Mobile impurity in SSH model creates flat band of zero-energy topological bound states without boundaries when impurity is sufficiently heavy.
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4 Pith papers cite this work. Polarity classification is still indexing.
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Topological surface phonons in isostatic lattices with z=2d become finite-frequency surface phonons in superisostatic lattices with z>2d when next-nearest-neighbor springs or bending forces are added.
Magnetic barriers on monolayer WSe2 produce spin- and valley-dependent oscillatory Goos-Hänchen shifts and group delay times that can be tuned by field, energy, angle, and barrier width.
In an off-diagonal Aubry-André-Harper chain, transport signatures distinguish edge states, in-band bulk states, and band-edge bulk states by their system-size dependence, resonance broadening, and dephasing sensitivity.
citing papers explorer
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Flat band of topological states bound to a mobile impurity
Mobile impurity in SSH model creates flat band of zero-energy topological bound states without boundaries when impurity is sufficiently heavy.
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Signatures of Topological Phonons in Superisostatic Lattices
Topological surface phonons in isostatic lattices with z=2d become finite-frequency surface phonons in superisostatic lattices with z>2d when next-nearest-neighbor springs or bending forces are added.
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Magnetic control of Goos-H\"anchen shifts and group delay time in monolayer WSe$_2$
Magnetic barriers on monolayer WSe2 produce spin- and valley-dependent oscillatory Goos-Hänchen shifts and group delay times that can be tuned by field, energy, angle, and barrier width.
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Transport characteristics of bulk and edge states in an off-diagonal Aubry--Andr\'e--Harper chain
In an off-diagonal Aubry-André-Harper chain, transport signatures distinguish edge states, in-band bulk states, and band-edge bulk states by their system-size dependence, resonance broadening, and dephasing sensitivity.