<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing DTD v2.3 20070202//EN" "journalpublishing.dtd">
<article article-type="review-article" dtd-version="2.3" xml:lang="EN" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Energy Res.</journal-id>
<journal-title>Frontiers in Energy Research</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Energy Res.</abbrev-journal-title>
<issn pub-type="epub">2296-598X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">639741</article-id>
<article-id pub-id-type="doi">10.3389/fenrg.2021.639741</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Energy Research</subject>
<subj-group>
<subject>Mini Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Recent Advances in Screening Lithium Solid-State Electrolytes Through Machine Learning</article-title>
<alt-title alt-title-type="left-running-head">Liu et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Screening Lithium Solid-State Electrolyte</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Liu</surname>
<given-names>Hongcan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="http://loop.frontiersin.org/people/1138636/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Ma</surname>
<given-names>Shun</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1217543/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wu</surname>
<given-names>Junjun</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1217545/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wang</surname>
<given-names>Yingkai</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1217539/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wang</surname>
<given-names>Xinghui</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x002A;<sup>&#x2020;</sup>
</xref>
<uri xlink:href="http://loop.frontiersin.org/people/843708/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<label>
<sup>1</sup>
</label>College of Physics and Information Engineering, Institute of Micro-Nano Devices and Solar Cells, Fuzhou University, <addr-line>Fuzhou</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<label>
<sup>2</sup>
</label>Jiangsu Collaborative Innovation Center of Photovolatic Science and Engineering, <addr-line>Changzhou</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1034458/overview">Jiajun Wang</ext-link>, Harbin Institute of Technology, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/354777/overview">Wei Luo</ext-link>, Tongji University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/190144/overview">Xia Li</ext-link>, Concordia University, Canada</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Xinghui Wang, <email>seaphy23@fzu.edu.cn</email>, <bold>
<sup>&#x2020;</sup>ORCID:</bold> Xinghui Wang, <email>orcid.org/0000-0002-5384-0666</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Electrochemical Energy Conversion and Storage, a section of the journal Frontiers in Energy Research</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>10</day>
<month>02</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>9</volume>
<elocation-id>639741</elocation-id>
<history>
<date date-type="received">
<day>09</day>
<month>12</month>
<year>2020</year>
</date>
<date date-type="accepted">
<day>07</day>
<month>01</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Liu, Ma, Wu, Wang and Wang.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Liu, Ma, Wu, Wang and Wang</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Compared to liquid electrolytes, lithium solid-state electrolytes have received increased attention in the field of all-solid-state lithium ion batteries due to safety requirements and higher energy density. However, solid-state electrolytes face many challenges, including lower ionic conductivity, complex interfaces, and unstable physical or electrochemical properties. One of the most effective strategies is to find a new type of lithium solid-state electrolyte with improved properties. Traditional trial and error methods require resources and time to verify the new solid-state electrolytes. Recently, new lithium solid-state electrolytes were predicted through machine learning (ML), which has proved to be an efficient and reliable method for screening new functional materials. This paper reviews the lithium solid-state electrolytes that have been discovered based on ML algorithms. The selection and preprocessing of datasets in ML technology are initially discussed before describing the latest developments in screening lithium solid-state electrolytes through different ML algorithms in detail. Lastly, the stability of candidate solid-state electrolytes and the challenges of discovering new lithium solid-state electrolytes through ML are highlighted.</p>
</abstract>
<kwd-group>
<kwd>lithium ion battery</kwd>
<kwd>solid-state electrolyte</kwd>
<kwd>machine learning</kwd>
<kwd>simulating calculation</kwd>
<kwd>material</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Air pollution control has become an increasingly severe problem in recent years. Some countries aim to ban new gasoline and diesel-powered vehicles by 2030, and governments have implemented policies that develop renewable energy. However, most renewable energy sources, such as wind and solar power, are intermittent energy sources that use rechargeable batteries for storage to enable daily usage. Rechargeable batteries, especially lithium ion batteries (LIBs) with an organic liquid electrolyte, are used in portable consumer electronics and electric vehicles owing to their high energy density and long life span. Even though the energy density of the LIBs has improved tremendously over recent decades, it still needs to be further enhanced to meet the high requirements of the consumers. Moreover, safety is another vital issue that has impeded the application of these types of batteries after LIB safety accidents caused by organic liquid electrolytes (<xref ref-type="bibr" rid="B30">Qu et&#x20;al., 2015</xref>). An efficient solution to this problem is to replace flammable organic electrolytes with solid-state electrolytes, which could significantly reduce the risk of leaks, evaporation, and decomposition and ensure higher safety. Solid-state lithium ion batteries (ASSLIB) are being explored in next-generation LIBs. This research faces the challenge of creating stable solid-state electrolytes with high ionic conductivity (<xref ref-type="bibr" rid="B5">Borodin et&#x20;al., 2015</xref>).</p>
<p>Ideal solid-state electrolytes should ideally have the following merits: high ionic conductivity, a low migration energy barrier, a wide electrochemical window, strong electrochemical stability, and high mechanical rigidity to suppress dendrite growth on the anode. In the past few years, Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> (<xref ref-type="bibr" rid="B22">Kamaya et&#x20;al., 2011</xref>), Li<sub>7</sub>P<sub>3</sub>S<sub>11</sub> (<xref ref-type="bibr" rid="B44">Yamane et&#x20;al., 2007</xref>), and some solid polymer electrolytes were widely investigated. However, the lithium solid-state electrolytes reported to-date do not meet these commercial requirements and properties (<xref ref-type="bibr" rid="B12">Do et&#x20;al., 2013</xref>; <xref ref-type="bibr" rid="B39">Sun et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B47">Zhang et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B6">Chai et&#x20;al., 2017</xref>; <xref ref-type="bibr" rid="B45">Yang et&#x20;al., 2017</xref>) and new solid-state electrolytes with better performance are required. Traditional searching tactics involve trial-and-error methods that require a lot of time to fabricate and verify the new solid-state electrolytes, with slow progress and low efficiency.</p>
<p>The Materials Genome Initiative (founded in 2011) has successfully used a machine learning (ML) algorithm to screen new solid-state electrolytes (<xref ref-type="bibr" rid="B17">Holdren, 2011</xref>; <xref ref-type="bibr" rid="B9">Sendek et al., 2019</xref>; <xref ref-type="bibr" rid="B16">Hatakeyama-Sato et&#x20;al., 2018</xref>; <xref ref-type="bibr" rid="B43">Xie and Grossman, 2018</xref>; <xref ref-type="bibr" rid="B9">Cubuk et&#x20;al., 2019</xref>; <xref ref-type="bibr" rid="B48">Zhang et&#x20;al., 2019</xref>). ML is a statistical method involving different algorithm structures that can learn the key information from available data and extract useful characteristics. The computation speed of ML algorithms is much faster than density functional theory (DFT) (<xref ref-type="bibr" rid="B25">Li et&#x20;al., 2017</xref>; <xref ref-type="bibr" rid="B35">Sendek et&#x20;al., 2018</xref>). Conventional methods (e.g., the first principle-based DFT) may take over four weeks to predict, while ML only takes 1&#xa0;s (<xref ref-type="bibr" rid="B33">Saal et&#x20;al., 2013</xref>). ML technology is usually applied in forecasting attributes, aiming to reflect molecular materials and targeted attributes. <xref ref-type="fig" rid="F1">Figure&#x20;1A</xref> shows the typical workflow used in screening lithium solid-state electrolytes through ML algorithms. The whole screening process begins by selecting suitable descriptors (datasets) divided into three parts: training data, testing data, and validating data. They then use different ML algorithms, including supervised, semi-supervised, and unsupervised learning, to calculate and predict potential candidates. The ionic conductivity of candidates is further verified by the DFT or Vienna Ab-initio Simulation Package (VASP) simulation.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>
