Unsupervised machine learning applied to scanning precession electron diffraction data

Scanning precession electron diffraction involves the acquisition of a two-dimensional precession electron diffraction pattern at every probe position in a two-dimensional scan. The data typically comprise many more diffraction patterns than the number of distinct microstructural volume elements (e.g. crystals) in the region sampled. A dimensionality reduction, ideally to one representative diffraction pattern per distinct element, may then be sought. Further, some diffraction patterns will contain contributions from multiple crystals sampled along the beam path, which may be unmixed by harnessing this oversampling. Here, we report on the application of unsupervised machine learning methods to achieve both dimensionality reduction and signal unmixing. Potential artefacts are discussed and precession electron diffraction is demonstrated to improve results by reducing the impact of bending and dynamical diffraction so that the data better approximate the case in which each crystal yields a given diffraction pattern.

Scanning transmission electron microscopy (STEM) investigations increasingly combine the measurement of multiple analytical signals as a function of probe position with post-facto computational analysis [1]. In a scan, the number of local signal measurements is usually much greater than the number of significantly distinct microstructural elements and this redundancy may be harnessed during analysis, for example by averaging signals over like regions to improve signal to noise. Unsupervised machine learning techniques automatically exploit data redundancy to find patterns with minimal prior constraints [2]. In analytical electron microscopy, such methods have been applied to learn representative signals corresponding to separate microstructural elements (e.g. crystal phases) and to unmix signals comprising contributions from multiple microstructural elements sampled along the beam path [3,4,5,6,7,8,9,10]. These studies have primarily applied linear matrix decompositions such as independent component analysis (ICA) and non-negative matrix factorisation (NMF).

Scanning precession electron diffraction (SPED) enables nanoscale investigation of local crystallography [11, 12] by recording electron diffraction patterns as the electron beam is scanned across the sample with a step size on the order of nanometres. The incorporation of double conical rocking of the beam, also known as precession [13], achieves integration through a reciprocal space volume for each reflection. Precession has been found to convey a number of advantages for interpretation and analysis of the resultant diffraction patterns, in particular the suppression of intensity variation due to dynamical scattering [14,15,16]. The resultant four-dimensional dataset, comprising two real and two reciprocal dimensions (4D-SPED), can be analysed in numerous ways. For example, the intensity of a sub-set of pixels in each diffraction pattern can be integrated (or summed) as a function of probe position, to form so-called virtual bright field (VBF) or virtual dark field (VDF) images [17, 18]. VBF/VDF analysis has been used to provide insight into local crystallographic variations such as phase [17], strain [19] and orientation [20]. In another approach, the collected diffraction patterns are compared against a library of precomputed templates, providing a visualisation of the microstructure and orientation information, a process known as template or pattern matching [11]. These analyses do not utilise the aforementioned redundancy present in data and may require significant effort on the part of the researcher. Here, we explore the application of unsupervised machine learning methods to achieve dimensionality reduction and signal unmixing.

Materials

GaAs (cubic, F43m) nanowires containing type I twin (\(\Sigma 3\)) [21] boundaries were taken as a model system for this work. The long axis of these nanowires is approximately parallel to the [111] crystallographic direction as a result of growth by molecular beam epitaxy [22] on (111). In cross section, these nanowires have an approximately hexagonal geometry with a vertex-to-vertex distance of 120–150 nm. Viewed near to the \([1{\overline{1}}0]\) zone axis, the twin boundary normal is approximately perpendicular to the incident beam direction.

SPED experiments

Scanning precession electron diffraction was performed on a Philips CM300 FEGTEM operating at 300 kV with the scan and simultaneous double rocking of the electron beam controlled using a NanoMegas Digistar external scan generator. A convergent probe with convergence semi-angle of \(\sim 1.5\hbox { mrad}\) and precession angles of 0, 9 and 35 mrad was used to perform scans with a step size of 10 nm using the ASTAR software package. The resolution was thus dominated by the step size. PED patterns were recorded using a Stingray CCD camera to capture the image on the fluorescent binocular viewing screen.

