2012/11/30 by Mor Verbin, Oded Zilberberg, Yaacov E. Kraus +2 · 380 citations
Materials Science · Mathematics · Physics and Astronomy · #Algebraic structures and combinatorial models #Condensed matter physics #Fibonacci number #Gapless playback #Mathematics #Phase (matter) #Phase transition #Phason #Physics #Quantum #Quantum mechanics #Quasicrystal #Quasicrystal Structures and Properties #Topological Materials and Phenomena #Topological defect #Topological insulator #Topological order #Topology (electrical circuits) #cond-mat.mes-hall #physics.optics #quant-ph
paper · pdf · doi:10.1103/physrevlett.110.076403
published in Physical Review Letters 110(7), 076403 (American Physical Society) · 7 pages, 6 figures, 2 appendices
openalex publication_date 2013/02/14 · arxiv created 2013/02/15 · arxiv updated 2013/02/18 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Topological insulators and topological superconductors are distinguished by their bulk phase transitions and gapless states at a sharp boundary with the vacuum. Quasicrystals have recently been found to be topologically nontrivial. In quasicrystals, the bulk phase transitions occur in the same manner as standard topological materials, but their boundary phenomena are more subtle. In this Letter we directly observe bulk phase transitions, using photonic quasicrystals, by constructing a smooth boundary between topologically distinct one-dimensional quasicrystals. Moreover, we use the same method to experimentally confirm the topological equivalence between the Harper and Fibonacci quasicrystals.