Electron Energy Loss Spectroscopy ********************************* .. _eels_tools-label: Tools for EELS data analysis ---------------------------- The functions described in this chapter are only available for the :py:class:`~._signals.eels.EELSSpectrum` class. To transform a :py:class:`~.signal.BaseSignal` (or subclass) into a :py:class:`~._signals.eels.EELSSpectrum`: .. code-block:: python >>> s.set_signal_type("EELS") Note these chapter discusses features that are available only for :py:class:`~._signals.eels.EELSSpectrum` class. However, this class inherits many useful feature from its parent class that are documented in previous chapters. 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 requieres this information. The elemental composition of the sample can be declared using :py:meth:`~._signals.eels.EELSSpectrum.add_elements`. The information is stored in the :py:attr:`~.signal.BaseSignal.metadata` attribute (see :ref:`metadata_structure`). This information is saved to file when saving in the hdf5 format. Thickness estimation ^^^^^^^^^^^^^^^^^^^^ The :py:meth:`~._signals.eels.EELSSpectrum.estimate_thickness` can estimate the thickness from a low-loss EELS spectrum using the Log-Ratio method. Zero-loss peak centre and alignment ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ The :py:meth:`~._signals.eels.EELSSpectrum.estimate_zero_loss_peak_centre` 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 approach see :py:meth:`~.signal.Signal1DTools.find_peaks1D_ohaver`. The :py:meth:`~._signals.eels.EELSSpectrum.align_zero_loss_peak` can align the ZLP with subpixel accuracy. It is more robust and easy to use than :py:meth:`~.signal.Signal1DTools.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. Deconvolutions ^^^^^^^^^^^^^^ Three deconvolution methods are currently available: * :py:meth:`~._signals.eels.EELSSpectrum.fourier_log_deconvolution` * :py:meth:`~._signals.eels.EELSSpectrum.fourier_ratio_deconvolution` * :py:meth:`~._signals.eels.EELSSpectrum.richardson_lucy_deconvolution` Estimate elastic scattering intensity ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ The :py:meth:`~._signals.eels.EELSSpectrum.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 :py:meth:`~._signals.eels.EELSSpectrum.estimate_elastic_scattering_threshold` with default values. :py:meth:`~._signals.eels.EELSSpectrum.estimate_elastic_scattering_threshold` 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. .. _eels.kk: Kramers-Kronig Analysis ^^^^^^^^^^^^^^^^^^^^^^^ .. versionadded:: 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. The :py:meth:`~._signals.eels.EELSSpectrum.kramers_kronig_analysis` method inplements the Kramers-Kronig FFT method as in [Egerton2011]_ to estimate the complex dielectric funtion 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 `_. Load the core-loss and low-loss spectra .. code-block:: python >>> s = hs.load("BN_(hex)_B_K_Giovanni_Bertoni_100.msa") >>> ll = hs.load("BN_(hex)_LowLoss_Giovanni_Bertoni_96.msa") Set some important experimental information that is missing from the original core-loss file .. code-block:: python >>> s.set_microscope_parameters(beam_energy=100, convergence_angle=0.2, collection_angle=2.55) .. warning:: `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 .. code-block:: python >>> s.add_elements(('B', 'N')) In order to include the effect of plural scattering we provide the low-loss spectrum to :py:meth:`~._signals.eels.EELSSpectrum.create_model`: .. code-block:: python >>> m = s.create_model(ll=ll) HyperSpy has created the model and configured it automatically: .. code-block:: python >>> m.components # | Attribute Name | Component Name | Component Type ---- | ------------------------- | ------------------------- | ------------------------- 0 | background | background | PowerLaw 1 | N_K | N_K | EELSCLEdge 2 | B_K | B_K | EELSCLEdge .. warning:: Notice that the PowerLaw component has been automatically renamed to "background". This behaviour is deprecated and will be removed in Hyperspy 1.0. From them on this component will keep its original name, "PowerLaw". Furthermore, the components are available in the user namespace .. code-block:: python >>> N_K >>> B_K >>> background .. warning:: This feature is deprecated and will be removed in Hyperspy 1.0. To access the automatically created component use the following equivalent syntax: .. code-block:: python >>> m.components.N_K >>> m.components.B_K >>> m.background Conveniently, variables named as the element symbol contain all the eels core-loss components of the element to facilitate applying some methods to all of them at once. Although in this example the list contains just one component this is not generally the case. .. code-block:: python >>> N [] By default the fine structure features are disabled (although the default value can be configured (see :ref:`configuring-hyperspy-label`). We must enable them to accurately fit this spectrum. .. code-block:: python >>> m.enable_fine_structure() We use smart_fit instead of standard fit method because smart_fit is optimized to fit EELS core-loss spectra .. code-block:: python >>> m.smart_fit() This fit can also be applied over the entire signal to fit a whole spectrum image .. code-block:: python >>> m.multifit(kind='smart') Print the result of the fit .. code-block:: python >>> m.quantify() Absolute quantification: Elem. Intensity B 0.045648 N 0.048061 Visualize the result .. code-block:: python >>> m.plot() .. figure:: images/curve_fitting_BN.png :align: center :width: 500 Curve fitting quantification of a boron nitride EELS core-loss spectrum from `The EELS Data Base `_ There are several methods that are only available in :py:class:`~.models.eelsmodel.EELSModel`: * :py:meth:`~.models.eelsmodel.EELSModel.smart_fit` is a fit method that is more robust than the standard routine when fitting EELS data. * :py:meth:`~.models.eelsmodel.EELSModel.quantify` prints the intensity at the current locations of all the EELS ionisation edges in the model. * :py:meth:`~.models.eelsmodel.EELSModel.remove_fine_structure_data` removes the fine structure spectral data range (as defined by the :py:attr:`~._components.eels_cl_edge.EELSCLEdge.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: * :py:meth:`~.models.eelsmodel.EELSModel.enable_edges` * :py:meth:`~.models.eelsmodel.EELSModel.enable_background` * :py:meth:`~.models.eelsmodel.EELSModel.disable_background` * :py:meth:`~.models.eelsmodel.EELSModel.enable_fine_structure` * :py:meth:`~.models.eelsmodel.EELSModel.disable_fine_structure` The following methods permit to easily enable/disable several ionisation edge functionalities: * :py:meth:`~.models.eelsmodel.EELSModel.set_all_edges_intensities_positive` * :py:meth:`~.models.eelsmodel.EELSModel.unset_all_edges_intensities_positive` * :py:meth:`~.models.eelsmodel.EELSModel.enable_free_onset_energy` * :py:meth:`~.models.eelsmodel.EELSModel.disable_free_onset_energy` * :py:meth:`~.models.eelsmodel.EELSModel.fix_edges` * :py:meth:`~.models.eelsmodel.EELSModel.free_edges` * :py:meth:`~.models.eelsmodel.EELSModel.fix_fine_structure` * :py:meth:`~.models.eelsmodel.EELSModel.free_fine_structure` 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, :py:meth:`~.models.eelsmodel.EELSModel.resolve_fine_structure`, to 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 manually. .. versionadded:: 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 :py:meth:`~.models.eelsmodel.EELSModel.suspend_auto_fine_structure_width`. To resume it use :py:meth:`~.models.eelsmodel.EELSModel.suspend_auto_fine_structure_width`