It is generally inappropriate to manipulate raw data before applying multivariate methods such as decomposition or clustering, which cannot be considered objective if subjective prior alterations have been made. In this work, the only data manipulation applied before machine learning is to align the central beams of each diffraction pattern. Geometric distortions introduced from the angle between the camera and the viewing screen were corrected by applying an opposite distortion to the data after the application of machine learning methods.

Multislice simulations

A twinned bi-crystal model was constructed with the normal to the [111] twin boundary inclined at an angle of \(55 ^{\circ }\) to the incident beam direction so that the two crystals overlapped in projection. In this geometry, both crystals are oriented close to \(\langle 511\rangle\) zone axes with coherent matching of the \(\{0{\bar{6}}6\}\) and \(\{2{\bar{8}}2\}\) planes in these zones. Three precession angles were simulated using the TurboSlice package [23]: 0, 10 and 20 mrad, with 200 distinct azimuthal positions about the optic axis to ensure appropriate integration in the resultant simulated patterns [24]. The crystal model used in the simulation comprised 9 unique layers each 0.404 nm thick. 15 layers were used leading to a total thickness of 54.6 nm. These \(512\times 512\)-pixel patterns with 16-bit dynamic range were convolved with a 4-pixel Gaussian kernel to approximate a point spread function.

Linear matrix decomposition

Latent linear models describe data by the linear combination of latent variables that are learned from the data rather than measured—more pragmatically, the repeated features in the data can be well approximated using a small number of basis vectors. With appropriate constraints, the basis vectors may be interpreted as physical signals. To achieve this, a data matrix, \(\mathbf X\), can be approximated as the matrix product of a matrix of basis vectors \(\mathbf W\) (components), and corresponding coefficients \(\mathbf Z\) (loadings). The error in the approximation, or reconstruction error, may be expressed as an objective function to be minimised in a least squares scheme:

where \(||\mathbf A ||_{\mathrm {F}}\) is the Frobenius norm^{Footnote 1} of matrix \(\mathbf A\). More complex objective functions, for example incorporating sparsity promoting weighting factors [25], may be defined. We note that the decomposition is not necessarily performed by directly computing this error minimisation.

Three linear decompositions were used here: singular value decomposition (SVD) [2, 26], independent component analysis (ICA) [27], and non-negative matrix factorisation (NMF) [25, 28]. These decompositions were used as implemented in HyperSpy [29], which itself draws on the algorithms implemented in the open-source package scikit-learn [30].

The singular value decomposition is closely related to the better-known principal component analysis, in which the vectors comprising \(\mathbf W\) are orthonormal. The optimal solution to rank L is then obtained when \(\mathbf W\) is estimated by eigenvectors (principal components) corresponding to the L largest eigenvalues of the empirical covariance matrix^{Footnote 2}. The optimal low-dimensional representation of the data is given by \(\mathbf z _{i} = \mathbf W ^{T}{} \mathbf x _{i}\), which is an orthogonal projection of the data on to the corresponding subspace and maximises the statistical variance of the projected data. This optimal reconstruction may be obtained via truncated SVD of the data matrix—the factors for PCA and SVD are equivalent, though the loadings may differ by independent scaling factors [31].

Unmixing measured signals to determine source signals a priori is known as blind source separation (BSS) [32]. SVD typically yields components that do not correspond well with the original sources due to its orthogonality constraint. ICA solves this problem by maximising the independence of the components, instead of the variance, and is applied to data previously projected by SVD using the widespread FastICA algorithm [27]. NMF [25, 28] may also be used for BSS and imposes \(\mathbf W \ge \mathbf 0 , \mathbf Z \ge \mathbf 0\). To impose these constraints, the algorithm computes a coordinate descent numerical minimisation of Eq. 1. Such an approach does not guarantee convergence to a global minimum and the results are sensitive to initialisation. The implementation used here initialises the optimisation using a non-negative double singular value decomposition (NNDSVD), which is based on two SVD processes, one approximating the data matrix, the other approximating positive sections of the resulting partial SVD factors [33]. This algorithm gives a well-defined non-negative starting point suitable for obtaining a sparse factorisation. Finally, the product \(\mathbf WZ\) is invariant under the transformation \(\mathbf W \rightarrow\) \(\mathbf W \varvec{\lambda }\), \(\mathbf Z \rightarrow\) \(\varvec{\lambda }^{-1}{} \mathbf Z\), where \(\varvec{\lambda }\) is a diagonal matrix. This fact is used to scale the loadings to a maximum value of 1.

