Deep Consensus, a deep learning-based approach for particle pruning in cryo-electron microscopy.

Single-particle cryo-electron microscopy (cryo-EM) has recently become a mainstream technique for the structural determination of macromolecules. Typical cryo-EM workflows collect hundreds of thousands of single-particle projections from thousands of micrographs using particle-picking algorithms. However, the number of false positives selected by these algorithms is large, so that a number of different 'cleaning steps' are necessary to decrease the false-positive ratio. Most commonly employed techniques for the pruning of false-positive particles are time-consuming and require user intervention. In order to overcome these limitations, a deep learning-based algorithm named Deep Consensus is presented in this work. Deep Consensus works by computing a smart consensus over the output of different particle-picking algorithms, resulting in a set of particles with a lower false-positive ratio than the initial set obtained by the pickers. Deep Consensus is based on a deep convolutional neural network that is trained on a semi-automatically generated data set. The performance of Deep Consensus has been assessed on two well known experimental data sets, virtually eliminating user intervention for pruning, and enhances the reproducibility and objectivity of the whole process while achieving precision and recall figures above 90%.

Introduction

The advent of direct electron detectors, together with the development of novel image-processing algorithms, have brought about a revolution in the field of single-particle analysis (SPA) in cryo-electron microscopy (cryo-EM; Nogales, 2016 ▸). As a result, SPA cryo-EM has been used to determine the structures of a wide range of protein complexes at near-atomic resolution (Bartesaghi et al., 2015 ▸; Merk et al., 2016 ▸; Banerjee et al., 2016 ▸) and is now regarded as a very promising tool for computer-aided drug design (Rawson et al., 2017 ▸).

In order to reconstruct the three-dimensional structure of a macromolecular complex employing SPA cryo-EM, tens of thousands of high-quality single-particle projections of the complex, generally termed particles, are required. These particles are picked from the micrographs, which generally suffer from a low signal-to-noise ratio, contamination and several other artifacts. These problems, along with the huge number of particles that need to be picked, make manual selection a tedious, time-consuming and potentially error-prone step, thus demanding substantial time and user intervention in most cases. On the contrary, automatic particle-picking algorithms (Adiga et al., 2005 ▸; Sorzano et al., 2009 ▸; Voss et al., 2009 ▸; Abrishami et al., 2013 ▸; Scheres, 2015 ▸; Wang et al., 2016 ▸) are well suited for high-throughput workflows, being able to quickly collect thousands of particles with decent performance. Nevertheless, the set of false-positive particles that are selected by these automatic methods is non-negligible, typically ranging from 10% to more than 25% (Zhu et al., 2004 ▸). As a consequence, it is common practice in the field to perform several pruning steps (Razi et al., 2017 ▸; Aramayo et al., 2018 ▸) in which a combination of algorithmic approaches such as particle sorting (Vargas et al., 2013 ▸) or two-dimensional classification (de la Rosa-Trevín et al., 2013 ▸; Scheres, 2012 ▸; Kimanius et al., 2016 ▸; Yang et al., 2012 ▸) are employed together with manual intervention in order to rule out false-positive particles.

One such approximation is MAPPOS (Norousi et al., 2013 ▸). In order to use MAPPOS, a training set of true particles and false particles needs to be provided by the user. The particles are then described by a set of seven features such as phase symmetry or dark dot dispersion. Finally, a bagging classifier of different types of algorithms, including decision trees and k-nearest neighbors, is employed to predict which already picked particles are good and which are false positives. Although this methodology showed promising results, it has not been commonly adopted, probably because the task of manually picking several hundred of particles, although doable, is regarded as a time-consuming task and thus other approaches are used instead. Moreover, the features that are employed to describe particles can suffer from various shortcomings (Vargas et al., 2013 ▸), limiting its applicability.

Recently, there has been a major breakthrough in machine learning with the development of deep learning (LeCun et al., 2015 ▸; Krizhevsky et al., 2012 ▸). Deep-learning approaches have shown outstanding performances in many different tasks such as image recognition, natural language processing and language translation, outperforming not only classical machine-learning algorithms but also humans in some tasks (He et al., 2015 ▸). The main difference of deep learning with respect to classical machine-learning approaches is its ability to learn directly from raw data, which makes the labor-intensive design of handcrafted features unnecessary (LeCun et al., 2015 ▸). Some of the most popular deep-learning models are convolutional neural networks (CNNs), which are the state-of-the-art in artificial vision (http://www.image-net.org/challenges/LSVRC). CNNs are multilayered feed-forward neural networks which are fed directly with input images. A typical CNN has two types of layers: convolutional and fully connected layers. Convolutional layers consist of convolution and pooling steps in tandem. The convolution kernels are automatically learned from training data and the pooling steps perform a down-sampling of the convolution outputs. Finally, the fully connected layers are classical neural network layers, the very last one of which produces an output that measures, in a classification problem, the probability of the input belonging to a given class.

