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Abstracts

P1.23

Graphene-like microwave billiards: Van-Hove singularities (VHS)

and Excited-State Quantum Phase Transitions (ESQPT).

Macek, Michal(1) Iachello, Francesco(2) Dietz, Barbara(3, 4)

1) The Czech Academy of Sciences, Institute of Scientific Instruments,

Kralovopolska 147, 612 64 Brno, Czech Republic

2) Yale University, Center for Theoretical Physics, Sloane Physics Laboratory,

New Haven, Connecticut 06520-8120, USA

3) Technische Universitaet Darmstadt, Institut fuer Kernphysik, D-64289

Darmstadt, Germany

4) Institute of Physics, Polish Academy of Sciences, Al. Lotnikow 32/46, 02-668

Warzawa, Poland

Superconducting 2D microwave resonators containing triangular lattices of

metallic cylinders form photonic crystals, which enable to model finite-sized

graphene flakes. High presision spectral measurements resolving all excitations

are possible. We describe the spectra by an algebraic model, providing analytical

solutions to the dispersion relations and density of states. At the VHS, whose

energies correspond to an ESQPT, we find stable stripe-like states parallel to the

zig-zag direction, simillar to the topological edge states, however these appear

in the bulk. They are stable with respect to long range perturbations and noise,

and appear also for irregular shapes of the boundaries.

P1.24

Localized excitations in 2D system of charged hard-core bosons

Yu.D. Panov(1), A.S. Moskvin(1), F.N. Rybakov(1,2), A.B. Borisov(1,2)

1) Ural Federal University, 620002, Mira str., 19, Ekaterinburg, Russia

2) Institute of Metal Physics UD RAS, 620990, S. Kovalevskaya str., 18,

Ekaterinburg, Russia

Making use of an asymptotic analysis and continual approximation we constructed

the phase diagram of localized excitations over a homogeneous ground state for

the 2D system of charged hard-core bosons. It is shown that in the superfluid

(SF) phase the excitations are the ferro- and antiferro- type vortices. Near the

boundary between the SF and supersolid (SS) phases, the antiferro-type vortices

in the SF phase begin to dominate, their inflation leads to a change of the

homogeneous ground state from the SF to SS phase. In the SS phase the vortices

are only possible at the half-filling (net charge-ordered phase), while at arbitrary

filling the topological excitations like skyrmions exist.

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