Abstract
The structural origin of the slow dynamics in glass formation remains to be understood owing to the subtle structural differences between the liquid and glass states. Even from simulations, where the positions of all atoms are deterministic, it is difficult to extract significant structural components for glass formation. In this study, we have extracted significant local atomic structures from a large number of metallic glass models with different cooling rates by utilising a computational persistent homology method combined with linear machine learning techniques. A drastic change in the extended range atomic structure consisting of 3–9 prismtype atomic clusters, rather than a change in individual atomic clusters, was found during the glass formation. The present method would be helpful towards understanding the hierarchical features of the unique static structure of the glass states.
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Introduction
Glass states are generally formed owing to an abrupt increase in their viscosity upon cooling from the liquid states^{1,2,3,4,5}. It is known that they are far from the equilibrium states owing to their long relaxation times that cannot be achieved experimentally. Naturally, the formation of glass states strongly depends on their thermal history, i.e. the cooling rate from the molten liquid to glass^{6}. A glass state formed at a slower cooling rate should be more stable, and therefore, closer to the ideal glass state. In general, there is no distinct difference between the atomicscale structures in the liquid and glass states where only several broad peaks, which indicate a disordered structure, are found in their structure factors, although the spatial heterogeneity of their dynamics increases during glass formation^{7,8}. It is even more difficult to distinguish between the different glass states formed at different cooling rates in terms of their static structures. Therefore, the development of analytical methodologies that can reveal the hidden structural features in disordered states such as liquid and glass is required.
For a long time, the cooling rate dependency of glass structures has primarily been examined using molecular dynamics simulations^{9,10,11,12,13,14}. Molecular dynamics simulation is a powerful tool that provides a complete set of information of all the experimentally inaccessible atomic positions. A slight structural difference between the glass states simulated by molecular dynamics with faster and slower cooling rates has been observed through a Voronoi polyhedral analysis^{12,13} or a bondorientational order analysis^{14}. In the case of densely packed structures, e.g. a fraction of the icosahedrallike clusters decreases with decreasing cooling rate when using the LennardJones potential^{9}, whereas this fraction increases when using the embedded atom method potentials^{13}. However, the structure units strongly depend on the glass systems, and therefore, the essential structures for glass formation still remain unclear. Furthermore, it is difficult to elucidate the structural features beyond a short range even when using the pair distribution function (PDF) and Voronoi polyhedral analyses.
A computational persistent homology method has been developed as a tool for analysing the topological features of threedimensional objects in the 2000s^{15}. This method is useful for surveying complicated objects such as glass structures and has already been applied to the structural analysis of oxide and metallic glasses^{16,17,18}. It is possible to visualise the hierarchical features of glass structures via persistence diagrams by detecting the creation and annihilation of holes with changing atomic size. In this study, we applied the persistent homology technique to the analysis of metallic glass structures prepared at different cooling rates and obtained the persistence diagrams for each model. The statistical features of the persistence diagrams were further analysed using machine learning techniques. Machine learning techniques can be useful to search for and extract important information from persistence diagrams. Both important and unimportant information are often mixed in the diagrams, and it is difficult to intuitively identify the important information from the diagrams. The combination of machine learning and persistent homology provides a systematic way to find important geometric patterns hidden behind the data.
In this work, typical local structures related to glass formation were extracted from molecular dynamics simulations through the inverse analysis of persistence diagrams using a combination of linear machine learning models, such as principal component analysis (PCA) and linear regression analysis (LRA)^{19,20}. We demonstrate that the persistence diagram/machine learning analysis is a powerful tool to statistically extract the significant extended range local structures of glasses that strongly depend on cooling rates. Consequently, we suggest the changes in extended range local structures including 3–9 prismtype clusters, rather than individual clusters, play a key role in the glass formation.