<bold>(A)</bold> Workflow of screening solid-state electrolytes through the ML algorithm. <bold>(B)</bold> The distribution of Li-contained compounds from the Material Project database. Inset: histogram of materials conductivity over standard value. <bold>(C)</bold> Computationally observed ionic conductivity in candidate materials and extrapolation to room temperature. Reprinted (adapted) with permission from (<xref ref-type="bibr" rid="B35">Sendek., et al 2018</xref>). Copyright (2019) American Chemical Society. <bold>(D)</bold> Predicted ionic conductivities for the system Li<sub>8-c</sub>A<sub>a</sub>B<sub>b</sub>O<sub>4</sub>. <bold>(E)</bold> Relationship between experimental and predicted ionic conductivity.</p>
</caption>
<graphic xlink:href="fenrg-09-639741-g001.tif"/>
</fig>
<p>Different ML algorithms with advantages could lead to varying results in screening lithium solid-state electrolytes. Generally, supervised learning (e.g., support vector machine, neural network, decision tree, regression method) needs huge data with an effective label to support the calculation and more accurate data. Unsupervised learning (e.g., clustering) could calculate the results by itself without labeling. Semi-supervised learning inherits the previous frame and is trained in many datasets. There is little cost involved in training new data, resulting in increasing calculation speed. This review offers a systematic comparison and discussion of the different algorithms used to boost discovery and further advance this new technology in screening the solid-state electrolytes.</p>
<p>The review first illustrates how others address and prepare with datasets, then introduces and discusses the latest developments in screening lithium solid-state electrolytes through different ML algorithms including Neural Network (NN), Support Vector Machine (SVM), Regression, and Clustering in detail. The review finally verifies the stability of some ML predicted materials and highlights the limitations and current challenges faced by ML-based screening for solid-state materials.</p>
</sec>
<sec id="s2">
<title>Screening Electrolytes Through Diverse Machine Learning</title>
<sec id="s2-1">
<title>Dataset and Preprocessing</title>
<p>ML technology prioritizes choosing an appropriate dataset and then transferring it to a shape that an algorithm can handle. The Material Project is a database of materials and core program of the Materials Genome Initiative (<xref ref-type="bibr" rid="B20">Jain et&#x20;al., 2013</xref>). It contains information about compounds from the Inorganic Crystal Structure Database (ICSD). <xref ref-type="fig" rid="F1">Figure&#x20;1B</xref> gives the lithium ionic conductivity distribution of all Li-contained compounds by pymatgen (<xref ref-type="bibr" rid="B27">Ong et&#x20;al., 2013</xref>). The data can be computed and analyzed by the Materials Application Programming Interface. The database includes information on the lattice structure, band structure, density of state, space group, energy, and phase diagram, etc. Different ML algorithms may use diverse descriptors and various representations as an input (<xref ref-type="bibr" rid="B10">Curtarolo et&#x20;al., 2012</xref>; <xref ref-type="bibr" rid="B21">Jain et&#x20;al., 2015</xref>; <xref ref-type="bibr" rid="B23">Kiran and Joseph, 2017</xref>). The more suitable the representation of the input data, the more accurately an algorithm can map it to the output data. For this reason, suitable input data should be easier to acquire than the output attributes that will be predicted, and it is better when the dimensionality is lower (<xref ref-type="bibr" rid="B15">Ghiringhelli et&#x20;al., 2015</xref>).</p>
<p>To solve simulation errors, data should be preprocessed deliberatively. The preprocessing stage extracts raw data features and gives the subset unique characteristics, consisting of a continuous curve or discrete data. Feature extraction involves the transformation of the original data to essential characteristics. Its transforms, maps, or changes the dimensions of the original data into new data that reflects the input information more clearly. A large number of descriptors encode structures and properties, including: Coulomb Matrix (<xref ref-type="bibr" rid="B31">Rupp et&#x20;al., 2012</xref>); Finger Prints; Graph Theory (<xref ref-type="bibr" rid="B4">Bonchev and Rouvray, 1991</xref>); 3D Geometry, Voronoi Tessellations (<xref ref-type="bibr" rid="B41">Ward et&#x20;al., 2017</xref>); Simplified Molecular Input Line Entry Systems (SMILES) based on radial distribution functions (<xref ref-type="bibr" rid="B34">Sch&#xfc;tt et&#x20;al., 2014</xref>); and property-labeled material fragments (<xref ref-type="bibr" rid="B18">Isayev et&#x20;al., 2017</xref>).</p>
</sec>
<sec id="s2-2">
<title>Neural Networks</title>
<p>Neural networks, like the human brain, have many layers and units. Weights store knowledge and then form a completed net. It can process the input data layer by layer, thus converting the initial input representation into a more closely related representation to the output target. Learning is the process of adjusting the weights so that the training data is more accurate.</p>
<p>Sendek et&#x20;al. reported a neural network for predicting the fast Li-ion conduction at room temperature (RT). They found that Li<sub>5</sub>B<sub>7</sub>S<sub>13</sub>, Li<sub>3</sub>InCl<sub>6</sub>, and Li<sub>2</sub>B<sub>2</sub>S<sub>5</sub> had high ionic conductivity (<xref ref-type="bibr" rid="B35">Sendek et&#x20;al., 2018</xref>). As shown in <xref ref-type="fig" rid="F1">Figure&#x20;1C</xref>, 11 crystalline compounds were identified from 317 candidate materials by the ML-guide method. The ionic conductivity of Li<sub>5</sub>B<sub>7</sub>S<sub>13</sub> was predicted to be 0.074&#xa0;S/cm, six times higher than the best-known material (<xref ref-type="bibr" rid="B11">Ding et&#x20;al., 2009</xref>; <xref ref-type="bibr" rid="B49">Zhao and Daemen, 2012</xref>; <xref ref-type="bibr" rid="B7">Chou and Hwang, 2014</xref>; <xref ref-type="bibr" rid="B8">Cubuk and Kaxiras, 2014</xref>; <xref ref-type="bibr" rid="B42">Xiao et&#x20;al., 2015</xref>). This study built a convolution neural network to train the atomistic structure, and five descriptors were used as input data. The ML-based simulation revealed a 44-times improvement in the log-average of conductivity compared to random guesswork and manual computation. However, the input data contained less information about properties, the number of materials screened was small, and the training precision was&#x20;low.</p>
<p>Zeeshan et&#x20;al. predicted that LiAuI<sub>4</sub> and Ba<sub>38</sub>Na<sub>58</sub>Li<sub>26</sub>N were superionic conductors with ionic conductivity of 9.4 &#xd7; 10<sup>&#x2013;4</sup> and 10<sup>&#x2013;3</sup>&#xa0;S/cm respectively through crystal graph convolutional neural network (CGCNN) (<xref ref-type="bibr" rid="B43">Xie and Grossman, 2018</xref>; <xref ref-type="bibr" rid="B46">Zeeshan et&#x20;al., 2018</xref>). The 100 networks model was used to predict shear and bulk moduli as well as some mechanical properties. The accuracy of the screening results was further confirmed by measuring electronic conductivity and thermodynamic stability. Compared to the usual models, the CGCNN method was more general but required more data to train. This method significantly decreased the costs involved with first-principles calculations.</p>
</sec>
<sec id="s2-3">
<title>Support Vector Machine</title>
<p>A support vector machine classifies various samples by different labels to find a partition hyperplane. However, there have many partition hyperplanes that can separate the training samples. The boundary should classify the input samples robustly and have the strongest generalization ability to the unseen examples. The Fujimura team employed the support vector regression (SVR) method to predict ionic conductivity (<xref ref-type="bibr" rid="B13">Fujimura et&#x20;al., 2013</xref>). <xref ref-type="fig" rid="F1">Figure&#x20;1D</xref> shows the predicted 72 compositions. This work indicated that Li<sub>4</sub>GeO<sub>4</sub> had the highest ionic conductivity. They used the SVM method with a Gaussian kernel to predict the low-temperature conductivities of the compounds. The phase transition temperature (<italic>T</italic>
<sub>c</sub>), diffusivity at 1600&#xa0;K (D<sub>1600</sub>), the average volume of the disordered structures (<italic>V</italic>