Data clustering

Clustering points in space may be achieved using numerous methods. One of the best known is k-means, in which the positions of several cluster prototypes (centroids) are iteratively updated according to the mean of the nearest data points [34]. The clusters thus found are considered to be “hard”—each datum can only belong to a single cluster. Here, we apply fuzzy c-means [35] clustering, which has the significant advantage that data points may be members of multiple clusters allowing for an interpretation based on mixing of multiple cluster centres. For example, a measured diffraction pattern that is an equal mixture of the two basis patterns lies precisely between the two cluster centres and will have a membership of 0.5 to each. We also employ the Gustafson–Kessel variation for c-means, which allows the clusters to adopt elliptical, rather than spherical, shapes [36].

Cluster analysis in spaces of dimension greater than about 10 is unreliable [37, 38] as with increasing dimension “long” distances become less distinct from “short”. The relevant dimension of the collected diffraction patterns is the size of the image, on the order of \(10^4\). A dimensionality reduction is, therefore, performed first, using SVD, and clustering is applied in the space of loading coefficients [34]. The cluster centres found in this low-dimensional space can be re-projected into the data space of diffraction patterns to produce a result equivalent to a weighted mean of the measured patterns within the cluster. The spatial occurrence of each basis pattern may then be visualised by plotting the membership values associated with each cluster as a function of probe position to form a membership map.

SPED data were acquired with precession angles of 0, 9 and 35 mrad from a GaAs nanowire oriented near to a \([1{\overline{1}}0]\) zone axis such that the twin boundary normal was approximately perpendicular to the incident beam direction, as shown in Fig. 1. The bending of this nanowire is evident in the data acquired without precession (Fig. 1a) as at position iii the diffraction pattern is near the zone axis, whereas at position i a Laue circle is clearly visible. The radius of this Laue circle is \(\sim 24\hbox { mrad}\), which provides an estimate of the bending angle across the field of view. When a precession angle of 35 mrad (i.e. larger than the bending angle) was used, all measured patterns appear close to zone axis (Fig. 1b) due to the reciprocal space integration resulting from the double conical rocking geometry. The effect of this integration is also seen in the contrast of the virtual dark-field image, which shows numerous bend contours without precession and less complex variation in intensity with precession. We surmise that precession leads to the data better approximating the situation where there is a single diffraction pattern associated with each microstructural element, which here is essentially the two twinned crystal orientations and the vacuum surrounding the sample. The region of interest also contains a small portion of carbon support film, which is just visible in the virtual dark-field images as a small variation in intensity. The position of the carbon film has been indicated in the figure.

SPED data from a GaAs nanowire and virtual dark-field images formed by plotting the intensity within the disks marked around \(\lbrace 111\rbrace\) reflections, as a function of probe position. a Without precession and b with 35 mrad precession. Diffraction pattern and VDF image scale bars are common to all subfigures and measure 1 Å\(^{-1}\) and 150 nm respectively. The approximate position of the carbon film is indicated by the red dashed line

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Using SVD, we can produce a scree plot showing the fraction of total variance in the data explained by each principal component pattern. Figure 2a shows the scree plot for the 0, 9 and 35 mrad data. A regime change, from relatively high variance components to relatively low variance components, may be identified [2, 39] after 3 components for the data acquired with 35 mrad precession, after 4 components with 9 mrad precession, and cannot clearly be identified without precession. While there is a small change in the line after 4 components in the curve for data recorded without precession, the variance described by the components on either side of this is relatively similar, particularly given the ordinate is on a log scale. This demonstrates that the use of precession reduces the number of components required to describe the data, consistent with the intuitive understanding of the effect of reciprocal space integration achieved using precession. The 4th component, significant in the 9 mrad data, arises because the top and bottom of the nanowire are sufficiently differently oriented, as a result of bending, to be distinguished by the algorithm. We, therefore, continue our analysis focusing attention on data acquired with relatively large precession angles.