Results
Structure models prepared by molecular dynamics simulation
The structure models prepared using molecular dynamics simulations in this study are summarised in Fig. 1. For LRA, a model each for 37 different cooling rates (from 1.7 × 10^{10} to 1.7 × 10^{14} K s^{−1}) was prepared. Separately, 30 models each for five different cooling rates (1.7 × 10^{10}, 1.7 × 10^{11}, 1.7 × 10^{12}, 1.7 × 10^{13} and 1.7 × 10^{14} K s^{−1}) were constructed for PCA. Note that the term “structure model” represents a snapshot in a molecular dynamics trajectory. Each model includes 12,000 atoms in total (9600 Pd atoms and 2400 Si atoms). The structure factors of these molecular dynamics models are consistent with the reported diffraction experiments (Supplementary Fig. S1). For the Pd_{80}Si_{20} models used in this study, all Si atoms were surrounded by Pd atoms. In other words, there are no nearest neighbour Si–Si bonds, as indicated by the PDF (Supplementary Fig. S2) and Voronoi polyhedral analyses (Supplementary Fig. S3). The shortrange structures are characterised by Sicentred prismtype clusters indexed by, for example, <0 3 6 0>, <0 4 4 0>, <0 5 4 0>, <0 2 8 0> and <0 3 6 1>, which are consistent with previous studies^{21,22}. In order to understand the features of the prismtype clusters and their arrangements, we calculated the persistence diagrams for models excluding all Si atoms or all Pd atoms (Fig. 1c, d).
Persistent homology analyses
Figure 2a, b shows PD2 for Pd atoms, while Fig. 2c, d shows the PD1 for Si atoms, obtained from the molecular dynamics structure models formed at the slowest and fastest cooling rates (1.7 × 10^{10} and 1.7 × 10^{14} K s^{−1}, respectively). Here, PD2 and PD1 denote the persistence diagrams for the second and first homologies, respectively. The PD2 provides information about a closed hole usually called a void or pore, whereas the PD1 corresponds to an open hole such as a ring or tube. The details regarding the persistence diagrams are described in the literature^{17}. Each persistence diagram is averaged over 30 models, each including 12,000 atoms. The horizontal axis in the persistence diagrams represents the birth time, i.e., when a hole is generated, while the vertical axis represents the death time, i.e., when an identical hole is annihilated. The characteristic islands found in PD2 for Pd atoms (indicated by arrows in Fig. 2a, b) correspond to prismtype atomic clusters, which is demonstrated by the PD2 for individual prismtype atomic clusters shown in Supplementary Fig. S4. The PD1 for Si atoms (Fig. 2c, d), which represent the spatial arrangements of Sicentred prism clusters, are characterised by two horns perpendicular to the horizontal birth axes. Note that the Sicentred local structures most likely belong to primstype atomic clusters (65–70% atomic clusters belong to <0 3 6 0>, <0 4 4 0>, <0 5 4 0>, <0 2 8 0>, and <0 3 6 1>) based on the statistics of Voronoi polyhedral analysis (Supplementary Fig. S3). In addition, it is understood that the surrounding atoms of prismtype atomic clusters are only Pd atoms based on the partial PDFs (Supplementary Fig. S2) as mentioned above. Thus, the structural features of the prismtype atomic clusters and their spatial arrangements can be basically understood from PD2 for Pd atoms and PD1 for Si atoms, respectively.