<sub>dis</sub>), and experimental temperature T were regarded as independent variables, while the logarithm of ionic conductivity as the dependent variable. To confirm which descriptor combinations can show the best performance, they undertook many experiments and included different numbers of variables to estimate the prediction error. The bootstrapping error was lowest when it chose a combination of these three: D<sub>1600</sub>,&#x20;T.</p>
<p>Cubuk et&#x20;al. discovered that LiN<sub>5</sub>P<sub>3</sub>O, Li<sub>3</sub>Na<sub>4</sub>O<sub>3</sub>, LiPO<sub>3</sub>, LiMg<sub>3</sub>K<sub>2</sub>O<sub>4</sub>, LiNaMg<sub>3</sub>O<sub>5</sub>, Li<sub>2</sub>K<sub>3</sub>GaO<sub>4</sub>, Li<sub>5</sub>Na<sub>2</sub>O<sub>3</sub>, Li<sub>4</sub>NaGaO<sub>4</sub>, Li<sub>2</sub>MgO<sub>2</sub>, Li<sub>5</sub>K<sub>2</sub>O<sub>3,</sub> and Li<sub>5</sub>Na<sub>2</sub>NO<sub>2</sub> satisfied all of the screening criteria, including stability, high Li conductivity, low cost and weight, and a large window of electrochemical stability (<xref ref-type="bibr" rid="B9">Cubuk et&#x20;al., 2019</xref>). They used 30 elemental descriptors from 40 materials to train a linear SVM through the leave-one-out cross-validation (<xref ref-type="bibr" rid="B36">Sendek et&#x20;al., 2016</xref>). The prediction accuracy is low because the selected 40 materials are out of Material Project or ICSD. In order to solve the trade-off between ML model accuracy and previously uncharacterized materials, they took the outputs of the structure model in Sendek&#x2019;s research (<xref ref-type="bibr" rid="B35">Sendek et&#x20;al., 2018</xref>) as the labels to train the generic descriptors model, named transfer learning (<xref ref-type="bibr" rid="B29">Pan and Yang, 2010</xref>). Through this transfer learning, a new generic model was trained using three datasets, including 40 data, Material Project data, and 21 of the 12,716&#x20;lithium-containing materials, with an accuracy of 87.5%, 92.0%, and 85.7%, respectively.</p>
<p>Because of these complex chemical systems, it is still difficult to completely calculate total conductivity by existing computing capacity. Most conductors have added polymers, such as plasticizers, which makes the calculations more complicated. To solve this complex interaction computing, Kan Hatakeyama-Sato&#x2019;s team used a polymer database to train a gradient boosting model, which shows a 90% accuracy for training data and 81% accuracy for the testing data (<xref ref-type="bibr" rid="B16">Hatakeyama-Sato et&#x20;al., 2018</xref>). As shown in <xref ref-type="fig" rid="F1">Figure&#x20;1E</xref>, experiment data were similar to the predicted ionic conductivity. The analysis indicated that electronegativity and polarity of the monomer units were dominant variables in determining ionic conductivity.</p>
</sec>
<sec id="s2-4">
<title>Regression Method</title>
<p>The regression model studies the relationship between dependent variables (targets) and independent variables (predictors), used in predictive analysis, time series models, and finding causal relationships between variables. The kernel ridge regression and gradient boosting regression algorithm model were used to find the potential solid-state electrolytes LiOH, LiAuI<sub>4</sub>, LiBH<sub>4</sub>, Li<sub>2</sub>WS<sub>4</sub>, and Ba<sub>38</sub>Na<sub>58</sub>Li<sub>26</sub>N, etc. (<xref ref-type="bibr" rid="B46">Zeeshan et&#x20;al., 2018</xref>), through training the elastic tensor from the materials project database. An elastic tensor can assess the interface stability between Li anode and solid-state electrolytes. Sendek&#x2019;s team related the crystallographic directions with the elastic tensor. They took DFT-computed information on 482 electrolyte materials as input data and set up an &#x2018;rbf&#x2019; kernel ridge model with &#x3b1; and &#x3b3; equal to 0.01, and two gradient boosting models with different max depth, minimum samples per leaf, and minimum samples split. This study predicted the elastic tensor of 548 materials with a cubic crystal structure. Although the training data was small, the regression model was useful. They found a relationship between material stiffness and other characteristics like mass density, the ratio of bond ionicity, volume per atom, and sub lattice electronegativity.</p>
<p>Another study employed logistic regression (LR) to identify superionic (<italic>&#x3c3;</italic> &#x2265; 10<sup>&#x2013;4</sup>&#xa0;S/cm) and non-superionic (<italic>&#x3c3;</italic> &#x3c; 10<sup>&#x2013;4</sup>&#xa0;S/cm) structures (<xref ref-type="bibr" rid="B36">Sendek et&#x20;al., 2016</xref>). Austin&#x2019;s team found that these compounds (BaLiBS<sub>3</sub>, Li<sub>5</sub>B<sub>7</sub>S<sub>13</sub>, Sr<sub>2</sub>LiCBr<sub>3</sub>N<sub>2</sub>, SrLi(BS<sub>2</sub>)<sub>3</sub>, LiErSe<sub>2</sub>, Li<sub>2</sub>B<sub>2</sub>S<sub>5</sub>, Li<sub>3</sub>ErCl<sub>6</sub>, Li<sub>2</sub>HIO, Li<sub>2</sub>GePbS<sub>4</sub>, LiSO<sub>3</sub>F, LiCl, LiSmS<sub>2</sub>, Li<sub>3</sub>InCl<sub>6</sub>, CsLi<sub>2</sub>BS<sub>3</sub>, LiMgB<sub>3</sub>(H<sub>9</sub>N)<sub>2</sub>, RbLiS, LiHoS<sub>2</sub>, LiErS<sub>2</sub>, LiHo<sub>3</sub>Ge<sub>2</sub>(O<sub>4</sub>F)<sub>2</sub>, KLiS) had superionic probability &#x2265;50%, band gap &#x2265;1&#xa0;eV, upper bound oxidation potential &#x2265;4&#xa0;V, no transition metals, energy above the convex hull &#x3d; 0&#xa0;eV per atom. The dataset consisted of 40 materials with 20 diverse feature characteristics shown in <xref ref-type="table" rid="T1">Table&#x20;1</xref>. It is worth noting that the Li&#x2013;B&#x2013;S system was also selected using NN methods (<xref ref-type="bibr" rid="B35">Sendek et&#x20;al., 2018</xref>). The regression illustrated how a multi-descriptor could build a model with better predictive power than a single feature alone. They used LR to build all possible models and then calculated the training misclassification rate (TMR) and the cross-validated misclassification rate (CVMR). As shown in <xref ref-type="fig" rid="F2">Figure&#x20;2A</xref>, the 5-feature model had minimal CVMR, proving that the model had statistical significance. The X-randomization performance metric parameter was above the conventional threshold of 0.5 for the optimal LR model. <xref ref-type="fig" rid="F2">Figure&#x20;2B</xref> shows the classification performance. The <italic>y</italic>-axis presents the conductivity higher than 10<sup>&#x2013;4</sup>&#xa0;S/cm, and four materials were misclassified.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Pearson correlation coefficient, training data standard deviation, training data mean, and normalized regression coefficient of 20 features.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="center">Feature</th>
<th align="center">Pearson correlation coefficient</th>
<th align="center">Training data standard deviation</th>
<th align="center">Training data mean</th>
<th align="center">Normalized regression coefficient</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">1</td>
<td align="left">Volume per atom<sup>a</sup>
</td>
<td align="center">0.20</td>
<td align="center">4.582</td>
<td align="center">13.342</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">2</td>
<td align="left">Standard deviation in Li neighbour count</td>
<td align="center">0.22</td>
<td align="center">1.430</td>
<td align="center">1.766</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">3</td>
<td align="left">Standard deviation in Li bond ionicity</td>
<td align="center">&#x2212;0.04</td>
<td align="center">0.274</td>
<td align="center">0.858</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">4</td>
<td align="left">Li bond ionicity<sup>a</sup>
</td>
<td align="center">&#x2212;0.18</td>
<td align="center">0.372</td>
<td align="center">1.403</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">5</td>
<td align="left">Li neighbour count<sup>a</sup>
</td>
<td align="center">&#x2212;0.19</td>
<td align="center">6.393</td>
<td align="center">21.359</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">6</td>
<td align="left">Li&#x2013;Li bonds per Li<sup>a</sup>
</td>
<td align="center">0.06</td>
<td align="center">4.432</td>
<td align="center">6.218</td>
<td align="center">&#x2b;0.817</td>
</tr>
<tr>
<td align="left">7</td>
<td align="left">Bond ionicity of sublattice<sup>a</sup>
</td>
<td align="center">&#x2212;0.28</td>
<td align="center">0.330</td>
<td align="center">0.978</td>
<td align="center">&#x2212;1.323</td>
</tr>
<tr>
<td align="left">8</td>
<td align="left">Sublattice neighbour count<sup>a</sup>
</td>
<td align="center">&#x2212;0.13</td>
<td align="center">7.087</td>
<td align="center">20.660</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">9</td>
<td align="left">Anion framework coordination<sup>a</sup>
</td>
<td align="center">&#x2212;0.06</td>
<td align="center">2.202</td>
<td align="center">10.073</td>
<td align="center">&#x2212;1.028</td>
</tr>
<tr>
<td align="left">10</td>