Following this line of investigation, in this work we present Deep Consensus (DC), a deep learning-based approach for the problem of particle pruning. Our method employs a deep CNN designed to classify which of the already picked particles are true particles and which are false positives. In this development, we pursued three main objectives: to rule out false particles, while retaining most of the good particles, to perform this efficiently and, finally, to reduce manual supervision to very low levels. In order to train our CNN, a data set of true and false particles needs to be elaborated. Although this could be compiled manually, here we propose a semi-automatic approach for the generation of such a training set. This latter procedure is based on the fact that different particle-picking algorithms work on different principles, so that the particles that they select may be substantially different. This consideration would naturally suggest the exploration of meta classifiers; this is performed in this work while everything is simultaneously posed in a deep-learning framework. Instead of considering particles selected by just one single picker, we propose considering all particles selected by any of the picking algorithms as candidates and letting the CNN automatically decide which particles are good independently of the algorithm that picked them. DC was evaluated using two well known data sets, EMPIAR-10028 (ribosome; Wong et al., 2014 ▸) and EMPIAR-10061 (β-galactosidase; Bartesaghi et al., 2015 ▸), achieving precision and recall figures above 90%. The DC method is publicly available through the Scipion (de la Rosa-Trevín et al., 2016 ▸) and Xmipp 3 (de la Rosa-Trevín et al., 2013 ▸) cryo-EM frameworks.

Methods

Algorithm

The DC method takes the particles picked by several algorithms as input and produces a new set of high-quality particles as output. To this end, DC employs a CNN trained on a set of positive and negative particles collected from the outputs of several particle pickers (see Fig. 1 ▸). Specifically, the intersection of several sets of particles is defined as the set of particles with common coordinates in each set and is used as a positive training set, termed the AND set (see Section 2.3 for further details). Any particle contained in the AND set has been picked by all of the pickers and, as a consequence, the number of false positives included in this set is expected to be smaller than in any of the single-particle sets. However, the expected low false-positive rate of the AND set comes at the cost of reducing the number of selected particles. Similarly, the union of particles, termed the OR set, is defined by the union of particles that have been picked by any of the methods. This set will contain many false positives but also most of the true, and thus useful, particles. The negative particles (termed the NEG set) used for training are picked at random coordinates, ensuring that there is no particle of the OR set that is close to the randomly picked particle. Additionally, as randomly picked particles tend to overrepresent empty or uncentered particles, a set of negative particles comprised of ice, carbon and other undesired types of contamination can be manually included in the NEG set (see Section 2.3 for further details). Finally, once the CNN has been trained using the AND and NEG sets, the particles of the OR set are evaluated and a score ranging from 0 to 1 is assigned to each particle. In the absence of any a priori information, especially if the user wants to run DC in a fully automated manner, particles with scores of greater than or equal to 0.5 will be classified as true positives, whereas particles with scores below 0.5 will be classified as false positives and thus removed from the final set. At this point, it is worth noting that better thresholds can be manually chosen after visual inspection of the final ranking.

Figure 1

Deep Consensus workflow. Deep Consensus takes the coordinates proposed by different particle pickers as input, from which the intersection (AND set) and the union (OR set) of these coordinates are computed. Next, it picks random coordinates providing that they do not overlap with the OR set (NEG set). The NEG and AND sets are then used to train a convolutional neural network (CNN) that will finally classify the coordinates of the OR set (which is the largest set) as positive particle coordinates or negative particle coordinates.

It is important to note that even after the careful automatic construction of the training sets described above, it is a fact that nothing is perfect and that there will be errors in the positive and negative training sets (the AND and NEG sets, respectively). Fortunately, it is well known that deep-learning approaches tend to be very robust to label noise (Rolnick et al., 2017 ▸; Zhang et al., 2017 ▸; Jindal et al., 2016 ▸). As a consequence, our CNN is indeed able to learn useful information from the AND and NEG sets, and the resulting pruned set is more accurate than any of the original input sets proposed by the particle pickers (see Appendix C ). Moreover, as the number of putative particles (the OR set) is also larger than the individual sets obtained from each picker, a larger number of positive particles can also be recovered while still maintaining low false-positive particle levels, which results in substantial gains in speed and reproducibility with respect to workflows that do not use DC (see Section 3.2).

