Daily ArXiv

Friday, 30 August 2019

[1908.10946] Similarities and differences between infinite-layer nickelates and cuprates and implications for superconductivity


 [1908.10976] Higher order topological insulators in a magnetic field

[1908.11362] Spin-1/2 XXZ Heisenberg chain in a longitudinal magnetic field


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Thursday, 29 August 2019

[1908.10371] Prethermalization without temperature

[1908.10381] Distinguish modular categories and 2+1D topological orders beyond modular data: Mapping class group of higher genus manifold

[1908.10453] Fermi/Pauli Duality in Arbitrary Dimension

[1908.10847] Vortices and composite order in $\mathrm{SU}(N)$ theories coupled to Abelian gauge field

[1908.10850] Phase transitions in $\mathrm{U}(1)^N$ lattice London models

[1908.10368] Anyons on the sphere: analytic states and spectrum


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Wednesday, 28 August 2019

[1908.09831] Pairing Instability on a Luttinger Surface: A Non-Fermi Liquid to Superconductor Transition and its Gravity Dual

[1908.09837] Magic-Angle Semimetals with Chiral Symmetry

[1908.09852] Entanglement spectrum and symmetries in non-Hermitian fermionic non-interacting models


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Tuesday, 27 August 2019

[1908.08958] A 1d lattice model for the boundary of the quantum spin-Hall insulator

[1908.09802] Why band theorists have been so successful in explaining and predicting novel superconductors?

[1908.09159] A 1+1 Lifshitz Weyl Anomaly From a Schrodinger-invariant Non-relativistic Chern-Simons Action


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Monday, 26 August 2019

[1908.08536] Electric Circuit Realizations of Fracton Physics

[1908.08540] Emergent fractons and algebraic quantum liquid from plaquette melting transitions

[1908.08726] Observation of a Room Temperature Two-dimensional Ferroelectric Metal

[1410.4540] Symmetry Fractionalization, Defects, and Gauging of Topological Phases
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Friday, 23 August 2019

[1908.08334] Abundance of $\mathbb{Z}_2$ topological order in exfoliable two-dimensional insulators

[1908.08352] Royal Society Inaugural Article Perspective: Multiferroics Beyond Electric-Field Control of Magnetism

[1908.08049] Sorting topological stabilizer models in three dimensions


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Thursday, 22 August 2019

[1908.07545] Isometric Tensor Network representation of string-net liquids

[1908.07601] Novel Fracton Phases from Gauge Theories

[1908.07671] Magnetic-field Induced Quantum Phases in Tensor Network Study of Kitaev Magnets

[1908.07540] The negativity contour: a quasi-local measure of entanglement for mixed states


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Wednesday, 21 August 2019

[1908.06984] On duality between Cosserat elasticity and fractons

[1908.06993] The Speed of Quantum Information Spreading in Chaotic Systems

[1908.07006] Bosonic fractional quantum Hall states in driven optical lattices

[1908.07010] Power-law entanglement growth from typical product states

[1908.06977] Superfluids as Higher-form Anomalies


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Sunday, 18 August 2019

[1908.05686] Linear in Temperature Resistivity and Associated Mysteries

[1908.05687] Bound states in the continuum of higher-order topological insulators


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Friday, 16 August 2019

[1908.05280] Non-Abelian chiral spin liquid on a simple non-Archimedean lattice

[1908.05417] Collective Excitations of Quantum Anomalous Hall Ferromagnets in Twisted Bilayer Graphene


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Wednesday, 14 August 2019

[1908.04299] Higher-order topological phase without crystalline symmetry

[1908.04307] The Hubbard model on the honeycomb lattice: from static and dynamical mean-field theories to lattice quantum Monte Carlo simulations

[1908.04557] Anomalous electrical magnetochiral effect by chiral spin fluctuation


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Monday, 12 August 2019

[1908.03217] Effective response theory for Floquet topological systems

[1908.03226] Ferromagnetism in Quantum Dot Plaquettes


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Friday, 9 August 2019

[1908.02753] Disorder in Twisted Bilayer Graphene

[1908.02757] Intrinsic superconducting instabilities of a solvable model for an incoherent metal