<td align="left">Minimum anion&#x2013;anion separation distance<sup>a</sup>
</td>
<td align="center">0.09</td>
<td align="center">0.708</td>
<td align="center">3.395</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">11</td>
<td align="left">Volume per anion (&#xc5;<sup>3</sup>)</td>
<td align="center">&#x2212;0.01</td>
<td align="center">35.131</td>
<td align="center">36.614</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">12</td>
<td align="left">Minimum Li&#x2013;anion separation distance<sup>a</sup> (&#xc5;)</td>
<td align="center">0.20</td>
<td align="center">0.288</td>
<td align="center">2.072</td>
<td align="center">&#x2b;2.509</td>
</tr>
<tr>
<td align="left">13</td>
<td align="left">Minimum Li&#x2013;Li separation distance<sup>a</sup> (&#xc5;)</td>
<td align="center">&#x2212;0.10</td>
<td align="center">0.746</td>
<td align="center">2.730</td>
<td align="center">&#x2212;1.619</td>
</tr>
<tr>
<td align="left">14</td>
<td align="left">Electronegativity of sublattice<sup>a</sup>
</td>
<td align="center">&#x2212;0.16</td>
<td align="center">0.306</td>
<td align="center">2.780</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">15</td>
<td align="left">Packing fraction of full crystal</td>
<td align="center">0.16</td>
<td align="center">0.173</td>
<td align="center">0.465</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">16</td>
<td align="left">Packing fraction of sublattice</td>
<td align="center">0.19</td>
<td align="center">0.186</td>
<td align="center">0.234</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">17</td>
<td align="left">Straight-line path width<sup>a</sup> (&#xc5;)</td>
<td align="center">0.07</td>
<td align="center">0.247</td>
<td align="center">0.852</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">18</td>
<td align="left">Straight-line path electronegativity<sup>a</sup>
</td>
<td align="center">&#x2212;0.29</td>
<td align="center">0.707</td>
<td align="center">2.535</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">19</td>
<td align="left">Ratio of features (4) and (7)</td>
<td align="center">&#x2212;0.03</td>
<td align="center">0.719</td>
<td align="center">1.611</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left">20</td>
<td align="left">Ratio of features (5) and (8)</td>
<td align="center">&#x2212;0.18</td>
<td align="center">0.152</td>
<td align="center">1.057</td>
<td align="center">0</td>
</tr>
<tr>
<td align="left"/>
<td align="left">Constant term</td>
<td align="center">&#x2014;</td>
<td align="center">&#x2014;</td>
<td align="center">&#x2014;</td>
<td align="center">&#x2212;1.944</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>The features &#x201c;a&#x201d; are averaged over the relevant parameter: bonds, atoms, Li&#x2013;Li pathways,&#x20;etc.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>
<bold>(A)</bold> The cross-validation misclassification rate (CVMR) curve and the training misclassification rate (TMR) curve. <bold>(B)</bold> Classification performance of the training data under leave-one-out cross-validation using logistic regression. <bold>(C)</bold> Unsupervised clustering of all Li-containing compounds, seven groups divided by algorithm. <bold>(D)</bold> The results of research through the ML method, displaying compound formula and ionic conductivity, respectively. <bold>(E)</bold> The parameters of energy formation/Atom (eV) and the energy above the hull/Atom (eV). The red line indicates the formation of energy, and the blue line indicates the energy above the&#x20;hull.</p>
</caption>
<graphic xlink:href="fenrg-09-639741-g002.tif"/>
</fig>
</sec>
<sec id="s2-5">
<title>Clustering Algorithm</title>
<p>It is difficult and time-consuming to calculate the migration barriers and ion diffusion of the solid-state electrolytes, especially considering the huge material space. The unsupervised learning algorithm can discover the relationship between properties and X-ray diffraction (XRD) intensities have emerged in screening lithium solid-state electrolytes. Zhang et&#x20;al. found that Li<sub>8</sub>N<sub>2</sub>Se, Li<sub>6</sub>KBiO<sub>6</sub>, and Li<sub>5</sub>P<sub>2</sub>N<sub>5</sub> (i.e.,&#x20;three new materials systems) had an ionic conductivity higher than 10<sup>&#x2013;2</sup>&#xa0;S/cm (<xref ref-type="bibr" rid="B48">Zhang et&#x20;al., 2019</xref>). <xref ref-type="fig" rid="F1">Figure&#x20;1C</xref> shows the tree dendrogram generated using the agglomerative hierarchical clustering method. The highest result appears in groups &#x2164; and &#x2165;. These new materials comprise new structures, chemistries, and compositions that are significantly different from existing chemistries. Using clustering methods to classify modified X-ray diffraction (mXRD) can define every anion lattice and fully capture the anionic crystal structure information. The data contained 528&#x20;compounds, and three different models were generated to classify the results. The latter two models were set to evaluate the robustness of the clustering algorithm.</p>
<p>The unsupervised learning rising algorithm discovered a quantitative correlation between group and conductivity. The clustering model captured the physical dependence of fast solid-state Li-ion diffusion on anion lattice and gathered excellent materials together. The unsupervised method solves the problem created by scarce datasets, unlike supervised learning models, which need label training data. In unsupervised learning, the label of training data is unknown. It relies on learning non-labeled data to reveal intrinsic properties and laws of data, which form the basis of data analysis. The variances and errors of model parameters are rarely affected by the experimental method.</p>
</sec>
</sec>
<sec sec-type="discussion" id="s3">
<title>Discussion</title>
<p>This study used different ML algorithms to screen and discover typical solid-state electrolytes with high ionic conductivity. As shown in <xref ref-type="fig" rid="F2">Figure&#x20;2D</xref>, most materials were concentrated in the range of 10<sup>&#x2013;4</sup>&#xa0;S/cm. In particular, Li<sub>5</sub>B<sub>7</sub>S<sub>13</sub>, Li<sub>8</sub>SeN<sub>2</sub>, KLi<sub>6</sub>BiO<sub>6</sub>, and Li<sub>5</sub>P<sub>2</sub>N<sub>5</sub> exhibit a high ionic conductivity near 10<sup>&#x2013;2</sup>&#xa0;S/cm. As a screening method for solid-state electrolytes, the NN structure had the most robust ability in precision or recall. The neural units can learn about the strange input layer by layer, resulting in a high learning rate, meaning that classification tasks often use the NN model. As for the clustering method, it can discover the complex unseen patterns hiding behind multi-dimensional data. If the clustering is sufficiently subdivided, the conductivity of the same species will be very similar. SVR has higher prediction accuracy and stability when there is less label data. Compared to the SVR, the LR algorithm has advantages in prediction efficiency, but the prediction accuracy fluctuates greatly. Gradient Boosting, Kernel Ridge Regression, and Crystal Graph Convolution Neural Network were distributed at lower ionic conductivity. Thus, clustering and the NN method provide robust prediction and a highly efficient screening method for solid-state electrolytes. Our recent work illustrates ML methods in applications, advantages, challenges, and typical references, as summarized in <xref ref-type="table" rid="T2">Table&#x20;2</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Comparison of different computational methods, the table shows the mentioned methods in advantages, challenges, applications, and recent typical references.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">References</th>
<th align="center">Application</th>
<th align="center">ML algorithm</th>
<th align="center">Advantage</th>
<th align="center">Challenge</th>
<th align="center">Year</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">12</td>
<td align="left">Stable composition screening</td>
<td align="left">Neural network</td>
<td align="left">High precision</td>
<td align="left">Model is too complex</td>
<td align="char" char=".">2018</td>
</tr>
<tr>
<td align="left">26</td>
<td align="left">Structure discovery</td>
<td align="left">Crystal graph convolutional neural network</td>
<td align="left">High accuracy and interpretability</td>
<td align="left">Data processing is too tedious</td>
<td align="char" char=".">2018</td>
</tr>
<tr>
<td align="left">27</td>
<td align="left">Ionic conductivity prediction</td>
<td align="left">Support vector regression</td>
<td align="left">Fast computing speed</td>
<td align="left">Low accuracy</td>
<td align="char" char=".">2013</td>
</tr>
<tr>
<td align="left">28</td>
<td align="left">Structure discovery</td>
<td align="left">Support vector machine and transfer learning</td>
<td align="left">Require less data</td>
<td align="left">Model is hard to be explained</td>
<td align="char" char=".">2019</td>
</tr>
<tr>
<td align="left">31</td>
<td align="left">Polymer material discovery</td>