Deep convolutional neural network

The core component of Deep Consensus is its CNN. CNNs are very popular deep-learning models that have shown outstanding performance in many artificial vision problems. For a brief introduction to neural networks and CNNs, see Appendix A .

The architecture of our deep CNN, which we derived after a thoughtful cross-validation process, is summarized in Table 1 ▸. Our model, implemented using Keras 2.1.5 (https://github.com/keras-team/keras) and TensorFlow 1.4 (Abadi et al., 2016 ▸), consists of four blocks of two convolutional layers followed by a batch normalization (Ren et al., 2017 ▸) and a pooling (down-sampling) layer. The output of the last convolutional block is fed into a single fully connected layer. Finally, a SoftMax layer is employed to obtain the probability of an input being either a good particle or a bad particle. Regularization is performed using a dropout with p = 0.5 after the fully connected layer, and L2 weight regularization was applied to each layer with strength 1 × 10−5. All layers were initialized using the default mechanisms included in Keras.

Table 1

The deep convolutional neural network architecture employed in Deep Consensus

Layer No.	Layer type	Kernel size/step size	Shape
1	Input	—/—	128 × 128 × 1
2	Conv2D + relu	15/1	128 × 128 × 8
3	Conv2D + batch normalization + relu	15/1	128 × 128 × 8
4	MaxPooling2D	7/2	64 × 64 × 8
5	Conv2D + relu	7/1	64 × 64 × 8
6	Conv2D + batch normalization + relu	7/1	64 × 64 × 16
7	MaxPooling2D	5/2	32 × 32 × 16
8	Conv2D + relu	3/1	32 × 32 × 32
9	Conv2D + batch normalization + relu	3/1	32 × 32 × 32
10	MaxPooling2D	3/2	16 × 16 × 32
11	Conv2D + relu	3/1	16 × 16 × 64
12	Conv2D + batch normalization + relu	3/1	16 × 16 × 64
13	AveragePooling2D	4/2	8 × 8 × 64
14	FullyConnected + relu + dropout (p = 0.5)	512/—	512
15	SoftMax	512/—	2

Network training is performed using the Adam optimizer (Kingma & Ba, 2014 ▸) and cross entropy as a loss function with default parameters and an initial learning rate of 1 × 10−4 until convergence is detected. A validation set is drawn from the training set, collecting a random sample of 10% of the set. When the validation accuracy does not improve for 300 steps (batches), the learning rate is divided by ten. Data augmentation is performed using random flips and rotations over the training set at a 1:1 ratio.

Training-set collection: consensus of coordinates and random picking

Given several sets of coordinates picked by different particle pickers, Deep Consensus (DC) firstly computes the intersection and the union of these sets of coordinates (the AND and OR sets, respectively). The OR set is composed of all of the coordinates picked by any picker. The AND set is obtained considering the Euclidean distances between each coordinate of the first set and all of the coordinates of the second set; if the distance between a particular particle is smaller than the 10% of the particle size, the average co­ordinate is added to the AND set. When more than two sets of coordinates are used, the previous strategy is repeated considering the coordinates of the AND set and the coordinates of the third set, then the fourth set, and so on.

The set of negative particles used for training (the NEG set) is collected from randomly picked coordinates. As some of these coordinates may correspond to actual particles, we remove those coordinates that are close (closer that 50% of the particle size) to any coordinate included in the OR set. We filter out coordinates using the OR set instead of the AND set because there are many more true-positive particles in the OR set than in the AND set, and we prefer to ensure that most of the particles included in the NEG set are negative particles. Random picking strategies tend to obtain mostly empty particles or noncentered particles. However, particles containing ice or picked in the carbon regions are underrepresented. For this reason, we allow the user to provide a complementary set of negative particles, such as that available at http://campins.cnb.csic.es/deep_cons, that will be merged with the NEG set. In the case that the user does not provide such a set, as in the examples presented in this work, we alternatively employed a set of negative particles that was semi-automatically collected by applying Xmipp particle sorting to the AND set and considering particles with Z-scores in the top 1%, which typically correspond to the worst picked particles.

