# Electron energy loss spectrum of silver

Electron energy loss spectroscopy (EELS) is a widely used method to obtain the excitation spectrum of materials. For metallic and semiconducting materials, the energy losses in the range 0-50 eV is primarily due excitations of plasmons, that are collective electronic excitations, corresponding to oscillations in the electron density. For a free-electron metal (Drude metal), the plasmon energy is given by the electron density, n:

In GPAW, the EELS can be calculated with the dielectric response module, where it is obtained from the macroscopic dielectric function:

where q is the momentum transfer. (Se the tutorial Linear dielectric response of an extended system for a detailed description of the dielectric response.)

Here we will calculate the EELS for bulk silver, where band-structure effects (coupling to inter-band transitions) are seen to have a big impact on the plasmon resonance, which means that the Drude description for the plasmon energy given above is not expected to hold. First restart the ground state calculation with the LDA functional, calculated in the bandstructure exercise Band structure and converge a larger number of bands:

```
import matplotlib.pyplot as plt
import numpy as np
from gpaw import GPAW
from gpaw.response.df import DielectricFunction
calc = GPAW('Ag_LDA.gpw', parallel={'domain': 1})
calc.diagonalize_full_hamiltonian(nbands=30)
calc.write('Ag_LDA_full.gpw', 'all')
```

Then we can set up the dielectric function, taking the ground state as input:

```
df = DielectricFunction(
calc='Ag_LDA_full.gpw', # Ground state input
frequencies={'type': 'nonlinear',
'domega0': 0.05}) # energy grid spacing at omega=0
```

The EELS spectrum is calculated with the
`get_eels_spectrum()`

method, that
takes the momentum transfer q as a parameter. This parameter is restricted to
be the difference between two k-points from the ground state calculation.
Let’s choose the smallest q possible: If you used \(N\times N\times N\)
k-points then that will be `[1.0 / N, 0, 0]`

:

```
q_c = [1.0 / 10, 0, 0]
df.get_eels_spectrum(q_c=q_c) # a file called 'eels.csv' is generated
```

The calculation (see `eels.py`

) takes some time due to a sum over
k-points. To speed up the calculation, run it in parallel:

```
$ mpiexec -np 4 gpaw python silver_EELS.py
```

The calculation saves the file `eels.csv`

by default, where the first
column is the energy grid, and the second and third columns are the loss
spectrum without and with local field corrections respectively. (The local
field corrections takes into account that the system responds on the
microscopic scale though the perturbation is macroscopic). You can plot the
spectrum by like this:

```
data = np.loadtxt('eels.csv', delimiter=',')
omega = data[:, 0]
eels = data[:, 2]
plt.plot(omega, eels)
plt.xlabel('Energy (eV)')
plt.ylabel('Loss spectrum')
plt.xlim(0, 20)
plt.show()
```

Look at the spectrum, where is the plasmon peak? Compare the result to the experimental plasmon energy \(\omega_P \approx 3.9 \mathrm{eV}\). Also compare the result to the Drude value for the plasmon frequency given above. (Hint: For silver there is one valence s electron pr. atom, use this to calculate the free-electron density.)

Hopefully you will find that there is large difference between the free electron and the quantum result. The plasmon is damped and shifted down in energy due to coupling to single-particle transitions (inter-band transitions). Here the d-band of silver plays a crucial role, since transitions from here up to the Fermi level defines the onset of inter-band transitions. For example you can calculate the loss spectrum from the LDA ground state result and see what is does to the spectrum. You can also investigate the single-particle spectrum by calculating the dielectric function:

```
df.get_dielectric_function(q_c=q_c),
```

which saves a file `df.csv`

(see
`get_dielectric_function()`

). Try
plotting the imaginary part (column 5 in the data file), which corresponds to
the single-particle spectrum. Compare this to the loss spectrum to see that
the plasmon peak is shifted down just below the single-particle transitions.