Machine learning analyses
To investigate the cooling rate dependence of the persistence diagrams, we first conducted an LRA of the molecular dynamics models prepared at 37 different cooling rates (Fig. 1a). The persistence diagrams obtained from 37 molecular dynamics atomic configurations were calculated and divided into N regions (bins), each containing birth–death pairs corresponding to the detected holes. The numbers of birth–death pairs for N regions were smoothed by a Gaussian filter and then converted into Ndimensional vectors as input data for the LRA. In this case, the N values for the persistence diagrams of the Pd and Si configurations were approximately 12,000 and 7500, respectively. Linear relationships between the number of birth–death pairs for each region and the cooling rate were modelled using LRA. This analysis enables us to determine the cooling rate dependence of each region in the persistence diagrams. The persistence diagrams indicating degrees of dependence on the cooling rate were finally reconstructed using the learned vectors. Figure 3a, b shows the persistence diagrams reconstructed by the learned vectors of Pd and Si atoms from PD2 and PD1, respectively. The colour levels in the persistence diagrams indicate the magnitude of the influence of the cooling rates. The characteristic structures for the slower and fastercooled models are contained in the darker blue and red regions of the persistence diagrams, respectively. The locations of the blue regions are clearly different from those of the red regions, indicating that the local structures strongly depend on the cooling rate. Similarly, we further performed PCA for 30 molecular dynamics models at five different cooling rates (Fig. 1b). The 30 atomic configurations, each for five different cooling rates, were converted into vectors as input files for PCA. The vectorization procedure was the same as in the case of LRA. The Ndimensional vectors, where N is the number of birth–death pairs for each region, were then analysed by PCA and reduced to twodimensional projections with respect to the first and second principal components. Note that the first principal component most properly explains the dispersion of the input data. Eventually, the first principal component becomes strongly dependent on the cooling rate, as mentioned below. The persistence diagrams were also reconstructed using the learned vectors by PCA. Figure 3c, d shows the projections of the persistence diagrams on the first and second principal component planes, respectively. Total 150 data (30 molecular dynamics models × 5 cooling rates) are plotted on the projected planes and different colours are assigned to each cooling rate. Clustering of the data points is seen at each cooling rate, and the clusters are observed to be aligned along the horizontal axis. It is apparent that the first principal components strongly correlate with the cooling rates, while the second principal components are almost independent of them. The learned vectors from the first principal components of PCA were also drawn on the reconstructed persistence diagrams, as shown in Fig. 3e, f. Interestingly, the locations of both the blue and red regions in the persistence diagrams of PCA coincide with those in the persistence diagrams of LRA. Thus, it is reasonable to state that the first principal component of PCA also represents the structures depending on the cooling rates. The molecular dynamics datasets for PCA are much more statistically warranted than those for LRA, and therefore, are more suitable for extracting specific local structures.
In order to understand the origin of the signals in the persistence diagrams, local atomic structures from the persistence diagrams were extracted through an inverse analysis process. The structural information of the original molecular dynamics models is initially recorded to the persistence diagrams together with birth–death pairs when computing persistence diagrams. After the machine learning analyses, a local structure corresponding to each birth–death pair can be mathematically reconstructed from the recorded structural information using the inverse analysis process. Figure 4a, b illustrates the prismtype clusters extracted from the central parts of the dark blue region ([1.79, 1.80]_{birth} × [2.43, 2.44]_{death}) corresponding to the slowestcooled sample and the dark red region ([1.89, 1.90]_{birth} × [2.44, 2.45]_{death}) corresponding to the fastestcooled sample, respectively, in Fig. 3e. The area of each face of the prismtype clusters is shown by a different colour and thus, the degree of distortion in these clusters can be immediately known based on their colour. The statistical distribution of the areas of the faces is also shown in Fig. 4c. The distributions for the area of a triangle face were statistically analysed for 710 and 435 atomic clusters in the slowest and fastestcooled samples, respectively. The distribution for the slowestcooled sample appears to be sharper than that for the fastestcooled sample, indicating that the prismtype clusters in the fastestcooled sample are more distorted than those in the slowestcooled sample, although the difference is not large.
