Electron Energy Loss Spectroscopy¶
Tools for EELS data analysis¶
The functions described in this chapter are only available for the
EELSSpectrum class. To transform a
BaseSignal (or subclass) into a
Note these chapter discusses features that are available only for
EELSSpectrum class. However, this class inherits
many useful feature from its parent class that are documented in previous
Elemental composition of the sample¶
It can be useful to define the elemental composition of the sample for
archiving purposes or to use some feature (e.g. curve fitting) that requires
this information. The elemental composition of the sample can be declared
information is stored in the
attribute (see Metadata structure). This information is saved to file
when saving in the hspy format (HyperSpy’s HDF5 specification).
estimate the thickness from a low-loss EELS spectrum using the Log-Ratio
Zero-loss peak centre and alignment¶
can be used to estimate the position of the zero-loss peak. The method assumes
that the ZLP is the most intense feature in the spectra. For a more general
align the ZLP with subpixel accuracy. It is more robust and easy to use than
align1D() for the task. Note that it is
possible to apply the same alignment to other spectra using the also_align
argument. This can be useful e.g. to align core-loss spectra acquired
quasi-simultaneously. If there are other features in the low loss signal
which are more intense than the ZLP, the signal_range argument can narrow
down the energy range for searching for the ZLP.
Three deconvolution methods are currently available:
Estimate elastic scattering intensity¶
can be used to calculate the integral of the zero loss peak (elastic intensity)
from EELS low-loss spectra containing the zero loss peak using the
(rudimentary) threshold method. The threshold can be global or spectrum-wise.
If no threshold is provided it is automatically calculated using
with default values.
can be used to calculate separation point between elastic and inelastic
scattering on EELS low-loss spectra. This algorithm calculates the derivative
of the signal and assigns the inflexion point to the first point below a
certain tolerance. This tolerance value can be set using the tol keyword.
Currently, the method uses smoothing to reduce the impact of the noise in the
measure. The number of points used for the smoothing window can be specified by
the npoints keyword.
New in version 0.7.
The single-scattering EEL spectrum is approximately related to the complex
permittivity of the sample and can be estimated by Kramers-Kronig analysis.
method implements the Kramers-Kronig FFT method as in
[Egerton2011] to estimate the complex dielectric function
from a low-loss EELS spectrum. In addition, it can estimate the thickness if
the refractive index is known and approximately correct for surface
plasmon excitations in layers.
EELS curve fitting¶
HyperSpy makes it really easy to quantify EELS core-loss spectra by curve fitting as it is shown in the next example of quantification of a boron nitride EELS spectrum from the The EELS Data Base (see Loading example data and data from online databases).
Load the core-loss and low-loss spectra
>>> s = hs.datasets.eelsdb(title="Hexagonal Boron Nitride", ... spectrum_type="coreloss") >>> ll = hs.datasets.eelsdb(title="Hexagonal Boron Nitride", ... spectrum_type="lowloss")
Set some important experimental information that is missing from the original core-loss file
>>> s.set_microscope_parameters(beam_energy=100, ... convergence_angle=0.2, ... collection_angle=2.55)
convergence_angle and collection_angle are actually semi-angles and are given in mrad. beam_energy is in keV.
Define the chemical composition of the sample
>>> s.add_elements(('B', 'N'))
In order to include the effect of plural scattering, the model is convolved with the loss loss spectrum in which case the low loss spectrum needs to be provided to
>>> m = s.create_model(ll=ll)
HyperSpy has created the model and configured it automatically:
>>> m.components # | Attribute Name | Component Name | Component Type ---- | -------------------- | -------------------- | -------------------- 0 | PowerLaw | PowerLaw | PowerLaw 1 | N_K | N_K | EELSCLEdge 2 | B_K | B_K | EELSCLEdge
Conveniently, all the EELS core-loss components of the added elements are added automatically, names after its element symbol.
By default the fine structure features are disabled (although the default value can be configured (see Configuring HyperSpy). We must enable them to accurately fit this spectrum.
We use smart_fit instead of standard fit method because smart_fit is optimized to fit EELS core-loss spectra
This fit can also be applied over the entire signal to fit a whole spectrum image
Print the result of the fit
>>> m.quantify() Absolute quantification: Elem. Intensity B 0.045648 N 0.048061
Visualize the result
There are several methods that are only available in
smart_fit()is a fit method that is more robust than the standard routine when fitting EELS data.
quantify()prints the intensity at the current locations of all the EELS ionisation edges in the model.
remove_fine_structure_data()removes the fine structure spectral data range (as defined by the
fine_structure_width)ionisation edge components. It is specially useful when fitting without convolving with a zero-loss peak.
The following methods permit to easily enable/disable background and ionisation edges components:
The following methods permit to easily enable/disable several ionisation edge functionalities:
When fitting edges with fine structure enabled it is often desirable that the
fine structure region of nearby ionization edges does not overlap. HyperSpy
provides a method,
automatically adjust the fine structure to prevent fine structure to avoid
overlapping. This method is executed automatically when e.g. components are
added or removed from the model, but sometimes is necessary to call it
New in version 0.7.1: Sometimes it is desirable to disable the automatic adjustment of the fine
structure width. It is possible to suspend this feature by calling
To resume it use