TY - JOUR
T1 - Understanding diffraction patterns of glassy, liquid and amorphous materials via persistent homology analyses
AU - Onodera, Yohei
AU - Kohara, Shinji
AU - Tahara, Shuta
AU - Masuno, Atsunobu
AU - Inoue, Hiroyuki
AU - Shiga, Motoki
AU - Hirata, Akihiko
AU - Tsuchiya, Koichi
AU - Hiraoka, Yasuaki
AU - Obayashi, Ippei
AU - Ohara, Koji
AU - Mizuno, Akitoshi
AU - Sakata, Osami
N1 - Funding Information:
Acknowledgments The synchrotron radiation experiments were performed at BL04B2 of SPring-8 with the approval of the Japan Synchrotron Radiation Research Institute (JASRI) (Proposal Nos. 2016A0134, 2016A4502). This research was supported by JST PRESTO, Japan Grant Numbers JPMPR15N4 (to S.K.) and JPMJPR16N6 (to M.S.); the “Materials Research by Information Integration” Initiative (MI2I) project of the Support Program for Starting Up Innovation Hub from JST (to Y.O., S.K., A.M., S.T. and Y.H.); JST CREST 15656429 (to Y.H.); and JSPS KAKENHI Grant Numbers JP19K05648 (to Y.O.) and JP17H03121 (to A.M.). We thank Mr. T. Harada for experimental assistance in the high-energy XRD measurement on liquid silicon. Discussions with Profs. T. Otomo, T. Usuki, P. S. Salmon, L. Pusztai, and M. Watanabe and with Drs. K. Suzuya, M. Tucker, and A. Zeidler are gratefully appreciated. The authors are grateful to Prof. K. Amiya for providing Cu50Zr50 glass ribbons. Profs. S. Roorda, E. Bychkov, and S. Hosokawa and Drs. A. C. Hannon and Y. Katayama are thanked for providing us with the experimental diffraction data.
Publisher Copyright:
© 2019 The Ceramic Society of Japan. All rights reserved.
PY - 2019
Y1 - 2019
N2 - The structure of glassy, liquid, and amorphous materials is still not well understood, due to the insufficient structural information from diffraction data. In this article, attempts are made to understand the origin of diffraction peaks, particularly of the first sharp diffraction peak (FSDP, Q1), the principal peak (PP, Q2), and the third peak (Q3), observed in the measured diffraction patterns of disordered materials whose structure contains tetrahedral motifs. It is confirmed that the FSDP (Q1) is not a signature of the formation of a network, because an FSDP is observed in tetrahedral molecular liquids. It is found that the PP (Q2) reflects orientational correlations of tetrahedra. Q3, that can be observed in all disordered materials, even in common liquid metals, stems from simple pair correlations. Moreover, information on the topology of disordered materials was revealed by utilizing persistent homology analyses. The persistence diagram of silica (SiO2) glass suggests that the shape of rings in the glass is similar not only to those in the crystalline phase with comparable density (¡-cristobalite), but also to rings present in crystalline phases with higher density (¡-quartz and coesite); this is thought to be the signature of disorder. Furthermore, we have succeeded in revealing the differences, in terms of persistent homology, between tetrahedral networks and tetrahedral molecular liquids, and the difference/similarity between liquid and amorphous (glassy) states. Our series of analyses demonstrated that a combination of diffraction data and persistent homology analyses is a useful tool for allowing us to uncover structural features hidden in halo pattern of disordered materials.
AB - The structure of glassy, liquid, and amorphous materials is still not well understood, due to the insufficient structural information from diffraction data. In this article, attempts are made to understand the origin of diffraction peaks, particularly of the first sharp diffraction peak (FSDP, Q1), the principal peak (PP, Q2), and the third peak (Q3), observed in the measured diffraction patterns of disordered materials whose structure contains tetrahedral motifs. It is confirmed that the FSDP (Q1) is not a signature of the formation of a network, because an FSDP is observed in tetrahedral molecular liquids. It is found that the PP (Q2) reflects orientational correlations of tetrahedra. Q3, that can be observed in all disordered materials, even in common liquid metals, stems from simple pair correlations. Moreover, information on the topology of disordered materials was revealed by utilizing persistent homology analyses. The persistence diagram of silica (SiO2) glass suggests that the shape of rings in the glass is similar not only to those in the crystalline phase with comparable density (¡-cristobalite), but also to rings present in crystalline phases with higher density (¡-quartz and coesite); this is thought to be the signature of disorder. Furthermore, we have succeeded in revealing the differences, in terms of persistent homology, between tetrahedral networks and tetrahedral molecular liquids, and the difference/similarity between liquid and amorphous (glassy) states. Our series of analyses demonstrated that a combination of diffraction data and persistent homology analyses is a useful tool for allowing us to uncover structural features hidden in halo pattern of disordered materials.
KW - Amorphous materials
KW - Glass
KW - Liquid
KW - Neutron diffraction
KW - Persistent homology
KW - Structure
KW - Topology
KW - X-ray diffraction
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M3 - Article
AN - SCOPUS:85078028916
SN - 1882-0743
VL - 127
SP - 853
EP - 863
JO - Nippon Seramikkusu Kyokai Gakujutsu Ronbunshi/Journal of the Ceramic Society of Japan
JF - Nippon Seramikkusu Kyokai Gakujutsu Ronbunshi/Journal of the Ceramic Society of Japan
IS - 12
ER -