The Si networks related to the framework of the arrangement of the prismtype clusters were also extracted from the reconstructed persistence diagrams of Fig. 3f. The change in the Si network is more prominent than that in individual prismtype atomic clusters. Typical arrangements of Si atoms with prismtype clusters (referred to as superclusters) in the slowestcooled and fastestcooled samples are depicted in Fig. 4d, e, respectively. Ordered structures consisting of some prisms (3–4 prisms) connected at their vertices are extracted from the dark blue region ([2.38, 2.40]_{birth} × [2.70, 2.72]_{death}) in the reconstructed persistence diagram of Fig. 3f and are frequently observed, especially in the slowestcooled sample (Fig. 4d). In contrast, in the fastestcooled sample, the number of units consisting of several prisms (extracted from the dark red region ([2.01, 2.05]_{birth} × [3.07, 3.11]_{death}) in the reconstructed persistence diagram of Fig. 3f), is much larger (5–9 prisms), as shown in Fig. 4e. We also calculated the histograms of the numbers of atoms constituting the superclusters for both samples, as shown in Fig. 4f. The distributions were statistically analysed for 460 and 358 atomic configurations in the slowest and fastestcooled samples, respectively. The extent of superclusters for the fastestcooled sample is much larger than that for the slowestcooled sample, indicating that slower cooling leads to the formation of compact units of prismtype clusters. The structural features of the superclusters will be discussed later.
Conventional pair distribution function and Voronoi polyhedral analyses
The Pd–Pd, Pd–Si and Si–Si partial PDFs of molecular dynamics models formed with cooling rates of 1.7 × 10^{10}, 1.7 × 10^{11}, 1.7 × 10^{12}, 1.7 × 10^{13} and 1.7 × 10^{14} K s^{−1} are shown in Supplementary Fig. S2. The profiles for Pd–Pd and Pd–Si pairs do not show any clear differences, whereas subtle changes can be observed in the profiles of the Si–Si pair. This implies that the shorterrange structures remain largely unchanged with respect to pair correlation, although some differences in distortion were detected in the present persistence diagram analyses (Fig. 4a, b). The subtle change in the Si–Si partial PDFs should be related to the drastic rearrangement of the prismtype clusters (Fig. 4c, d). The Voronoi polyhedral analyses were also performed for molecular dynamics models formed with the five different cooling rates (Supplementary Fig. S3). Although there are some subtle differences due to cooling rates, it was hard to find systematic structural changes from the lists of Voronoi indices and also extract extended range structural changes beyond the nearest neighbour environment. Thus, our persistence diagram analyses have a higher sensitivity in detecting structural changes in disordered structures compared to conventional PDF and Voronoi polyhedral analyses.
Discussion
To understand the extracted local structures shown in Fig. 4, we calculate “local” structure factors S(Q) for those structures and compare them with the experimental S(Q) curve obtained by neutron scattering^{23}, as shown in Fig. 5. The experimental S(Q) curve possesses a characteristic second peak splitting, which is generally recognized as a feature of glass structures. The local S(Q) curves obtained from the superclusters (3–4 prisms) frequently found in the slowestcooled model also exhibit similar second peak splitting (Fig. 5a), whereas the curves of the local structures (5–9 prisms) in the fastestcooled model do not (Fig. 5b). This fact implies that the superclusters formed in the slowestcooled model largely contribute to the experimentally observable structural feature of the glass state. In other words, the formation of the superclusters presumably induces the development of a glassy structural order. Although the cooling rate for real glass is beyond the range of molecular dynamics simulations, it is expected that the volume fraction of the superclusters will increase by further decreasing the cooling rate.
As mentioned above, the persistence diagram/PCA analyses enable us to extract changes in the static local structures, particularly those related to the cooling rate. Beyond the local structure changes estimated from this work, there could be a hypothetical ideal glass that corresponds to an inherent structure in the energy landscape description. By obtaining a thorough dataset, it might be possible to predict the plot positions generated by the ideal glass structure on the persistence diagram by LRA. It is presumed that the ideal glass structure is mostly filled with unique noncrystalline local structures without any longrange order. A candidate of such local structures could be a triangular configuration of vertexsharing lessdistorted prisms (Fig. 4c), as found mainly in the slowly cooled models in the present work, which are different from other related crystal structures such as Pd_{9}Si_{2} and Pd_{3}Si (Supplementary Fig. S5).