SVD and ICA analysis of SPED data from a GaAs nanowire. a Scree plot of variance explained by each SVD component for 0, 9 and 35 mrad data. b First 3 SVD components for 35 mrad data. c ICA components for 35 mrad data. Intensities in red indicate positive values and those in blue indicate negative values. Pattern and loading scale bars are common to all subfigures and measure 1 Å\(^{-1}\) and 150 nm respectively

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Component patterns and corresponding loading maps obtained by SVD and ICA analysis of 35 mrad SPED data are shown in Fig. 2b, c, respectively. In either analysis, each feature clearly describes some significant variation in the diffraction peak intensities, although it is worth noting that SVD requires two components to describe the two twins in the wire where ICA needs only one. Both descriptions of the data are mathematically sensible and physical insight can be obtained from the differences between diffraction patterns that are highlighted by negative values in the SVD and ICA component patterns, but neither method produces patterns that can be directly associated with crystal structure. To make use of more conventional diffraction pattern analysis, we seek decomposition constraints that yield learned components which more closely resemble physical diffraction patterns. To this end, we apply NMF and fuzzy clustering.

The data were decomposed to three component patterns using NMF, of which, by inspection, one corresponded to the background and two corresponded to the two twinned crystal orientations—the latter shown in Fig. 3a, b. The choice of three components was guided by the intrinsic dimensionality indicated by the SVD analysis and it was further verified that a plot of the NMF reconstruction error (Eq. 1) as a function of increasing number of components showed a similar regime change to the SVD scree plot (see “Availability of data and materials” section at the end of the main text). In the NMF component patterns, white spots are visible, representing intensity lower than background level. We describe these as a pseudo-subtractive contribution of intensity from those locations.

NMF and fuzzy clustering of SPED data from a GaAs nanowire. a, b NMF factors and corresponding loading maps. c Two-dimensional projection of 3 component SVD loadings onto the plane of the second and third loading with cluster membership as contours. d, e Weighted average cluster centre patterns. Pattern and loading scale bars are common to all subfigures and measure 1 Å\(^{-1}\) and 150 nm respectively

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In Fig. 3c, SVD loadings for the scan data are shown as a scatter plot, where the axes correspond to the SVD factors. Because the SVD and PCA factors are equivalent, this projection represents the maximum possible variation in the data, and so the maximum discrimination. The loadings associated with each measured pattern are approximately distributed about a triangle in this space. Fuzzy clustering was applied to three SVD components, and the learned memberships are overlaid as contours. Three clusters describe the distribution of the loadings well, and the cluster centres correspond to the background and the twinned crystals as shown in Fig. 3d, e. Both the NMF factors and c-means centers represent the same orientations, but the pseudo-subtractive artefacts in the NMF factors are not present in the cluster centers.

The scatter plot in Fig. 3c also shows that two of the clusters comprise two smaller subclusters. Membership maps for these subclusters reveal that the splitting is due to the underlying carbon film with the subcluster nearer to the background cluster in each case corresponding to the region where the film is present. In the membership maps, there are bright lines along the boundaries between the nanowire and the vacuum, due to overlap between clusters.

