Multi-fold EP protected by anti-unitary symmetry

Multi-fold EP protected by anti-unitary symmetry

Generic degeneracy of a non-hermitian hamiltonian implies a set of the eigenvectors is not enough to span the total linear space. One needs to extend the idea of the eigenstates to the generic ones, w...
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3D HOTI of Hubbard model by  negative sign free quantum Monte Carlo

3D HOTI of Hubbard model by negative sign free quantum Monte Carlo

Corner states of the breezing Pyrochlore lattice are protected by the Z4 symmetry as a typical example of the bulk-edge/boundary correspondence using Z4 Berry phase. With on-site Coulomb interaction, ...
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Bulk-edge correspondence of interacting bosonic pump

Bulk-edge correspondence of interacting bosonic pump

Topological (adiabatic) pumps are typical problems where the bulk-edge correspondence is justified. The Chern number of the bulk and the behavior of the edge states are linked intimately. As for most ...
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Hofstadter’s butterfly and TKNN integers

Hofstadter’s butterfly and TKNN integers

Hofstadter's butterfly & TKNN integers (Chern numbers)
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Non real energies for Hermitian problems

Non real energies for Hermitian problems

Eigenvalues may not be always real for generalized eigenvalue problems even if the Hamiltonian and overlap matrices are both Hermitian. When the overlap is associated with a norm of physical state, th...
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Multiple quantum scars and dynamics

Multiple quantum scars and dynamics

A flat band system with interaction that possesses a single "quantum scar", which we have proposed in Kuno-Mizoguchi-Hatsugai, Phys. Rev. B 102, 241115(R) (2020), is extended to a system with multiple...
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One more topological phase with chiral edge states

One more topological phase with chiral edge states

Bulk-edge correspondence is universal. We do find a novel playground of the chiral edge states protected by bulk topology. It is in the evolutionary game theory realized in a kagome network. The paper...
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Flat bands of COF/MOF in any dimension

Flat bands of COF/MOF in any dimension

Covalent/Metal-organic framework (COF/MOF) is a 2D/3D network compound of organic molecules (linkages) connected by linker molecules. This material possesses a set of flat bands (at least in a tight-b...
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Flat bands and spin-1 Dirac cone

Flat bands and spin-1 Dirac cone

We are proposing one more lattice structure with frustration that hosts flat bands, square-Kagome lattice. Using a molecular orbital representation, its flat band and flat dispersion only in some spec...
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Reduction of non-hermitian topology in 0-D

Reduction of non-hermitian topology in 0-D

Many body interactions may modify the topology of physical systems. We have discussed it for a simple 0-D system with non-hermitian hamiltonian. Have a look at our recent paper, "Correlation effects o...
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Non-real energies in  real world

Non-real energies in real world

Our paper on non-real things has been picked up by JPS Hot Topics. It's real.
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Plateau transitions of quantum spin chain

Plateau transitions of quantum spin chain

Quantum mechanics tells us particles are waves at the same time. One may then naively expect that the quantum state is extended, especially with translational invariance. However, it is not always tru...
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Symmetries and square-root operations

Symmetries and square-root operations

Motivated by the relation between the Dirac/Schrodinger hamiltonians, the square root topological phase (SRTI) has been discussed in several cases recently. Here the roles of symmetries in SRTI are fo...
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Square-root topological semimetals

Square-root topological semimetals

We propose topological semimetals generated by the square-root operation for tight-binding models in two and three dimensions, which we call square-root topological semimetals. The square-root topolog...
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Bulk-edge correspondence with generalized chiral symmetry

Bulk-edge correspondence with generalized chiral symmetry

Dirac cones are generically tilted when realized in a realistic material. This gapless structure is effectively protected by the generalized chiral symmetry. It induces topological edge states when th...
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Revisiting flat bands and localization

Revisiting flat bands and localization

Flat bands cannot be accidental. Physically, it implies that the itinerancy of the system is not sufficient. Formal reasons are given by a molecular orbital (MO) representation which we are proposing....
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Kekule ordering and zero modes with disorder

Kekule ordering and zero modes with disorder

Zero modes of chiral symmetric systems are stable as for symmetry preserving disorder. On a honeycomb lattice with Kekule ordering, we have demonstrated this stabilities numerically. It has been pubis...
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Prefatory note in KOGAKU “Optical phenomena due to topology and applications”, Nov., 2020 (The Optical Society of Japan)

Sorry in Japanese.
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Machine learning for mirror skin effects

Machine learning for mirror skin effects

Robustness of the mirror skin effects against for randomness breaking the symmetry is demonstrated by machine learning. The letter has been published in J. Phys. Soc. Jpn. 90, 053703 (2021) by Hiromu ...
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Diffusion as a new platform of bulk-edge correspondence

Diffusion as a new platform of bulk-edge correspondence

Diffusion in non-equilibrium phenomena is typical and universal. Any unbalance away from the equilibrium is always/necessarily relaxed to the steady state. Here non-uniform (periodic) modulation of th...
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