We have combined a persistent homology analysis with machine learning techniques such as PCA and LRA, to analyse the coolingrate dependence of the atomic structural order of Pd–Si metallic glasses. Persistent homology analysis enables us to survey the threedimensional structural features from short to extendedranges based on the distributions visualised via persistence diagrams. The machine learning techniques were able to deduce the core local atomic structures that are strongly correlated to the cooling rates of liquidtoglass transitions. In other words, from the analyses, it is possible to extract the essential features in the static structures during glass formation. In the present case, we found a drastic change in the extended range atomic structure, which corresponds to the spatial arrangement of the prismtype clusters, rather than to a change in individual atomic clusters during glass formation. In particular, the extended range atomic structures with 5–9 atomic clusters leading to larger holes in the persistence diagrams of Si atoms are dominant in the sample cooled rapidly, whereas those with 3–4 atomic clusters (superclusters) leading to smaller holes become more prominent in the sample cooled more slowly. It should be noted that the latter superclusters largely contribute to the second peak splitting in S(Q), which is known as a feature of glass structures, thereby inducing a glassy structural order. In the future, we will apply the present techniques to different types of glass in order to gain a deeper insight into general trends.
Methods
Molecular dynamics simulation
Models of amorphous Pd_{80}Si_{20} alloys were constructed using molecular dynamics methods. The embedded atom method potentials developed by Sheng (https://sites.google.com/site/eampotentials/) were employed for the simulations. Molecular dynamics simulations were performed under constant isothermicisobaric (NPT) conditions using a LAMMPS Molecular Dynamics Simulator^{24}. First, 9600 Pd and 2400 Si atoms were prepared randomly in cubic molecular dynamics cells with periodic boundary conditions. The initial configurations were kept at 2500 K for more than 50 ps and then cooled to 300 K at different cooling rates (1.7 × 10^{10}–1.7 × 10^{14} K s^{−1}). For stabilisation, the cooled models were further kept at 300 K for 125 ps. The system temperature and pressure were controlled using a Nose–Hoover thermostat and a Nose–Hoover barostat, respectively.
Computational homology analysis
A unified method proposed by Obayashi et al.^{25,26}, which combines a linear machine learning method for persistence images with an inverse analysis method, was adopted in this study. The outline is as follows:

1.
Persistence diagrams were computed from molecular dynamics simulation datasets with ith homology, where i = 1 and 2 for Si and Pd, respectively.

2.
The diagrams were converted into vectors using the persistence image, a technique proposed by Adams et al.^{27}

3.
Linear regression analysis and principal component analysis were applied to the vectors. L2 regularisation was used for the regression analysis. As a result, we obtained the optimal coefficients and eigenvalues as dual vectors for each analysis.

4.
The persistence diagrams were reconstructed using the learned vectors. The important regions that contain a high contribution of the eigenvalues were drawn on the diagrams. From the diagrams, the birth–death pairs for the characteristic holes or cavities were extracted.

5.
The geometric structures were extracted from the original atomic configuration by carrying out explicit inverse analysis of the pairs.
Here, we utilised the data analysis software “HomCloud” (https://homcloud.dev/index.en.html) based on persistent homology in order to compute the persistence diagrams, carry out vectorisation of the diagrams, and solve the inverse problem. We also used Python’s scikitlearn to implement the linear learning method (http://scikitlearn.org/).
In order to compute the histograms from the persistence diagrams, the targeted regions were clipped into rectangles using [1.2, 2.6] × [1.4, 2.8] and [1.8, 4.0] × [2.1, 4.3] windows and were then divided into 140 × 140 and 110 × 110 boxes for Pd and Si, respectively. The clipped regions were chosen to contain all the cells having values more than zero on the persistence diagrams, and the widths of the grids were chosen such that they reproduced the detailed patterns schematically.
