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We develop a novel framework to study quantum phase transitions in two-dimensional topological insulators (TIs) driven by strain-induced perturbations. Using a new perturbation Hamiltonian that couples mechanical strain to topological edge states, we derive formulations for the continuous transition from topological to trivial insulator phases via an intermediate critical phase. Our model introduces critical exponents (v = 1, z = 1), a universal scaling law for the energy gap, and a real-space correlation function, validated through analytical and numerical methods. Phase diagrams, density of states, and correlation functions, visualized in four figures, illustrate the transition dynamics. This work addresses a key gap in controlling topological phases via external fields, offering insights for quantum device engineering and experimental realization in strain-tunable systems like HgTe quantum wells.
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http://dx.doi.org/10.1088/1361-648X/ae0288 | DOI Listing |
Phys Rev Lett
August 2025
University of Southern Denmark, Centre for Nano Optics, Campusvej 55, Odense M DK-5230, Denmark.
Controlling the spontaneous emission of nanoscale quantum emitters (QEs) is crucial for developing advanced photon sources required in many areas of modern nanophotonics, including quantum information technologies. Conventional approaches to shaping photon emission are based on using bulky configurations, while approaches recently developed in quantum metaphotonics suffer from limited capabilities in achieving desired polarization states and directionality, failing to provide on-demand photon sources tailored precisely to technological needs. Here, we propose a universal approach to designing versatile photon sources using on-chip QE-coupled meta-optics that enable direct transformations of QE-excited surface plasmon polaritons into spatially propagating photon streams with arbitrary polarization states, directionality, and amplitudes via both resonance and geometric phases supplied by scattering meta-atoms.
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August 2025
Weizmann Institute of Science, Department of Condensed Matter Physics, Rehovot 7610001, Israel.
We address the problem of identifying a 2+1D topologically ordered phase using measurements on the ground-state wave function. For nonchiral topological order, we describe a series of bulk multipartite entanglement measures that extract the invariants ∑_{a} d_{a}^{2}θ_{a}^{r} for any r≥2, where d_{a} and θ_{a} are the quantum dimension and topological spin of an anyon a, respectively. These invariants are obtained as expectation values of permutation operators between 2r replicas of the wave function, applying different permutations on four distinct regions of the plane.
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August 2025
Institut für Theoretische Physik, Universität zu Köln, Zülpicher Straße 77, 50937 Cologne, Germany.
Monitored quantum circuits have attracted significant interest as an example of synthetic quantum matter, intrinsically defined by their quantum information content. Here, we propose a multipartite entanglement perspective on monitored phases through the lens of quantum Fisher information. Our findings reveal that unstructured monitored random circuits fail to exhibit divergent multipartite entanglement even at criticality, highlighting their departure from standard quantum critical behavior.
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August 2025
East China Normal University, Key Laboratory of Polar Materials and Devices (MOE), School of Physics and Electronic Science, Shanghai 200241, China.
The far-from-equilibrium dynamics of certain interacting quantum systems still defy precise understanding. One example is the so-called quantum many-body scars (QMBSs), where a set of energy eigenstates evade thermalization to give rise to long-lived oscillations. Despite the success of viewing scars from the perspectives of symmetry, commutant algebra, and quasiparticles, it remains a challenge to elucidate the mechanism underlying all QMBS and to distinguish them from other forms of ergodicity breaking.
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August 2025
University of Alberta, Department of Physics, Edmonton, Alberta T6G 2E1, Canada.
Hyperbolic lattices present a unique opportunity to venture beyond the conventional paradigm of crystalline many-body physics and explore correlated phenomena in negatively curved space. As a theoretical benchmark for such investigations, we extend Kitaev's spin-1/2 honeycomb model to hyperbolic lattices and exploit their non-Euclidean space-group symmetries to solve the model exactly. We elucidate the ground-state phase diagram on the {8,3} lattice and find a gapped Z_{2} spin liquid with Abelian anyons, a gapped chiral spin liquid with non-Abelian anyons and chiral edge states, and a Majorana metal whose finite low-energy density of states is dominated by non-Abelian Bloch states.
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