[1908.02762] Valence bond solid and possible deconfined quantum criticality in an extended kagome lattice Heisenberg antiferromagnet

[1908.02767] The "not-A", SPT and Potts phases in an $S_3$-invariant chain

[1908.02758] Fractionalized Degrees of Freedom at Infinite Coupling in large Nf QED in 2+1 dimensions


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Thursday, 8 August 2019

[1908.02369] New Materials Physics

[1908.02599] Matrix formulation for non-Abelian families

[1908.02613] Lattice models that realize $\mathbb{Z}_n$-1-symmetry protected topological states for even $n$

[1908.02667] A Practical Mini-Course on Applied Holography
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Tuesday, 6 August 2019

[1908.02186] $\mathbb{Z}_n$ Solitons in Intertwined Topological Phases: From Boson Fractionalization to a Generalized Bulk-Defect Correspondence

[1908.02257] Anisotropic layer construction of anisotropic fracton models

[1908.02271] Goldstone Modes in the Emergent Gauge Fields of a Frustrated Magnet

[1908.02235] Real Clifford algebras and their spinors for relativistic fermions


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[1908.00986] Symmetry breaking and skyrmionic transport in twisted bilayer graphene

[1908.00988] Interaction-driven plateau transition between integer and fractional Chern Insulators

[1908.00995] Supersymmetry in the nonsupersymmetric Sachdev-Ye-Kitaev model

[1908.01021] Polarization-resolved Raman spectroscopy of α-RuCl3 and evidence of room temperature two-dimensional magnetic scattering

[1908.01248] Multicritical behavior of the fidelity susceptibility for the 2D quantum transverse-field $XY$ model

[1908.01758] An in-plane hexagonal antiferromagnet in the Cu-Mn-As system, Cu$_{0.82}$Mn$_{1.18}$As


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Monday, 5 August 2019

[1908.00718] Antiadiabatic Phonons and Superconductivity in Eliashberg-McMillan Theory

[1908.00729] Specific Heat Signature of the Berezinskii-Kosterlitz-Thouless Transition in Ultrathin Superconducting Films


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Thursday, 1 August 2019

[1908.00011] Boundary-obstructed topological phases

[1908.00016] Strong and "Fragile" Topological Dirac Semimetals with Higher-Order Fermi Arcs

[1908.00030] Physics of Superconducting Transition Temperatures

[1908.00058] Angle-Dependent {\it Ab initio} Low-Energy Hamiltonians for a Relaxed Twisted Bilayer Graphene Heterostructure

[1908.00103] Solvable lattice models for metals with Z2 topological order


Posted by Shenoy at 20:37 No comments:
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      • [1908.10946] Similarities and differences between...
      • [1908.10371] Prethermalization without temperatur...
      • [1908.09831] Pairing Instability on a Luttinger S...
      • [1908.08958] A 1d lattice model for the boundary ...
      • [1908.08536] Electric Circuit Realizations of Fra...
      • [1908.08334] Abundance of $\mathbb{Z}_2$ topologi...
      • [1908.07545] Isometric Tensor Network representat...
      • [1908.06984] On duality between Cosserat elastici...
      • [1908.05686] Linear in Temperature Resistivity an...
      • [1908.05280] Non-Abelian chiral spin liquid on a ...
      • [1908.04299] Higher-order topological phase witho...
      • [1908.03217] Effective response theory for Floque...
      • [1908.02753] Disorder in Twisted Bilayer Graphene...
      • [1908.02369] New Materials Physics [1908.02599] ...
      • [1908.02186] $\mathbb{Z}_n$ Solitons in Intertwin...
      • [1908.00986] Symmetry breaking and skyrmionic tra...
      • [1908.00718] Antiadiabatic Phonons and Supercondu...
      • [1908.00011] Boundary-obstructed topological phas...
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