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Figure 9
To explain the structure–property relations, a crystal structure S with infinitely many representations under isometry should be bijectively mapped by a complete and continuous invariant I to the space of invariants so that any image I(S) can be efficiently inverted back to a representative crystal [S\subset\mathbb{R}^{3}].

Volume 11| Part 4| July 2024| Pages 453-463
ISSN: 2052-2525