with frequency raised to $2\beta/(3\beta+4)$ power in the exponent. For the power-law electron distribution without high-energy cut-off, we find the coefficient $a_m$ as a function of the power-law index, which results in exact expression for the synchrotron spectrum when using monochromatic (i.e., each electron radiates at frequency $\omega_m = a_m \gamma^2 \, \frac{e B_0}{m_e c}$) approximation.