Machine learning
To apply LRA and PCA, we converted the histograms into persistence image vectors. The hyper parameters for vectorisation were taken to be (σ, c, p) = (0.02, 1.0, 1.0) for Pd and (σ, c, p) = (0.04, 1.0, 1.0) for Si. Here, σ indicates the standard deviation and c and p are the parameters of the weight function^{26}. We applied Ridge regularisation (L2 regularisation) for the linear regression analysis. The regularisation parameter was set to 200 to simplify the learned result and to avoid overfitting. We also checked these results using LASSO (L1 regularisation). However, the vectors thus obtained were too sparse to extract a sufficient number of characteristic structures from the original datasets.
The abovementioned parameters were tuned to not only obtain a better R^{2} score for LRA and contribution ratio for PCA, but also to obtain the monophasic peaked reconstructed persistence diagrams from the learned vectors for analysis. In other words, complicated structures of the reconstructed persistence diagrams were not preferred to interpret the result of the inverse analysis. The R^{2} score and contribution ratio of 0.509 and 0.754 for the second homology of Pd and 0.549 and 0.675 for the first homology of Si, respectively, were obtained.
Under the above setting, for the final calculations, we defined the regions on the persistence diagrams that contributed the most to the cooling rate, namely, [1.79, 1.80] × [2.43, 2.44] for the slowest cooling rate and [1.89, 1.90] × [2.44, 2.45] for the fastest cooling rate for Pd with the second homology; likewise, [2.38, 2.40] × [2.70, 2.72] and [2.01, 2.05] × [3.07, 3.11] for Si with the first homology. We extracted 460 and 358 rings as the structures contributing most to the slowest and fastest cooling rates, respectively, for Si, and 710 and 435 cavities, respectively, for Pd.
Data availability
All datasets are available from the corresponding author upon reasonable request.
Code availability
The opensource HomCloud code used in this work is available on the following link: https://homcloud.dev/index.en.html.
References
Debenedetti, P. G. & Stillinger, F. H. Supercooled liquids and the glass transition. Nature 410, 259–267 (2001).
Stillinger, F. H. A topographic view of supercooled liquids and glassformation. Science 267, 1935–1939 (1995).
Stillinger, F. H. Supercooled liquids, glass transitions, and the Kauzmann paradox. J. Chem. Phys. 88, 7818–7825 (1988).
Ediger, M. D., Angell, C. A. & Nagel, S. R. Supercooled liquids and glasses. J. Phys. Chem. 100, 13200–13212 (1996).
Ediger, M. D. & Harrowell, P. Perspective: supercooled liquids and glasses. J. Chem. Phys. 137, 0809011–08090115 (2012).
Jund, P., Caprion, D. & Jullien, R. Is there an ideal quenching rate for an ideal glass? Phys. Rev. Lett. 79, 91–94 (1997).
Ediger, M. D. Spatially heterogeneous dynamics in supercooled liquids. Ann. Rev. Phys. Chem. 51, 99–128 (2000).
Glotzer, S. C. Spatially heterogeneous dynamics in liquids: insights from simulation. J. Noncryst. Solids 274, 342–355 (2000).
Vollmayr, K., Kob, W. & Binder, K. How do the properties of a glass depend on the cooling rate? A computer simulation study of a LennardJones system. J. Chem. Phys. 105, 4714–4728 (1996).
Vollmayr, K., Kob, W. & Binder, K. Coolingrate effects in amorphous silica: a computersimulation study. Phys. Rev. B. 54, 15808–15827 (1996).
Buchholz, J., Paul, W., Varnik, F. & Binder, K. Cooling rate dependence of the glass transition temperature of polymer melts: molecular dynamics study. J. Chem. Phys. 117, 7364–7372 (2002).
Li, M., Wang, C. Z., Hao, S. G., Kramer, M. J. & Ho, K. M. Structural heterogeneity and mediumrange order in Zr_{x}Cu_{100x} metallic glasses. Phys. Rev. B 80, 1–7 (2009).
Cheng, Y. Q., Sheng, H. W. & Ma, E. Relationship between structure, dynamics, and mechanical properties in metallic glassforming alloys. Phys. Rev. B 78, 0142071–0142077 (2008).