The unmixing of diffraction signals from overlapping crystals was investigated. SPED data with a precession angle of 18 mrad were acquired from a nanowire tilted away from the \([1{\overline{1}}0]\) zone axis by \(\sim 30 ^{\circ }\), such that two microstructural elements overlapped in projection. The overlap of the two crystals was assessed using virtual dark-field imaging, NMF loading maps, and fuzzy clustering membership maps (Fig. 4). The region in which the crystals overlap can be identified by all these methods. The VDF result can be considered a reference and is obtained with minimal processing but requires manual specification of appropriate diffracting conditions for image formation. The NMF and fuzzy clustering approaches are semi-automatic. There is good agreement between the VDF images and NMF loading maps. The boundary appears slightly narrower in the clustering membership map. The NMF loading corresponding to the background component decreases along the profile, which may be related to the underlying carbon film, whilst the cluster membership for the background contains a spurious peak in the overlap region. Finally, the direct beam intensity is much lower in the NMF component patterns than in the true source signals. Our results indicate that either machine learning method is superior to conventional linear decomposition for the analysis of SPED datasets, but some unintuitive and potentially misleading features are present in the learning results.

SPED data from a GaAs nanowire with a twin boundary at an oblique angle to the beam. a Virtual dark-field images formed, using a virtual aperture 4 pixels in diameter, from the circled diffraction spots. b NMF decomposition results. c Clustering results. For b and c the profiles are taken from the line scans indicated, and the blue profile represents the intensity of the background component. Pattern and loading scale bars are common to all subfigures and measure 1 Å\(^{-1}\) and 70 nm respectively

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Unsupervised learning methods (SVD, ICA, NMF, and fuzzy clustering) have been explored here in application to SPED data as applied to materials where the region of interest comprises a finite number of significantly different microstructrual elements, i.e. crystals of particular phase and/or orientation. In this case, NMF and clustering may yield a small number of component patterns and weighted average cluster centres that resemble physical electron diffraction patterns. These methods are, therefore, effective for both dimensionality reduction and signal unmixing although we note that neither approach is well suited to situations where there are continuous changes in crystal structure. By contrast, SVD and ICA provide effective means of dimensionality reduction but the components are not readily interpreted using analogous methods to conventional electron diffraction analysis, owing to the presence of many negative values. The SVD and ICA results do nevertheless tend to highlight physically important differences in the diffraction signal across the region of interest. The massive data reduction from many thousands of measured diffraction patterns to a handful of learned component patterns is very useful, as is the unmixing achieved. Artefacts in the learning results were however identified, particularly when applied to achieve signal unmixing, and these are explored further here.

To illustrate artefacts resulting from learning methods, model SPED datasets were constructed based on line scans across inclined boundaries in hypothetical bicrystals. Models (Figs. 5 and 6) were designed to highlight features of two-dimensional diffraction-like signals rather than to reflect the physics of diffraction. These were, therefore, constructed with the strength of the signal directly proportional to thickness of the hypothetical crystal at each point, with no noise, and Gaussian peak profiles.

Construction and decomposition of an idealised model SPED dataset system comprising non-overlapping two-dimensional signals. a Schematic representation of hypothetical bi-crystal. b Ground truth end-member patterns and relative thickness of the two crystals. c Factors and loadings obtained by 2-component NMF. d Cluster centre average patterns and membership maps obtained by fuzzy clustering

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Non-independent components. a Expected result for an artificial dataset with two ‘phases’ with overlapping peaks. b NMF decomposition. c Cluster results. d SVD loadings of the dataset, used for clustering. Each point corresponds to a diffraction pattern in the scan—several are indicated with the dotted lines. Contours indicate the value of membership to the two clusters—refer to “Methods” section “Data clustering”

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The model SPED dataset shown in Fig. 5 comprises the linear summation of two square arrays of Gaussians (to emulate diffraction patterns) with no overlap between the two patterns. NMF decomposition exactly recovers the signal profile in this simple case. In contrast, the membership profile obtained by fuzzy clustering, which varies smoothly owing to the use of a Euclidean distance metric, does not match the source signal. The boundary region instead appears qualitatively narrower than the true boundary. Further, the membership value for each of the pure phases is slightly below 100% because the cluster centre is a weighted average position that will only correspond to the end member if there are many more measurements near to it than away from it. A related effect is that the membership value rises at the edge of the boundary region where mixed patterns are closer to the weighted centre than the end members. We conclude that clustering should be used only if the data comprises a significant amount of unmixed signal. In the extreme, cluster analysis cannot separate the contribution from a microstructural feature which has no pure signal in the scan, for example a fully embedded particle. These observations are consistent with the results reported in association with Fig. 4.

