4.4 Article

Entanglement entropy and negativity in the Ising model with defects

期刊

JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 6, 页码 -

出版社

SPRINGER
DOI: 10.1007/JHEP06(2022)165

关键词

Anyons; Conformal Field Models in String Theory; Field Theories in Lower Dimensions; Lattice Integrable Models

资金

  1. Simons Foundation [825876]
  2. European Research Council (ERC) under the European Unions Horizon 2020 research and innovation program [771537]
  3. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy [EXC-2111-390814868]
  4. Bavarian state government
  5. Hightech Agenda Bayern Plus

向作者/读者索取更多资源

Defects in two-dimensional conformal field theories (CFTs) exhibit different characteristics in terms of entanglement properties. This work focuses on the entanglement entropy (EE) and entanglement negativity (EN) of subsystems in the Ising CFT with energy and duality defects. Interestingly, the EE for the duality defect is fundamentally different from the energy defect due to the existence of zero energy modes. The logarithmic scaling of the EN is found to have a continuously-varying effective central charge, which is different from that obtained from the EE. Defects also leave their fingerprints in the subleading term of the scaling of the EN.
Defects in two-dimensional conformal field theories (CFTs) contain signatures of their characteristics. In this work, we analyze entanglement properties of subsystems in the presence of energy and duality defects in the Ising CFT using the density matrix renormalization group (DMRG) technique. In particular, we compute the entanglement entropy (EE) and the entanglement negativity (EN) in the presence of defects. For the EE, we consider the cases when the defect lies within the subsystem and at the edge of the subsystem. We show that the EE for the duality defect exhibits fundamentally different characteristics compared to the energy defect due to the existence of localized and delocalized zero energy modes. Of special interest is the nontrivial 'finite-size correction' in the EE obtained recently using free fermion computations [1]. These corrections arise when the subsystem size is appreciable compared to the total system size and lead to a deviation from the usual logarithmic scaling characteristic of one-dimensional quantum-critical systems. Using matrix product states with open and infinite boundary conditions, we numerically demonstrate the disappearance of the zero mode contribution for finite subsystem sizes in the thermodynamic limit. Our results provide further support to the recent free fermion computations, but clearly contradict earlier analytical field theory calculations based on twisted torus partition functions. Subsequently, we compute the logarithm of the EN (log-EN) between two disjoint subsystems separated by a defect. We show that the log-EN scales logarithmically with the separation of the subsystems. However, the coefficient of this logarithmic scaling yields a continuously-varying effective central charge that is different from that obtained from analogous computations of the EE. The defects leave their fingerprints in the subleading term of the scaling of the log-EN. Furthermore, the log-EN receives similar 'finite size corrections' like the EE which leads to deviations from its characteristic logarithmic scaling.

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