<td align="left">Gradient boosting regression</td>
<td align="left">High accuracy</td>
<td align="left">Complex interactions computing</td>
<td align="char" char=".">2018</td>
</tr>
<tr>
<td align="left">29</td>
<td align="left">Superionic classification</td>
<td align="left">Logistic regression</td>
<td align="left">Abundant experiment metrics</td>
<td align="left">Processing is too complex</td>
<td align="char" char=".">2016</td>
</tr>
<tr>
<td align="left">40</td>
<td align="left">Solid-state electrolytes classification</td>
<td align="left">Clustering</td>
<td align="left">Candidate compounds have excellent properties</td>
<td align="left">Need a quantity of XRD data</td>
<td align="char" char=".">2019</td>
</tr>
<tr>
<td align="left">48</td>
<td align="left">Prediction of initial capacity and cycle life</td>
<td align="left">Extremely randomized tree and adaptive boosting</td>
<td align="left">High accuracy</td>
<td align="left">The scarcity of dataset</td>
<td align="char" char=".">2018</td>
</tr>
<tr>
<td align="left">49</td>
<td align="left">Ionic conductivity prediction</td>
<td align="left">Logistic regression</td>
<td align="left">Exhibit wider thermodynamic electrochemical stability</td>
<td align="left">Validation accuracy still too low</td>
<td align="char" char=".">2019</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>It is important to verify the stability of the predicted materials, which could be determined by their formation energy and energy above hull: E<sub>hull</sub> (<xref ref-type="bibr" rid="B28">Ong et&#x20;al., 2008</xref>; <xref ref-type="bibr" rid="B19">Jain et&#x20;al., 2011</xref>). Theoretically, the formation of energy should be negative and E<sub>hull</sub> &#x3d; 0&#xa0;eV for thermodynamically stable materials. First principles were used to calculate the formation of energy and E<sub>hull</sub> of the screening results from previous research via VASP. As shown in <xref ref-type="fig" rid="F2">Figure&#x20;2E</xref>, the typical predicted materials have negative formation energy, and most of the samples exhibit a low E<sub>hull</sub>, almost equal to zero, confirming a stable thermodynamically. It is worth to mention that Li<sub>6</sub>Ho(BO<sub>3</sub>)<sub>3</sub>, with ionic conductivity of up to 5.1 &#xd7; 10<sup>&#x2212;3</sup>&#xa0;S/cm in (<xref ref-type="bibr" rid="B35">Sendek et&#x20;al., 2018</xref>) shows both low formation energy and zero energy above the hull, which could be a promising material. In addition to the ionic conductivity, the electrochemical stable window (<xref ref-type="bibr" rid="B40">Wang et&#x20;al., 2015</xref>) is another crucial feature in screening excellent solid-state electrolytes. Yizhou Zhu&#x2019;s team (<xref ref-type="bibr" rid="B51">Zhu et&#x20;al., 2015</xref>) used first principles to analyze thermodynamics and found that solid-state electrolyte materials have a limited electrochemical window. Thus, when considering candidate solid-state electrolytes, formation energy, energy above the hull, and the electrochemical window should also be included.</p>
<p>There are still many factors limiting the process of screening new solid-state electrolytes. 1) The training data is still not large enough to satisfy the big structure model, which affects the accuracy of the screening results. 2) The constructed model is still too complicated and cannot adapt to the scarcity of material data, and the model should be as simple as possible. 3) Suitable descriptors have not yet been precisely selected, and there is still no quantitative connection between performance and the parameters of the material. To tackle these challenges, we need greater effects both from the material and algorithmic scientists. On the one hand, material scientists should fabricate and verify the lithium solid-state electrolytes found through ML, which will increase the dataset and provide better guidance for the further optimization of the algorithm. On the other hand, more advanced or updated methodologies could be applied to screen lithium solid-state electrolytes according to data availability. For example, neural networks (e.g., Auto Encoders, Generative Adversarial Networks, etc.) were recently used to predict crystal and material properties (<xref ref-type="bibr" rid="B32">Ryan et&#x20;al., 2018</xref>; <xref ref-type="bibr" rid="B50">Zheng et&#x20;al., 2018</xref>), even in a scenario with little training data. Active learning (<xref ref-type="bibr" rid="B14">Gao et&#x20;al., 2020</xref>) combines data labeling and model training to minimize labeling costs by prioritizing high-value data and classifying the materials based on small material data. These new algorithms have potential applications in screening for lithium solid-state electrolytes.</p>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>This review discusses the latest developments in the use of ML algorithms in screening for solid-state electrolyte materials. Some potential lithium solid-state electrolytes were predicted with high ionic conductivity and stability. We focused on demonstrating various ML algorithms, including clustering, support vector machine, neural networks, and regression, used in screening for solid-state electrolytes. In general, neural networks showed a significant advantage in screening. The challenge of using ML in screening for solid-state electrolytes include a lack of data and complicated algorithms. These could be resolved by experimentally verifying the predicted candidates and developing new ML algorithms. As a powerful simulation method, ML have accelerated the discovery of lithium solid-state electrolytes and could be developed to screen for other functional materials.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Author Contributions</title>
<p>HL, SM, JW, YW - College of Physics and Information Engineering, Institute of Micro-Nano Devices and Solar Cells, Fuzhou University, Fuzhou, Fujian 350108, People&#x0027;s Republic of China; XW &#x2010; College of Physics and Information Engineering, Institute of Micro-Nano Devices and Solar Cells, Fuzhou University, Fuzhou, Fujian 350108, People&#x0027;s Republic of China; Jiangsu Collaborative Innovation Center of Photovolatic Science and Engineering, Changzhou, Jiangsu 213164, People&#x0027;s Republic of China.</p>
</sec>
<sec id="s6">
<title>Funding</title>
<p>This work was supported by the National Natural Science Foundation of China (Grant 11704071), the Excellent Youth Foundation of the Fujian Scientific Committee (Grant 2019J06008), and the Award Program, Fujian Minjiang Scholar Professorship.</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<ref-list>
<title>References</title>
<ref id="B4">
<citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname>Bonchev</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Rouvray</surname>
<given-names>D. H.</given-names>
</name>
</person-group> (<year>1991</year>). <source>Chemical graph theory: introduction and fundamentals</source>. <publisher-loc>New York</publisher-loc>: <publisher-name>Abacus Press</publisher-name>.</citation>
</ref>
<ref id="B5">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Borodin</surname>
<given-names>O.</given-names>
</name>
<name>
<surname>Olguin</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Spear</surname>
<given-names>C. E.</given-names>
</name>
<name>
<surname>Leiter</surname>
<given-names>K. W.</given-names>
</name>
<name>
<surname>Knap</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Towards high throughput screening of electrochemical stability of battery electrolytes</article-title>. <source>Nanotechnology</source> <volume>26</volume> (<issue>35</issue>), <fpage>354</fpage>. <pub-id pub-id-type="doi">10.1088/0957-4484/26/35/354003</pub-id> </citation>
</ref>
<ref id="B6">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Chai</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Liu</surname>
<given-names>Z.</given-names>
</name>
<name>
<surname>Ma</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Liu</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Miao</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Liu</surname>
<given-names>D.</given-names>
</name>
<etal/>
</person-group> (<year>2017</year>). <article-title>
<italic>In Situ</italic> generation of poly (Vinylene carbonate) based solid electrolyte with interfacial stability for LiCoO2 lithium batteries</article-title>. <source>Adv. Sci.</source> <volume>4</volume> (<issue>2</issue>), <fpage>377</fpage>. <pub-id pub-id-type="doi">10.1002/advs.201600377</pub-id> </citation>
</ref>
<ref id="B7">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Chou</surname>
<given-names>C.-Y.</given-names>
</name>
<name>
<surname>Hwang</surname>
<given-names>G. S.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>On the origin of the significant difference in lithiation behavior between silicon and germanium</article-title>. <source>J.&#x20;Power Sources</source> <volume>263</volume>, <fpage>252</fpage>&#x2013;<lpage>258</lpage>. <pub-id pub-id-type="doi">10.1016/j.jpowsour.2014.04.011</pub-id> </citation>