Evaluation: testing-set elaboration

In order to evaluate the performance of our method, we employed precision-recall and receiver operating characteristic (ROC) curves and computed the areas under both curves for each data set. Similarly, we estimated the accuracy, precision, recall and Matthews correlation coefficient (MCC) of DC predictions using the value that maximizes the MCC as a threshold. Such evaluations require a testing data set of particles for each evaluated case. We elaborated these by employing the particles deposited in EMPIAR as positive particles and randomly picked particles as negative particles, as performed in training-set generation. With the aim of improving the quality of our testing set, for each complex we manually curated both the positive and the negative particles of the initial testing set to a subset of 2000 positive and 2000 negative particles in which we also included ice, contamination etc. similarly as was performed in training-set generation.

Evaluation: resolution estimation

The goodness of the pruning performed by DC was also assessed by estimating the resolution values reached by the selected particles. To this end, we employed the RELION auto-refine algorithm (Scheres, 2012 ▸; Kimanius et al., 2016 ▸) using the set of particles that we collected internally in DC (AND/OR sets) as input as well as the DC-selected set (DC-retained set) and the filtered-out set of particles (DC-pruned set). The initial volumes required for auto-refine were downloaded from EMDB (Tagari et al., 2002 ▸) entries EMD-2984 and EMD-2984 filtered at 60 Å. In order to obtain the DC-retained and DC-pruned sets, a threshold of 0.5 was employed. Consequently, the DC-retained set is composed of all of the particles originally found in the OR set with a DC score greater than or equal to 0.5 and the DC-pruned set contains the particles included in the OR set with DC scores smaller than 0.5.

Evaluation: two-dimensional classification and class averages of different particle sets

The class averages displayed in Section 3.1.3 were obtained using the RELION two-dimensional classification algorithm (Scheres, 2012 ▸; Kimanius et al., 2016 ▸) on the particles of the OR, AND and DC-retained sets (a threshold of 0.5 was set). We only show the four classes with the most particles. All 32 classes obtained in the execution of the RELION two-dimensional classification are included in Appendix B .

Comparison with other pruning approaches

DC was compared with other pruning methodologies in terms of achieved resolution and execution time. Resolution estimation was performed as explained in Section 2.5. Two-dimensional classification was performed using RELION-2.0. Other two-dimensional classification algorithms such as cl2d in Xmipp (Sorzano et al., 2010 ▸) or ISAC in SPARX (Yang et al., 2012 ▸) were also initially considered, but since they were much slower than RELION-2.0 on GPUs and their use was only for comparison purposes and was not at the core of our newly proposed method, they were not finally included in this work. Both RELION two-dimensional classification and DC were executed using one Nvidia 1070 GTX graphics card, while RELION auto-refine was executed using two Nvidia 1070 GTX graphics cards. DC-retained particles were selected with a 0.5 threshold.

Results and discussion

Performance evaluation

The performance of our approach has been assessed on two publicly available data sets: EMPIAR-10028 (ribosome; Wong et al., 2014 ▸) and EMPIAR-10061 (β-galactosidase; Bartesaghi et al., 2015 ▸). In both cases we compiled the DC input sets using two well established algorithms: the Xmipp autopicker (Abrishami et al., 2013 ▸) and the EMAN2/SPARX Gaussian picker (Tang et al., 2007 ▸; Hohn et al., 2007 ▸). We carried out three different quality-assessment tests on the obtained results: a statistical analysis of manually curated testing sets of particles, a visual inspection of two-dimensional class averages and an evaluation of the final resolution obtained from the different sets of particles.

Statistical analysis

We evaluated the performance of DC by measuring several statistical scores on a manually curated testing set derived from particles deposited in the EMPIAR database (Iudin et al., 2016 ▸; see Section 2.4 for details of the testing-set collection) and we compared it with the individual performance of each of the particle pickers that were used for input to DC. Table 2 ▸ displays how DC obtained almost perfect classification metrics for the two evaluated data sets, with precision and recall values above 0.9. Similarly, the curves displayed in Fig. 2 ▸ are close to a perfect classification, indicating that DC was able to distinguish positive particles from negative particles outstandingly well. Finally, as can be appreciated from Table 2 ▸, DC achieved better results than those obtained by the individual particle pickers used as input, which proves that DC has succeeded in going beyond merely combining the two sets of input particles.