A common challenge for signal separation arises when the source signals contain coincident peaks from distinct microstructural elements, as would be the case in SPED data when crystallographic orientation relationships exist between crystals. A model SPED dataset corresponding to this case was constructed and decomposed using NMF and fuzzy clustering (Fig. 6). In this case, the NMF decomposition yields a factor containing all the common reflections and a factor containing the reflections unique to only one end member. Whilst this is interpretable, it is not physical, although it should be noted that this is an extreme example where there is no unique information in one of the source patterns. Nevertheless, it should be expected that the intensity of shared peaks is likely to be unreliable in the learned factors and this was the case for the direct beam in learned component patterns shown in Fig. 4. As a result, components learned through NMF should not be analysed quantitatively^{Footnote 3}. The weighted average cluster centres resemble the true end members much more closely than the NMF components. The pure phases have a membership of around 99%, rather than 100%, due to the cluster centre being offset from the pure cluster by the mixed data, as shown in Fig. 6d. The observation that memberships extend across all the data (albeit sometimes with vanishingly small values) explains the rise in intensity of the background component in Fig. 4c in the interface region. Such interface regions do not evenly split their membership between their two true constituent clusters, meaning that some membership is attributed to the third cluster, causing a small increase in the membership locally. These issues may potentially be addressed using extensions to the algorithm developed by Rousseeuw et al. [41] or using alternative geometric decompositions such as vertex component analysis [42].

Precession was found empirically to improve machine learning decomposition as discussed above (Fig. 2), so long as the precession angle is large enough. This was attributed primarily to integration through bending of the nanowire. Precession may also result in a more monotonic variation of diffracted intensity with thickness [15] as a result of integration through the Bragg condition. It was, therefore, suggested that precession may improve the approximation that signals from two overlapping crystals may be considered to be combined linearly. To explore this, a multislice simulation of a line scan across a bi-crystal was performed and decomposed using both NMF and fuzzy clustering (Fig. 7). Without precession, both the NMF loadings and the cluster memberships do not increase monotonically with thickness but rather vary significantly in a manner reminiscent of diffracted intensity modulation with thickness due to dynamical scattering. Both the loading profile and the membership profile reach subsidiary minima when the corresponding component is just thicker than half the thickness of the simulation, which corresponds to a thickness of approximately 100 nm and is consistent with the \(2{\bar{2}}0\) extinction length for GaAs of 114 nm. This suggests that the decomposition of the diffraction patterns is highly influenced by a few strong reflections; hence, the variation of the \(2{\bar{2}}0\) reflections with thickness is overwhelming the other structural information encoded in the patterns. The removal of this effect, an essential function of applying precession, is seen: with 10 or 20 mrad precession this intensity modulation is suppressed and the loading or membership maps obtained show a monotonic increase across the inclined boundary. The cluster centres again show intensity corresponding to the opposite end member due to the weighted averaging. Precession is, therefore, beneficial for the application of unsupervised learning algorithms both in reducing signal variations arising from bending, which is a common artefact of specimen preparation, and reducing the impact of dynamical effects on signal mixing.

Unsupervised learning applied to SPED data simulated using dynamical multislice calculations a Original data with a 20 mrad precession angle. b NMF decomposition, in which the loadings have been re-scaled as in Fig. 5. The factors show pseudo-subtractive features, typical of NMF. c Cluster analysis. The high proportion of data points from the boundary means there is information shared between the cluster centres. Without precession, neither method can reproduce the original data structure

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Noise and background are both significant in determining the performance of unsupervised learning algorithms. Extensive exploration of these parameters is beyond the scope of this work but we note that the various direct electron detectors that have recently been developed and that are likely to play a significant role in future SPED studies have very different noise properties. Therefore, understanding the optimal noise performance for unsupervised learning may become an important consideration. We also note that the pseudo-subtractive features evident in the NMF decomposition results of Fig. 3 may become more significant in this case and the robustness of fuzzy clustering to this may prove advantageous.

