Non-Bloch Dirac Points and Phase Diagram in the Stacked Non-Hermitian SSH Model.
ORAL
Abstract
Topological semimetals exhibit protected band crossings in momentum space with
corresponding surface states. Non-Hermitian Hamiltonians introduce geometry-sensitive features
that dissolve this bulk-boundary correspondence principle. In this talk, we exemplify this by
showing a non-Hermitian 2D stacked SSH chain model with non-reciprocal on-site gain/loss. We
obtain an analytical phase diagram of its complex spectrum under open boundary conditions. We
reveal that the model can exhibit non-Bloch Dirac points, which only appears under open
boundary conditions but disappear in Bloch bands under periodic boundary conditions. Due to
the reality of spectrum in the vicinity of non-Bloch Dirac points, we can map it to Hermitian
band crossings within the Altland-Zirnabuer symmetry classes. Based on this mapping, we
demonstrate that non-Bloch Dirac points are characterized by the integer topological charge.
Moreover, the locations of the non-Bloch Dirac points under different boundary geometries do
not match with each other, indicating the breakdown of bulk-boundary correspondence in non-
Hermitian semimetals. Our findings provide new insights into establishing unconventional bulk-
boundary correspondence for non-Bloch Dirac metals in non-Hermitian systems.
corresponding surface states. Non-Hermitian Hamiltonians introduce geometry-sensitive features
that dissolve this bulk-boundary correspondence principle. In this talk, we exemplify this by
showing a non-Hermitian 2D stacked SSH chain model with non-reciprocal on-site gain/loss. We
obtain an analytical phase diagram of its complex spectrum under open boundary conditions. We
reveal that the model can exhibit non-Bloch Dirac points, which only appears under open
boundary conditions but disappear in Bloch bands under periodic boundary conditions. Due to
the reality of spectrum in the vicinity of non-Bloch Dirac points, we can map it to Hermitian
band crossings within the Altland-Zirnabuer symmetry classes. Based on this mapping, we
demonstrate that non-Bloch Dirac points are characterized by the integer topological charge.
Moreover, the locations of the non-Bloch Dirac points under different boundary geometries do
not match with each other, indicating the breakdown of bulk-boundary correspondence in non-
Hermitian semimetals. Our findings provide new insights into establishing unconventional bulk-
boundary correspondence for non-Bloch Dirac metals in non-Hermitian systems.
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Presenters
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Megan Schoenzeit
University of Minnesota
Authors
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Megan Schoenzeit
University of Minnesota
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Chang Shu
University of Michigan
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Kai Zhang
University of Michigan
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Kai Sun
University of Michigan