Table 2

Statistical measurements of Deep Consensus and the performance of the input particle pickers

MCC, Matthews correlation coefficient; ACC, accuracy; ROC-auc, area under the ROC curve; PR-auc, area under the precision-recall curve; NA, not available; DC, Deep Consensus; Xmipp, Xmipp autopicker; Gaussian, EMAN2/SPARX Gaussian picker. MCC, precision and recall were computed at the threshold that maximizes the MCC for DC and at the suggested threshold for Xmipp and Gaussian.

Algorithm	EMPIAR data set	MCC	ACC	Precision	Recall	ROC-auc	PR-auc
DC	10061	0.889	0.944	0.927	0.965	0.982	0.973
DC	10028	0.942	0.971	0.958	0.984	0.993	0.989
Xmipp	10061	0.782	0.893	0.898	0.849	NA	NA
Xmipp	10028	0.818	0.908	0.872	0.937	NA	NA
Gaussian	10061	0.697	0.845	0.778	0.904	NA	NA
Gaussian	10028	0.726	0.871	0.798	0.860	NA	NA

Figure 2

Deep Consensus precision-recall and ROC curves computed from testing sets. Red, the EMPIAR 10028 data set (ribosome); blue, the EMPIAR 10061 data set (β-galactosidase). The area under the curve (auc) is given in parentheses.

Resolution analysis

At this point, we wanted to better understand the new scenario that DC brings to the SAP field with a very simple and direct experiment: what are the final resolutions of the different cryo-EM maps obtained from each of the particle sets? For simplicity, we always use the same reconstruction method (Scheres, 2012 ▸; Kimanius et al., 2016 ▸) with all parameters set to the same values for the different runs (see Section 2.5). In this way, the single difference between the runs will be the different data sets of particles that are being fed into the algorithm. Table 3 ▸ compares the different resolution values computed over the different particle sets.

Table 3

Resolution achieved in both data sets when refining different sets of particles

OR, particles selected by any picker; AND, particles selected by both pickers; BPP, particles selected by the picker that obtained the best results; DC-pruned, particles ruled out by Deep Consensus; DC-retained, particles selected as good by Deep Consensus; R, resolution; N, number of particles.

	OR		AND		BPP		DC-retained		DC-pruned
EMPIAR data set	R (Å)	N	R (Å)	N	R (Å)	N	R (Å)	N	R (Å)	N
10061	3.76	231251	3.32	25600	2.92	117047	2.83	125586	12.74	105665
10028	3.83	119171	3.87	67043	3.70	97561	3.65	88622	33.50	30549

From inspection of this table, it is very clear that the resolution obtained using the OR set of particles (those picked by at least one of the pickers) is comparable or worse than the resolution obtained using the AND set (the consensus data set among the pickers), even if this latter set contains an order of magnitude fewer particles than the former set. However, many good particles are missing in the small AND set, which is shown clearly by the fact that if we were to use the results of only ‘the best picker’ (we refer to the picker that performed the best in these two data sets, which was the Xmipp picker) the resolution would still be better than that obtained with the small AND particle set.

However, the power of DC becomes evident when viewing the results presented in the two leftmost columns. Indeed, when the particles retained by DC are employed, the resolution of the maps always increases over that achieved when using any other data set, including that formed by the particles from the best-performing picking algorithm. At the same time, it is very clear that those particles rejected by DC (which are between 20% and greater than 30% of the OR data set) were creating very important inconsistencies in the whole reconstruction process, simply because their resulting map has a resolution that is an order of magnitude worse than that obtained with any other data set.

Finally, if we also consider the number of particles included in the AND, OR and DC-retained sets, it seems clear that our method has been able to go beyond the AND set by rescuing from the OR set many particles that are not included in the AND set but are still positive particles and thus good candidates to achieve a better resolution map. This also proves that our neural network, which has been trained on a reduced and slightly mislabeled training set, is able to learn and generalize to other particles that were not included in the training set.

Two-dimensional classification and class averages of different particle sets

In order to obtain another assessment of the value of DC, we performed a two-dimensional classification using the same data sets as presented in the previous section and compared the classes visually. As before, we used the same processing parameters in all runs, only changing the data sets. Fig. 3 ▸ shows the four most populated two-dimensional class averages obtained from the particles in the AND, OR and DC-retained data sets, so that a visual (qualitative) assessment can be performed (the averages of all classes have been included in Appendix B ). Within the limits of this assessment (and considering that the four major classes from each data set do not necessarily have to present the complex in the same orientation, especially for data sets with a good angular coverage, as is the case in our examples), at the level of high-resolution content the classes obtained from the DC-retained particles are the best, followed by those from the AND data set, while those from the OR data set are very poor. These results support the notion that DC has been able to prune many of the bad particles contained in the OR set but yet recovered many more particles than those included in the AND set.