</ref>
<ref id="B8">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Cubuk</surname>
<given-names>E. D.</given-names>
</name>
<name>
<surname>Kaxiras</surname>
<given-names>E.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>Theory of structural transformation in lithiated amorphous silicon</article-title>. <source>Nano Lett.</source> <volume>14</volume> (<issue>7</issue>), <fpage>4065</fpage>&#x2013;<lpage>4070</lpage>. <pub-id pub-id-type="doi">10.1021/nl5015525</pub-id> </citation>
</ref>
<ref id="B9">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Cubuk</surname>
<given-names>E. D.</given-names>
</name>
<name>
<surname>Sendek</surname>
<given-names>A. D.</given-names>
</name>
<name>
<surname>Reed</surname>
<given-names>E. J.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Screening billions of candidates for solid lithium-ion conductors: a transfer learning approach for small data</article-title>. <source>J.&#x20;Chem. Phys.</source> <volume>150</volume>, <fpage>214701</fpage>. <pub-id pub-id-type="doi">10.1063/1.5093220</pub-id> </citation>
</ref>
<ref id="B10">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Curtarolo</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Setyawan</surname>
<given-names>W.</given-names>
</name>
<name>
<surname>Wang</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Xue</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Yang</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Taylor</surname>
<given-names>R. H.</given-names>
</name>
<etal/>
</person-group> (<year>2012</year>). <article-title>AFLOWLIB.ORG: a distributed materials properties repository from high-throughput ab initio calculations</article-title>. <source>Comput. Mater. Sci.</source> <volume>58</volume>, <fpage>227</fpage>&#x2013;<lpage>235</lpage>. <pub-id pub-id-type="doi">10.1016/j.commatsci.2012.02.002</pub-id> </citation>
</ref>
<ref id="B11">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ding</surname>
<given-names>N.</given-names>
</name>
<name>
<surname>Xu</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Yao</surname>
<given-names>Y. X.</given-names>
</name>
<name>
<surname>Wegner</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Fang</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Chen</surname>
<given-names>C. H.</given-names>
</name>
<etal/>
</person-group> (<year>2009</year>). <article-title>Determination of the diffusion coefficient of lithium ions in nano-Si</article-title>. <source>Solid State Ionics</source> <volume>180</volume> (<issue>2&#x2013;3</issue>), <fpage>222</fpage>&#x2013;<lpage>225</lpage>. <pub-id pub-id-type="doi">10.1016/j.ssi.2008.12.015</pub-id> </citation>
</ref>
<ref id="B12">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Do</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Lunkenheimer</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Diddens</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>G&#xf6;tz</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Weiss</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Loidl</surname>
<given-names>A.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Li&#x2b; transport in poly(ethylene oxide) based electrolytes: neutron scattering, dielectric spectroscopy, and molecular dynamics simulations</article-title>. <source>Phys. Rev. Lett.</source> <volume>111</volume> (<issue>1</issue>), <fpage>018301</fpage>. <pub-id pub-id-type="doi">10.1103/PhysRevLett.111.018301</pub-id> </citation>
</ref>
<ref id="B13">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Fujimura</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Seko</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Koyama</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Kuwabara</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Kishida</surname>
<given-names>I.</given-names>
</name>
<name>
<surname>Shitara</surname>
<given-names>K.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Accelerated materials design of lithium superionic conductors based on first-principles calculations and machine learning algorithms</article-title>. <source>Adv. Energy Mater.</source> <volume>3</volume>, <fpage>980</fpage>&#x2013;<lpage>985</lpage>. <pub-id pub-id-type="doi">10.1002/aenm.201300060</pub-id> </citation>
</ref>
<ref id="B14">
<citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname>Gao</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Zhang</surname>
<given-names>Z.</given-names>
</name>
<name>
<surname>Guo</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Ar&#x131;k</surname>
<given-names>S. &#xd6;.</given-names>
</name>
<name>
<surname>Davis</surname>
<given-names>L. S.</given-names>
</name>
<name>
<surname>Pfister</surname>
<given-names>T.</given-names>
</name>
</person-group> (<year>2020</year>). &#x201c;<article-title>Consistency-based semi-supervised active learning: towards minimizing labeling cost</article-title>,&#x201d; in <source>Computer Vision &#x2013; ECCV 2020. Eccv 2020. Lecture Notes in Computer Science</source>. Editors <person-group person-group-type="editor">
<name>
<surname>Vedaldi</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Bischof</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Brox</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>Frahm</surname>
<given-names>JM.</given-names>
</name>
</person-group> (<publisher-loc>Cham</publisher-loc>: <publisher-name>Springer</publisher-name>). </citation>
</ref>
<ref id="B15">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ghiringhelli</surname>
<given-names>L. M.</given-names>
</name>
<name>
<surname>Vybiral</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Levchenko</surname>
<given-names>S. V.</given-names>
</name>
<name>
<surname>Draxl</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Scheffler</surname>
<given-names>M.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Big data of materials science: critical role of the descriptor</article-title>. <source>Phys. Rev. Lett.</source> <volume>114</volume> (<issue>10</issue>), <fpage>105503</fpage>. <pub-id pub-id-type="doi">10.1103/PhysRevLett.114.105503</pub-id> </citation>
</ref>
<ref id="B16">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hatakeyama-Sato</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Tezuka</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>Nishikitani</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Nishide</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Oyaizu</surname>
<given-names>K.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Synthesis of lithium-ion conducting polymers designed by machine learning-based prediction and screening</article-title>. <source>Chem. Lett.</source> <volume>48</volume>, <fpage>130</fpage>. <pub-id pub-id-type="doi">10.1246/cl.180847</pub-id> </citation>
</ref>
<ref id="B17">
<citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname>Holdren</surname>
<given-names>J.&#x20;P.</given-names>
</name>
</person-group> (<year>2011</year>). <source>Materials genome initiative for global competitiveness, Report</source>. <publisher-loc>United&#x20;States</publisher-loc>: <publisher-name>White House Office of Science and Technology Policy</publisher-name>.</citation>
</ref>
<ref id="B18">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Isayev</surname>
<given-names>O.</given-names>
</name>
<name>
<surname>Oses</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Toher</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Gossett</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Curtarolo</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Tropsha</surname>
<given-names>A.</given-names>
</name>
</person-group> (<year>2017</year>). <article-title>Universal fragment descriptors for predicting properties of inorganic crystals</article-title>. <source>Nat. Commun.</source> <volume>8</volume>, <fpage>15679</fpage>. <pub-id pub-id-type="doi">10.1038/ncomms15679</pub-id> </citation>
</ref>
<ref id="B19">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jain</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Hautier</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Moore</surname>
<given-names>C. J.</given-names>
</name>
<name>
<surname>Fischer</surname>
<given-names>C. C.</given-names>
</name>
<name>
<surname>Persson</surname>
<given-names>K. A.</given-names>
</name>
<etal/>
</person-group> (<year>2011</year>). <article-title>Formation enthalpies by mixing GGA and GGA &#x2b; U calculations</article-title>. <source>Phys. Rev. B Condens. Matter</source> <volume>84</volume> (<issue>4</issue>), <fpage>045115</fpage>. <pub-id pub-id-type="doi">10.1103/physrevb.84.045115</pub-id> </citation>
</ref>
<ref id="B20">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jain</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Hautier</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Chen</surname>
<given-names>W.</given-names>
</name>
<name>
<surname>Richards</surname>
