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. 2020 Mar 27;6(13):eaay5986. doi: 10.1126/sciadv.aay5986

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Copyright © 2020 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

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Fig. 5 — (A) Model highlighting the transformation of eight unit cells of BPII₍₁₀₀₎ (2 × 2 × 2) to BPI_{(110),−9.75°}. All the strain components are idealized values. (B) Four BPI₍₁₁₀₎ lattices, which can be transformed from single-crystalline BPII₍₁₀₀₎, and their strain values in global coordination after the transformation. (C) 64 × 64 single-crystalline BPII₍₁₀₀₎ and transformed 32 × 32 BPII_{(110),−9.75°}. (D) Representative twin 1 and twin 2 lamellae formation. (E) Idealized cross-hatched structure formation, which consists of twin 1 and twin 2 and actual cross-hatched structure of BPI₍₁₁₀₎ after the martensitic transformation (inset).