Figure 3

Averages of the major classes obtained from the particles in the AND, OR and DC-retained data sets, all computed using the RELION two-dimensional classification algorithm.

In SPA cryo-EM there is currently a trend towards selecting as many particles as possible at the beginning of the image-processing workflow (Wang et al., 2016 ▸) despite the inclusion of many false positives. These false-positive particles are expected to be ruled out in the subsequent steps of the image-processing workflow, especially in the very time-consuming steps of two-dimensional and three-dimensional classification, which are certainly demanding of computational resources but also rely on strong human intervention, a factor that introduces subjective decisions into the analysis workflow. Consequently, and this is one of the motivations of this work, processing workflows can be substantially accelerated and automated by applying precise pruning methods such as DC at the very beginning of the image-processing workflow in such a way that the initial set of particles will be smaller but better.

In order to grasp how useful our approach may be, we have compared DC with other techniques that are commonly employed as pruning steps, specifically Z-score particle sorting (Vargas et al., 2013 ▸) and two-dimensional classification (Scheres, 2012 ▸; Kimanius et al., 2016 ▸). Comparisons have focused on the execution time and on the quality of the selected particles (see Section 2.7 for details).

Owing to their similarities, we would have liked to compare DC with MAPPOS (Norousi et al., 2013 ▸); however, as neither the program nor the particles that were used to evaluate MAPPOS are available, we were not able to do so. Nevertheless, it is worth noting that our approach exhibits a very important advantage over MAPPOS: the semi-automatic training-set generation. Moreover, the precision-recall values reported in the MAPPOS publication (around 0.9 and 0.7, respectively) are noticeably worse than those that we have measured in this work and, although not directly comparable, they are in line with the idea that deep-learning algorithms tend to outperform conventional machine-learning approaches.

When DC was compared with the Z-score particle-sorting approach (Vargas et al., 2013 ▸), using default thresholds for both methods, DC was able to prune many more particles. Moreover, the resolution obtained by DC was substantially better than that obtained when using only Z-score particle sorting.

A more detailed comparison was performed between the relative performance of DC and a ‘typical’ step of particle pruning by two-dimensional classification. Naturally, pruning by two-dimensional classification requires user intervention, which in the case of the results presented in this manuscript was achieved by a member of the laboratory experienced in dealing with many experimental data sets. Still, there is an intrinsic ‘human variability and subjectivity’ factor in this procedure that is unavoidable (and that DC aims to abolish). In this way, DC was able to prune slightly more particles than two-dimensional classification, while preserving essentially the same resolution values (see Table 4 ▸). Similarly, in order to study the composition of the ruled-out sets of particles, we measured the resolution that was achieved by these sets using the same evaluation procedure for both DC and two-dimensional classification (see Table 2 ▸). Thus, we measured a resolution of ∼12 Å for the EMPIAR-10061 data set (12.7 and 11.4 Å, respectively), whereas a resolution of ∼32 Å was measured for the EMPIAR-10028 data set (33.5 and 31.6 Å, respectively); the resolution was better for EMPIAR-10061, probably because the set of discarded particles was larger, but was still similar for both DC and two-dimensional classification. Accordingly, from the ‘final resolution’ point of view, DC and pruning by two-dimensional classification achieved similar results, suggesting that they could be employed interchangeably. However, under our benchmarking conditions (see Section 2.7) the running time of DC was approximately five times faster than a typical two-dimensional classification step while not introducing any human subjectivity, leading to automation; these are two very valuable parameters in order to increase data processivity and reproducibility in cryo-EM.

Table 4

Comparison of different pruning approaches

DC-retained, particles selected as good by Deep Consensus; Z-score-retained, particles that were selected as good using Xmipp particle sorting; R-2D-retained, particles that were selected as good by an expert after using RELION two-dimensional classification; R, resolution; PR, percentage of retained particles compared with the total number of particles (231 251 and 119 171, respectively); T, running time of the pruning algorithm; TT, total running time for the pruning and RELION auto-refine steps.