<given-names>W. D.</given-names>
</name>
<name>
<surname>Dacek</surname>
<given-names>S.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Commentary: the materials project: a materials genome approach to accelerating materials innovation</article-title>. <source>Appl. Mater.</source> <volume>1</volume> (<issue>1</issue>), <fpage>011002</fpage>. <pub-id pub-id-type="doi">10.1063/1.4812323</pub-id> </citation>
</ref>
<ref id="B21">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jain</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Chen</surname>
<given-names>W.</given-names>
</name>
<name>
<surname>Medasani</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Qu</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Kocher</surname>
<given-names>M.</given-names>
</name>
<etal/>
</person-group> (<year>2015</year>). <article-title>FireWorks: a dynamic workflow system designed for high-throughput applications</article-title>. <source>Concurr. Comput. Pract. Ex.</source> <volume>27</volume> (<issue>17</issue>), <fpage>5037</fpage>&#x2013;<lpage>5059</lpage>. <pub-id pub-id-type="doi">10.1002/cpe.3505</pub-id> </citation>
</ref>
<ref id="B22">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Kamaya</surname>
<given-names>N.</given-names>
</name>
<name>
<surname>Homma</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Yamakawa</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Hirayama</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Kanno</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Yonemura</surname>
<given-names>M.</given-names>
</name>
<etal/>
</person-group> (<year>2011</year>). <article-title>A lithium superionic conductor</article-title>. <source>Nat. Mater.</source> <volume>10</volume>, <fpage>682</fpage>&#x2013;<lpage>686</lpage>. <pub-id pub-id-type="doi">10.1038/nmat3066</pub-id> </citation>
</ref>
<ref id="B23">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Kiran</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Joseph</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2017</year>). <article-title>Atomate: a high-level interface to generate, execute, and analyze computational materials science workflows</article-title>. <source>Comput. Mater. Sci.</source> <volume>10</volume>, <fpage>64</fpage>. </citation>
</ref>
<ref id="B25">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Li</surname>
<given-names>W.</given-names>
</name>
<name>
<surname>Ando</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Minamitani</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Watanabe</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2017</year>). <article-title>Study of Li atom diffusion in amorphous Li3PO4 with neural network potential</article-title>. <source>J.&#x20;Chem. Phys.</source> <volume>147</volume> (<issue>21</issue>), <fpage>214106</fpage>. <pub-id pub-id-type="doi">10.1063/1.4997242</pub-id> </citation>
</ref>
<ref id="B27">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Richards</surname>
<given-names>W. D.</given-names>
</name>
<name>
<surname>Jain</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Hautier</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Kocher</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Cholia</surname>
<given-names>S.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Python Materials Genomics (pymatgen): a robust, open-source python library for materials analysis</article-title>. <source>Comput. Mater. Sci.</source> <volume>68</volume>, <fpage>314</fpage>&#x2013;<lpage>319</lpage>. <pub-id pub-id-type="doi">10.1016/j.commatsci.2012.10.028</pub-id> </citation>
</ref>
<ref id="B28">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Wang</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Kang</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Ceder</surname>
<given-names>G.</given-names>
</name>
</person-group> (<year>2008</year>). <article-title>Li&#x2013;Fe&#x2013;P&#x2013;O2 phase diagram from first principles calculations</article-title>. <source>Chem. Mater.</source> <volume>20</volume> (<issue>5</issue>), <fpage>1798</fpage>&#x2013;<lpage>1807</lpage>. <pub-id pub-id-type="doi">10.1021/cm702327g</pub-id> </citation>
</ref>
<ref id="B29">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Pan</surname>
<given-names>S. J.</given-names>
</name>
<name>
<surname>Yang</surname>
<given-names>Q.</given-names>
</name>
</person-group> (<year>2010</year>). <article-title>A survey on transfer learning</article-title>. <source>IEEE Trans. Knowl. Data Eng.</source> <volume>22</volume>, <fpage>1345</fpage>&#x2013;<lpage>1359</lpage>. <pub-id pub-id-type="doi">10.1109/TKDE.2009.191</pub-id> </citation>
</ref>
<ref id="B30">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Qu</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Jain</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Rajput</surname>
<given-names>N. N.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>The Electrolyte Genome project: a big data approach in battery materials discovery</article-title>. <source>Comput. Mater. Sci.</source> <volume>103</volume>, <fpage>56</fpage>&#x2013;<lpage>67</lpage>. </citation>
</ref>
<ref id="B31">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Rupp</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Tkatchenko</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>M&#xfc;ller</surname>
<given-names>K. R.</given-names>
</name>
<name>
<surname>von Lilienfeld</surname>
<given-names>O. A.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Fast and accurate modeling of molecular atomization energies with machine learning</article-title>. <source>Phys. Rev. Lett.</source> <volume>108</volume>, <fpage>058301</fpage>. <pub-id pub-id-type="doi">10.1103/PhysRevLett.108.058301</pub-id> </citation>
</ref>
<ref id="B32">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ryan</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Lengyel</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Shatruk</surname>
<given-names>M.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Crystal structure prediction via deep learning</article-title>. <source>J.&#x20;Am. Chem. Soc.</source> <volume>140</volume>, <fpage>10158</fpage>&#x2013;<lpage>10168</lpage>. <pub-id pub-id-type="doi">10.1021/jacs.8b03913</pub-id> </citation>
</ref>
<ref id="B33">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Saal</surname>
<given-names>J.&#x20;E.</given-names>
</name>
<name>
<surname>Kirklin</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Aykol</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Meredig</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Wolverton</surname>
<given-names>C.</given-names>
</name>
</person-group> (<year>2013</year>). <article-title>Materials design and discovery with high-throughput density functional theory: the open quantum materials database (OQMD)</article-title>. <source>JOM</source> <volume>65</volume> (<issue>11</issue>), <fpage>1501</fpage>&#x2013;<lpage>1509</lpage>. <pub-id pub-id-type="doi">10.1007/s11837-013-0755-4</pub-id> </citation>
</ref>
<ref id="B34">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sch&#xfc;tt</surname>
<given-names>K. T.</given-names>
</name>
<name>
<surname>Glawe</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Brockherde</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Sanna</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>M&#xfc;ller</surname>
<given-names>K. R.</given-names>
</name>
<name>
<surname>Gross</surname>
<given-names>E.</given-names>
</name>
<etal/>
</person-group> (<year>2014</year>). <article-title>How to represent crystal structures for machine learning: towards fast prediction of electronic properties</article-title>. <source>Phys. Rev. B</source> <volume>89</volume>, <fpage>205118</fpage>. <pub-id pub-id-type="doi">10.1103/physrevb.89.205118</pub-id> </citation>
</ref>
<ref id="B35">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sendek</surname>
<given-names>A. D.</given-names>
</name>
<name>
<surname>Cubuk</surname>
<given-names>E. D.</given-names>
</name>
<name>
<surname>Antoniuk</surname>
<given-names>E. R.</given-names>
</name>
<etal/>
</person-group> (<year>2018</year>). <article-title>Machine learning-assisted discovery of solid Li-ion conducting materials</article-title>. <source>Chem. Mater.</source> <volume>31</volume> (<issue>2</issue>), <fpage>3272</fpage>. <pub-id pub-id-type="doi">10.1021/acs.chemmater.8b03272</pub-id> </citation>
</ref>
<ref id="B36">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sendek</surname>
<given-names>A. D.</given-names>
</name>
<name>
<surname>Yang</surname>
<given-names>Q.</given-names>
</name>
<name>
<surname>Cubuk</surname>
<given-names>E. D.</given-names>
</name>
<etal/>
</person-group> (<year>2016</year>). <article-title>Holistic computational structure screening of more than 12,000 candidates for solid lithium-ion conductor materials</article-title>. <source>Energy Environ. Sci.</source> <volume>10</volume>, <fpage>1039</fpage>. <pub-id pub-id-type="doi">10.1021/acs.chemmater.8b03272</pub-id> </citation>
