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  1. All interesting physics is decentralized and local. If there was a central algorithm deciding what physics is allowed, we wouldn't have the enormous diversity and beauty of the universe emerging out of something like two dozen fundamental physical constants.

    I think this decentralized nature is also important when trying to understand physical systems. When we came up with our definition of topological order based on error correction (doi.org/10.1103/PhysRevB.106.0), it was absolutely crucial to use a decentralized algorithm and not a centralized one where you feed in the positions of all errors at once. It's the fediverse approach to error correction, if you like.

    #physics #condensedmatter #condmat #fediverse

  2. All interesting physics is decentralized and local. If there was a central algorithm deciding what physics is allowed, we wouldn't have the enormous diversity and beauty of the universe emerging out of something like two dozen fundamental physical constants.

    I think this decentralized nature is also important when trying to understand physical systems. When we came up with our definition of topological order based on error correction (doi.org/10.1103/PhysRevB.106.0), it was absolutely crucial to use a decentralized algorithm and not a centralized one where you feed in the positions of all errors at once. It's the fediverse approach to error correction, if you like.

    #physics #condensedmatter #condmat #fediverse

  3. Topologically ordered states of matter are characterized by fascinating non-local quantum correlations in the many-body wave function. However, deciding whether a quantum state is topologically ordered or not is extremely difficult. A large part of the problem is that so far, signatures like the topological entanglement entropy could not be efficiently computed.

    We are happy to present a framework for the computation of topological order that provides an exponential speedup over existing methods: dx.doi.org/10.1088/1367-2630/a

    #quantum #physics #condensedmatter #condmat

  4. Topologically ordered states of matter are characterized by fascinating non-local quantum correlations in the many-body wave function. However, deciding whether a quantum state is topologically ordered or not is extremely difficult. A large part of the problem is that so far, signatures like the topological entanglement entropy could not be efficiently computed.

    We are happy to present a framework for the computation of topological order that provides an exponential speedup over existing methods: dx.doi.org/10.1088/1367-2630/a

    #quantum #physics #condensedmatter #condmat

  5. Today's #arXivsummary: arxiv.org/abs/2311.06350 by Romen et. al. Authors investigate deconfined quantum critical points in the long-range, anisotropic Heisenberg chain. Model undergoes a continuous phase transition from valence bond solid to an antiferromagnet. Long-range interactions are irrelevant & transition is well described by a double frequency sine-Gordon model. #CondMat #arXiv_2311_06350

  6. Today's #arXivsummary: arxiv.org/abs/2311.06350 by Romen et. al. Authors investigate deconfined quantum critical points in the long-range, anisotropic Heisenberg chain. Model undergoes a continuous phase transition from valence bond solid to an antiferromagnet. Long-range interactions are irrelevant & transition is well described by a double frequency sine-Gordon model. #CondMat #arXiv_2311_06350

  7. Today's #arXivsummary: arxiv.org/abs/2311.04266 by Radzihovsky. Author points out a simple and generic mechanism for a thermally-driven reentrant supersolidity. Mechanism reduces to a re-enterant low-temperature normal-superfluid transition. #CondMat #arXiv_2311_04266

  8. Today's #arXivsummary: arxiv.org/abs/2311.04266 by Radzihovsky. Author points out a simple and generic mechanism for a thermally-driven reentrant supersolidity. Mechanism reduces to a re-enterant low-temperature normal-superfluid transition. #CondMat #arXiv_2311_04266

  9. Today's #arXivsummary: arxiv.org/abs/2311.02155 by Pak et. al. Authors show that the PT-symmetry stabilizes the Hopf invariant in the Hopf insulator even in the presence of non-Hermiticity. Zak phase remains quantized. #CondMat #arXiv_2311_02155

  10. Today's #arXivsummary: arxiv.org/abs/2310.11236 by Misawa. Author's work suggests that quasiparticles in the normal state of high-Tc cuprate superconductors behave as a 3D Fermi liquid. Logarithmic formula as a function of T emerges in transport quantities and thermodynamics results from quasiparticle interactions. #CondMat #arXiv_2310_11236

  11. Today's #arXivsummary: arxiv.org/abs/2310.09324 by Sun. Authors show that an indirect exchange interaction between spin impurities can be controlled by a dissipationless supercurrent with just a conventional superconductor and two spin impurities placed on its surface. #CondMat #arXiv_2310_09324

  12. Today's arXivsummary: arxiv.org/abs/2310.09063, by Witt et. al. Multi-orbital model of alkali-doped fullerides (A3C60) developed using Dynamical Mean-Field Theory, which is utilized to show how proximity of superconductivity, Jahn-Teller metallic, and Mott-localized states impact the superconducting coherence, order parameter stiffness, & critical temperature. Localized superconducting regime with very short coherence length. #CondMat #arXiv_2310_09063

  13. Today's #arXivsummary: arxiv.org/abs/2310.07978 by Chen et. al. Authors study Anderson localization in disordered tight-binding models on hyperbolic lattices. Numerically show the existence of an Anderson localization transition on the {8,3} & {8,8} lattices. #CondMat #arXiv_2310_07978

  14. Today's #arXivsummary: arxiv.org/abs/2310.06891 by Kao et. al. Authors study the dynamical response of vacancy-induced quasiparticle excitations in a site-diluted Kitaev spin liquid in the presence of a magnetic field. STM response is shown to be sensitive to the local flux configuration, magnetic field strength, and vacancy concentration. #CondMat #arXiv_2310_06891

  15. Today's #arXivsummary: arxiv.org/abs/2310.06748 by Shankar & Maciejko. Authors utilize semiclassical instanton methods not relying on conformal invariance to construct monopole operators directly in (2+1)D spacetime as instanton-induced 't Hooft vertices, as applied to the Dirac liquid. Instanton-based approach can determine monopole quantum numbers on bipartite lattices. #CondMat #arXiv_2310_06748