	DC-retained				Z-score-retained				R-2D-retained
EMPIAR data set	R (Å)	PR (%)	T (h)	TT (h)	R (Å)	PR (%)	T (h)	TT (h)	R (Å)	PR (%)	T (h)	TT (h)
10061	2.83	54.3	3.9	20.3	3.72	95.2	2.0	25.1	2.80	56.9	23.1	40.2
10028	3.65	74.4	2.7	12.0	3.77	94.9	1.4	14.6	3.65	85.6	14.8	27.6

Conclusions

In this work, we describe Deep Consensus, a deep-learning approach for the pruning of cryo-EM particles. Our method employs a convolutional neural network (CNN) trained on a set of true and false particles. Contrary to most deep-learning setups, for which data sets need to be carefully compiled by human experts, we employed a semi-automatically collected training set. This training set is obtained by computing the consensus outputs of multiple particle-picking algorithms. Thus, the positive particles used for training are obtained by taking the intersection of the output coordinates (allowing some error margins), whereas the negative particles are picked at random coordinates that are distant from any of the particles picked by any method (union). Finally, the particles contained in the union are classified as positive or negative by the trained CNN and those classified as negative are removed from the initial set.

We have shown that the Deep Consensus approach is considerably robust to mislabeling, and thus our method is able to be trained using sets that contain a significant fraction of false positives and false negatives. Indeed, as shown in Section 3.1, we have proven that Deep Consensus was able to learn from the semi-automatically generated sets and was able to identify a large number of positive particles that were not included in the initial training set, while removing many of the negative particles selected by the picking algorithms.

Finally, we have compared Deep Consensus with other pruning strategies and showed that it works better, or at least as well, as commonly applied methods. Moreover, Deep Consensus provides an important advantage, since it accelerates the image-processing workflow while avoiding user subjectivity, so that it can be fully standardized and automated. As a result, Deep Consensus seems to be a very promising approach for application at the very beginning of cryo-EM workflows, just after the step of particle picking.

Consequently, we consider that we have achieved our aim of helping the user to accelerate and automate one of the most critical steps in cryo-EM image processing, particle pruning, thus increasing objectivity and reproducibility in the initial steps of processing and at the same time facilitating the widespread usage of cryo-EM image-processing workflows by users with many diverse backgrounds.

Deep Consensus is publicly available from Xmipp (http://xmipp.cnb.csic.es) and Scipion (http://scipion.cnb.csic.es).

Table 5

Deep Consensus performance on testing sets when trained using synthetic AND sets with different levels of mislabeling noise

R, ribosome data set (EMPIAR-10028); G, β-galactosidase data set (EMPIAR-10061); MCC, Matthews correlation coefficient; ACC, accuracy; ROC-auc, area under the ROC curve. MCC, precision and recall were computed at the threshold that maximizes the MCC.

	MCC		Precision		Recall		ACC		ROC-auc
Corruption level	R	G	R	G	R	G	R	G	R	G
0%	0.934	0.884	0.965	0.937	0.952	0.927	0.982	0.961	0.992	0.969
25%	0.906	0.861	0.946	0.928	0.948	0.914	0.965	0.950	0.987	0.967
30%	0.875	0.851	0.923	0.918	0.942	0.914	0.949	0.944	0.978	0.964
40%	0.722	0.672	0.845	0.834	0.872	0.786	0.870	0.849	0.926	0.878
45%	0.435	0.264	0.710	0.652	0.736	0.527	0.720	0.630	0.776	0.663
50%	0.087	0.077	0.563	0.574	0.598	0.646	0.536	0.531	0.523	0.491

Table 6

Deep Consensus precision and recall on testing sets when trained using synthetic AND sets of different sizes with different levels of mislabelling noise

R, ribosome data set (EMPIAR-10028); G, β-galactosidase data set (EMPIAR-10061); #Partic, number of true particles included in the data set; corrupt, corruption level. Each cell displays the precision and recall measured in each condition.

#Partic	3000		2000		1000		500
Corrupt	R	G	R	G	R	G	R	G
30%	0.923/0.942	0.918/0.914	0.920/0.923	0.902/0.917	0.866/0.926	0.876/0.952	0.800/0.888	0.816/0.900
40%	0.839/0.902	0.840/0.897	0.774/0.819	0.835/0.890	0.738/0.820	0.762/0.595	0.693/0.818	0.726/0.586
45%	0.705/0.762	0.695/0.817	0.662/0.698	0.610/0.701	0.602/0.777	0.581/0.731	0.625/0.709	0.578/0.604