</ref>
<ref id="B38">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sendek</surname>
<given-names>A. D.</given-names>
</name>
<name>
<surname>Cubuk Ekin</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>van Antoniuk</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Cheon</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Cui</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Reed</surname>
<given-names>E. J.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Machine learning-assisted discovery of many new solid Li-ion conducting materials</article-title>. <source>Mater. Sci.</source> <volume>8</volume>, <fpage>750</fpage>. <pub-id pub-id-type="doi">10.1021/acs.chemmater.8b03272</pub-id> </citation>
</ref>
<ref id="B39">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sun</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Mindemark</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Edstr&#xf6;m</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Brandell</surname>
<given-names>D.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>Polycarbonate-based solid polymer electrolytes for Li-ion batteries</article-title>. <source>Solid State Ionics</source> <volume>262</volume>, <fpage>738</fpage>&#x2013;<lpage>742</lpage>. <pub-id pub-id-type="doi">10.1016/j.ssi.2013.08.014</pub-id> </citation>
</ref>
<ref id="B40">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Wang</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Richards</surname>
<given-names>W. D.</given-names>
</name>
<name>
<surname>Ong</surname>
<given-names>S. P.</given-names>
</name>
<name>
<surname>Miara</surname>
<given-names>L. J.</given-names>
</name>
<name>
<surname>Kim</surname>
<given-names>J.&#x20;C.</given-names>
</name>
<name>
<surname>Mo</surname>
<given-names>Y.</given-names>
</name>
<etal/>
</person-group> (<year>2015</year>). <article-title>Design principles for solid-state lithium superionic conductors</article-title>. <source>Nat. Mater.</source> <volume>14</volume>, <fpage>1026</fpage>&#x2013;<lpage>1031</lpage>. <pub-id pub-id-type="doi">10.1038/nmat4369</pub-id> </citation>
</ref>
<ref id="B41">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ward</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Liu</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Krishna</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Hegde</surname>
<given-names>V. I.</given-names>
</name>
<name>
<surname>Agrawal</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Choudhary</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Wolverton</surname>
<given-names>C.</given-names>
</name>
<etal/>
</person-group> (<year>2017</year>). <article-title>Including crystal structure attributes in machine learning models of formation energies via Voronoi tessellations</article-title>. <source>Phys. Rev. B</source> <volume>96</volume>, <fpage>024104</fpage>. <pub-id pub-id-type="doi">10.1103/physrevb.96.024104</pub-id> </citation>
</ref>
<ref id="B42">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Xiao</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Li</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Chen</surname>
<given-names>L.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Candidate structures for inorganic lithium solid-state electrolytes identified by high-throughput bond-valence calculations</article-title>. <source>J.&#x20;Materiom.</source> <volume>1</volume> (<issue>4</issue>), <fpage>235</fpage>. <pub-id pub-id-type="doi">10.1016/j.jmat.2015.08.001</pub-id> </citation>
</ref>
<ref id="B43">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Xie</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>Grossman</surname>
<given-names>J.&#x20;C.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Crystal graph convolutional neural networks for an accurate, and interpretable prediction of material properties</article-title>. <source>Phys. Rev. Lett.</source> <volume>120</volume> (<issue>14</issue>), <fpage>145301</fpage>. <pub-id pub-id-type="doi">10.1103/physrevlett.120.145301</pub-id> </citation>
</ref>
<ref id="B44">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Yamane</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Shibata</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Shimane</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Junke</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>Seino</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Adams</surname>
<given-names>S.</given-names>
</name>
<etal/>
</person-group> (<year>2007</year>). <article-title>Crystal structure of a superionic conductor, Li7P3S11</article-title>, <source>Solid State Ionics</source>. <volume>178</volume>, <fpage>1163</fpage>&#x2013;<lpage>1167</lpage>. <pub-id pub-id-type="doi">10.1016/j.ssi.2007.05.020</pub-id> </citation>
</ref>
<ref id="B45">
<citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname>Yang</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Pistorino</surname>
<given-names>J.&#x20;C.</given-names>
</name>
<name>
<surname>Pratt</surname>
<given-names>R. C.</given-names>
</name>
<name>
<surname>Eitouni</surname>
<given-names>H. B.</given-names>
</name>
</person-group> (<year>2017</year>). <source>Copolymers of peo and fluorinated polymers as electrolyte for lithium batteries</source>. <publisher-name>US</publisher-name>.</citation>
</ref>
<ref id="B46">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zeeshan</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Tian</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Chinmay</surname>
<given-names>M.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Machine learning enabled computational screening of inorganic solid electrolytes for suppression of dendrite formation in lithium metal anodes</article-title>. <source>ACS Cent. Sci. Acscentsci.</source> <volume>8</volume>, <fpage>996</fpage>&#x2013;<lpage>1006</lpage>. <pub-id pub-id-type="doi">10.1021/acscentsci.8b00229</pub-id> </citation>
</ref>
<ref id="B47">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhang</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Yue</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Hu</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Liu</surname>
<given-names>Z.</given-names>
</name>
<name>
<surname>Qin</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Zhang</surname>
<given-names>B.</given-names>
</name>
<etal/>
</person-group> (<year>2014</year>). <article-title>Taichi-inspired rigid-flexible coupling cellulose-supported solid polymer electrolyte for high-performance lithium batteries</article-title>. <source>Sci. Rep.</source> <volume>4</volume> (<issue>1</issue>), <fpage>6272</fpage>. <pub-id pub-id-type="doi">10.1038/srep06272</pub-id> </citation>
</ref>
<ref id="B48">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhang</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>He</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Chen</surname>
<given-names>Z.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Unsupervised discovery of solid-state lithium ion conductors</article-title>. <source>Nat. Commun.</source> <volume>10</volume>, <fpage>5260</fpage>. <pub-id pub-id-type="doi">10.1038/s41467-019-13214-1</pub-id> </citation>
</ref>
<ref id="B49">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhao</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>Daemen</surname>
<given-names>L. L.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Superionic conductivity in lithium-rich anti-perovskites</article-title>. <source>J.&#x20;Am. Chem. Soc.</source> <volume>134</volume> (<issue>36</issue>), <fpage>15042</fpage>&#x2013;<lpage>15047</lpage>. <pub-id pub-id-type="doi">10.1021/ja305709z</pub-id> </citation>
</ref>
<ref id="B50">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zheng</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Zheng</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Zhang</surname>
<given-names>R. Z.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Machine learning material properties from the periodic table using convolutional neural networks</article-title>. <source>Chem. Sci.</source> <volume>9</volume>, <fpage>8426</fpage>. <pub-id pub-id-type="doi">10.1039/c8sc02648c</pub-id> </citation>
</ref>
<ref id="B51">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhu</surname>
<given-names>Y.</given-names>
</name>
<name>
<surname>He</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Mo</surname>
<given-names>Y.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Origin of outstanding stability in the lithium solid electrolyte materials: insights from thermodynamic analyses based on first-principles calculations</article-title>. <source>ACS Appl. Mater. Interfaces</source>, <volume>7</volume>, <fpage>23685</fpage>&#x2013;<lpage>23693</lpage>. <pub-id pub-id-type="doi">10.1021/acsami.5b07517</pub-id> </citation>
</ref>
</ref-list>
</back>
</article>