Entanglement Entropy – Part 2: Quantum Field Theory - Comments

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Discussion Overview

The discussion revolves around the topic of entanglement entropy in the context of quantum field theory, particularly focusing on conformal field theories (CFTs) in various dimensions. It explores the mathematical formulations and implications of entanglement entropy, including specific results and challenges in higher dimensions.

Discussion Character

  • Technical explanation
  • Exploratory

Main Points Raised

  • One participant notes that the formula S = \frac{c}{3} \log \frac{\ell}{a} is applicable only to (1+1)-dimensional CFTs, where the conformal anomaly is characterized by a single constant c.
  • It is mentioned that in higher dimensions, "twist fields" act as nonlocal "line" operators, necessitating additional work to derive results.
  • Free fields have been analyzed by Casini and Huerta, with references to their work on entanglement entropy and its relation to Euclidean free energy in (2+1)-dimensional CFTs.
  • Some isolated results for certain CFTs can be accessed perturbatively using the Calabrese-Cardy replica trick.
  • A participant clarifies that their discussion is specifically focused on (1+1) dimensions, suggesting that the figures and parts of the calculation should make this clear.
  • Another participant expresses appreciation for the article, indicating engagement with the content.

Areas of Agreement / Disagreement

The discussion includes multiple perspectives on the applicability of the entanglement entropy formula across different dimensions, indicating that there is no consensus on general results for strongly-interacting CFTs.

Contextual Notes

Participants reference specific studies and results, but there are limitations in generalizing findings across different dimensions and types of CFTs. The discussion also highlights the complexity of deriving results in strongly-interacting scenarios.

ShayanJ
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Entanglement Entropy – Part 2: Quantum Field Theory
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The result

S = \frac{c}{3} \log \frac{\ell}{a}

only applies to (1+1)-d CFTs, where the conformal anomaly exists and is parametrized by a single constant c. For higher dimensions, the "twist fields" are nonlocal "line" operators and you need to do some work. Free fields have been studied by Casini and Huerta ( ttps://arxiv.org/abs/0905.2562), and AdS/CFT gives some results from holography. Casini and Huerta have also shown that the entanglement entropy of a circle in a (2+1)-d CFT is equal to the Euclidean free energy on the sphere (see the Hartman lectures you asked about in another recent thread), and there are isolated results for certain CFTs which can be perturbatively accessed using this Calabrese-Cardy replica trick you describe. But general results for general regions in strongly-interacting CFTs are rare.
 
king vitamin said:
The result

S = \frac{c}{3} \log \frac{\ell}{a}

only applies to (1+1)-d CFTs, where the conformal anomaly exists and is parametrized by a single constant c. For higher dimensions, the "twist fields" are nonlocal "line" operators and you need to do some work. Free fields have been studied by Casini and Huerta ( ttps://arxiv.org/abs/0905.2562), and AdS/CFT gives some results from holography. Casini and Huerta have also shown that the entanglement entropy of a circle in a (2+1)-d CFT is equal to the Euclidean free energy on the sphere (see the Hartman lectures you asked about in another recent thread), and there are isolated results for certain CFTs which can be perturbatively accessed using this Calabrese-Cardy replica trick you describe. But general results for general regions in strongly-interacting CFTs are rare.

Of course, I just forgot to make it clear that I'm working in 1+1 dimensions. But I think the figures and some parts of the calculation make it clear.
 

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