Ryltsev, R. E., Klumov, B. A. & Chtchelkatchev, N. M. Cooling rate dependence of simulated Cu_{64.5}Zr_{35.5} metallic glass structure. J. Chem. Phys. 145, 0345061–03450610 (2016).
Edelsbrunner, H., Letscher, D. & Zomorodian, A. Topological persistence and simplication. Discrete Comput. Geom. 28, 511–533 (2002).
Hirata, A. et al. Geometric frustration of icosahedron in metallic glasses. Science 341, 376–379 (2013).
Hiraoka, Y. et al. Hierarchical structures of amorphous solids characterized by persistent homology. Proc. Natl Acad. Sci. USA 113, 7035–7040 (2016).
Hirata, A. Matsue, K. & Chen, M. W. in Structural Analysis of Metallic Glasses with Computational Homology, Vol. 2 (SpringerBriefs in the Mathematics of Materials, Springer, 2016).
Dey, T., Hirani, A. N. & Krishnamoorthy, B. Optimal homologous cycles, total unimodularity, and linear programming. SIAM J. Comput. 40, 1026–1044 (2011).
Escolar, E. G. & Hiraoka, Y. in Optimization in the Real World Towards Solving Real World Optimization Problems (eds Fujisawa, K., Shinano, Y. & Waki, H.), 79–96 (Springer, Tokyo, 2015).
Durandurdu, M. Ab initio modelling of metallic Pd_{80}Si_{20} glass. Comput. Mater. Sci. 65, 44–47 (2012).
Adjaoud, O. & Albe, A. Interfaces and interphases in nanoglasses: surface segregation effects and their implications on structural properties. Acta Mater 113, 284–292 (2016).
Fukunaga, T. & Suzuki, K. Radial distribution functions of PdSi alloy glasses by pulsed neutron total scattering measurements and geometrical structure relaxation simulations. Sci. Rep. Res. Inst. Tohoku Univ. 29, 153–175 (1980).
Plimpton, S. Fast parallel algorithms for shortrange molecular dynamics. J. Comp. Phys. 117, 1–19 (1995).
Obayashi, I. Volumeoptimal cycle: tightest representative cycle of a generator in persistent homology. SIAM J. Appl. Algebra Geometry 2, 508–534 (2018).
Obayashi, I., Hiraoka, Y. & Kimura, M. Persistence diagrams with linear machine learning models. J. Appl. Comput. Topology 1, 421–449 (2018).
Adams, H. et al. Persistence images: a stable vector representation of persistent homology. J. Mach. Learn. Res. 18, 1–35 (2017).
Acknowledgements
This work was partially sponsored by the Fusion Research Funds from the “World Premier International (WPI) Research Center Initiative for Atoms, Molecules and Materials” programme of MEXT of Japan, the GrantinAid for Scientific Research (A) (No. 17H01325, 19H00834, 20H00119) and the GrantinAid for Young Scientists (B) (No. 16K17638, 20H04241) from Japan Society for the Promotion of Science (JSPS), JST CREST Mathematics (15656429), JST MIRAI Programme (JPMJMI18G3), JST PRESTO (JPMJPR1923), Crossministerial Strategic Innovation Promotion Programme (SIP, Structural Materials for Innovation D72) of the Ministry of Agriculture, and the New Energy and Industrial Technology Development Organization (NEDO). This work was also supported by Council for Science, Technology and Innovation (CSTI), Crossministerial Strategic Innovation Promotion Programme (SIP) and “Materials Integration” for revolutionary design system of structural materials (Funding agency: JST).
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A.H. conceived the study, performed molecular dynamics simulations and analyses. T. W., I.O. and Y.H. developed and conducted computational homology analyses. A.H. wrote the manuscript, and all authors discussed the results and commented on the manuscript.
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Hirata, A., Wada, T., Obayashi, I. et al. Structural changes during glass formation extracted by computational homology with machine learning. Commun Mater 1, 98 (2020). https://doi.org/10.1038/s43246020001003
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DOI: https://doi.org/10.1038/s43246020001003
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