Unsupervised machine learning methods, particularly non-negative matrix factorisation and fuzzy clustering, have been demonstrated here to be capable of learning the significant microstructural features within SPED data. NMF may be considered a true linear unmixing whereas fuzzy clustering, when applied to learn representative patterns, is essentially an automated way of performing a weighted averaging with the weighting learned from the data. The former can struggle to separate coincident signals (including signal shared with a background or noise) whereas the latter implicitly leaves some mixing when a large fraction of measurements are mixed. In both cases, precession electron diffraction patterns are more amenable to unsupervised learning than the static beam equivalents. This is due to the integration through the Bragg condition, resulting from rocking the beam, causing diffracted beam intensities to vary more monotonically with thickness and the integration through small orientation changes due to out of plane bending. This work has, therefore, demonstrated that unsupervised machine learning methods, when applied to SPED data, are capable of reducing the data to the most salient structural features and unmixing signals. The scope for machine learning to reveal nanoscale crystallography will expand rapidly in the coming years with the application of more advanced methods.

1. 1.

   The Frobenius norm is defined as \(||\mathbf A ||_{\mathrm {F}} = \sqrt{\sum \limits _{i=1}^{m} \sum \limits _{j=1}^{n} a_{ij}^{2}}\)

2. 2.

   The empirical covariance matrix, \(\Sigma = \frac{1}{N}\sum _{i=1}^{N} \mathbf x _{i}{} \mathbf x _{i}^{T}\)

3. 3.

   This problem may be mitigated by enforcing a sum-to-one constraint on the loadings learned through NMF during optimisation. See for example [40].

BSS:

blind source separation

FEGTEM:

field-emission gun transmission electron microscope

ICA:

independent component analysis

NNDSVD:

non-negative double singular value decomposition

NMF:

non-negative matrix factorisation

PED:

precession electron diffraction

PCA:

principal component analysis

SPED:

scanning precession electron diffraction

STEM:

scanning transmission electron microscopy

SVD:

singular value decomposition

VBF:

virtual bright field

VDF:

virtual dark field

BHM, DNJ, ASE, and PAM proposed the investigation. DNJ, ASE, and ATJvH performed the SPED experiments, ASE provided the multislice simulations, and BHM implemented the c-means algorithm. The data analysis was undertaken by BHM and DNJ who also prepared the manuscript, with oversight and critical contributions from ASE, ATJvH, and PAM. All authors read and approved the final manuscript.

Acknowlegements

Prof. Weman and Fimland of IES at NTNU are acknowledged for supplying the nanowire samples.

Competing interests

The authors declare that they have no competing interests.

Availability of data and materials

Data used in this work has been made freely available to download at https://doi.org/10.17863/CAM.26432.

The Python 3 code to perform the analysis has also been made available, at https://doi.org/10.17863/CAM.26444.

Funding

The authors acknowledge financial support from: The Royal Society (Grant RG140453; UF130286); the Seventh Framework Programme of the European Commission: ESTEEM2, contract number 312483; the European Research Council under the European Union’s Seventh Framework Programme (FP7/2007-2013)/ERC grant agreement 291522-3DIMAGE; the University of Cambridge and the Cambridge NanoDTC; the EPSRC (Grant no. EP/R008779/1).

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Affiliations

1. Department of Materials Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge, CB3 0FS, UK
   • Ben H. Martineau
   • , Duncan N. Johnstone
   •  & Paul A. Midgley
2. The School of Materials, The University of Manchester, Oxford Road, Manchester, M13 9PL, UK
   • Alexander S. Eggeman
3. Department of Physics, Norwegian University of Science and Technology, Hogskolering 5, 7491, Trondheim, Norway
   • Antonius T. J. van Helvoort

Corresponding author

Correspondence to Ben H. Martineau.

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