Dielectric function tools¶

The DielectricFunction class inherits from ComplexSignal and can thus access complex properties. To convert a ComplexSignal to a DielectricFunction, make sure that the signal dimension and signal type are properly set:

>>> s.set_signal_type('DielectricFunction')

Note that DielectricFunction is complex and therefore is a subclass of ComplexSignal1D.

Number of effective electrons¶

The Bethe f-sum rule gives rise to two definitions of the effective number (see [Egerton2011]):

$n_{\mathrm{eff1}}\left(-\Im\left(\epsilon^{-1}\right)\right)=\frac{2\epsilon_{0}m_{0}}{\pi\hbar^{2}e^{2}n_{a}}\int_{0}^{E}E'\Im\left(\frac{-1}{\epsilon}\right)dE' n_{\mathrm{eff2}}\left(\epsilon_{2}\right)=\frac{2\epsilon_{0}m_{0}}{\pi\hbar^{2}e^{2}n_{a}}\int_{0}^{E}E'\epsilon_{2}\left(E'\right)dE'$

where $n_a$ is the number of atoms (or molecules) per unit volume of the sample, $\epsilon_0$ is the vacuum permittivity, $m_0$ is the electron mass and $e$ is the electron charge.

The get_number_of_effective_electrons() method computes both.

Compute the electron energy-loss signal¶

The get_electron_energy_loss_spectrum() “naively” computes the single-scattering electron-energy loss spectrum from the dielectric function given the zero-loss peak (or its integral) and the sample thickness using:

$S\left(E\right)=\frac{2I_{0}t}{\pi a_{0}m_{0}v^{2}}\ln\left[1+\left(\frac{\beta}{\theta(E)}\right)^{2}\right]\Im\left[\frac{-1}{\epsilon\left(E\right)}\right]$

where $I_0$ is the zero-loss peak integral, $t$ the sample thickness, $\beta$ the collection semi-angle and $\theta(E)$ the characteristic scattering angle.