We study the entanglement entropy of random partitions in one- and two-dimensional critical fermionic systems. In an infinite system we consider a finite, connected (hypercubic) domain of linear extent L, the points of which with probability p belong to the subsystem. The leading contribution to the average entanglement entropy is found to scale with the volume as a(p)LD, where a(p) is a non-universal function, to which there is a logarithmic correction term, b(p)LD−1 ln L. In 1D the prefactor is given by b(p)=c/3f(p),where c is the central charge of the model and f(p) is a universal function. In 2D the prefactor has a different functional form of p below and above the percolation threshold.
Description
Entanglement entropy of random partitioning | The European Physical Journal B
%0 Journal Article
%1 Roósz2020
%A Roósz, Gergő
%A Kovács, István A.
%A Iglói, Ferenc
%D 2020
%J Eur. Phys. J. B
%K a
%N 1
%P 8
%R 10.1140/epjb/e2019-100496-y
%T Entanglement entropy of random partitioning
%U https://doi.org/10.1140/epjb/e2019-100496-y
%V 93
%X We study the entanglement entropy of random partitions in one- and two-dimensional critical fermionic systems. In an infinite system we consider a finite, connected (hypercubic) domain of linear extent L, the points of which with probability p belong to the subsystem. The leading contribution to the average entanglement entropy is found to scale with the volume as a(p)LD, where a(p) is a non-universal function, to which there is a logarithmic correction term, b(p)LD−1 ln L. In 1D the prefactor is given by b(p)=c/3f(p),where c is the central charge of the model and f(p) is a universal function. In 2D the prefactor has a different functional form of p below and above the percolation threshold.
@article{Roósz2020,
abstract = {We study the entanglement entropy of random partitions in one- and two-dimensional critical fermionic systems. In an infinite system we consider a finite, connected (hypercubic) domain of linear extent L, the points of which with probability p belong to the subsystem. The leading contribution to the average entanglement entropy is found to scale with the volume as a(p)LD, where a(p) is a non-universal function, to which there is a logarithmic correction term, b(p)LD−1 ln L. In 1D the prefactor is given by b(p)=c/3f(p),where c is the central charge of the model and f(p) is a universal function. In 2D the prefactor has a different functional form of p below and above the percolation threshold.},
added-at = {2023-10-31T11:39:49.000+0100},
author = {Roósz, Gergő and Kovács, István A. and Iglói, Ferenc},
biburl = {https://www.bibsonomy.org/bibtex/2815cd94c876519182a2759f2335f8998/ctqmat},
day = 20,
description = {Entanglement entropy of random partitioning | The European Physical Journal B},
doi = {10.1140/epjb/e2019-100496-y},
interhash = {59c814a372d44c4b86670367edaaccfa},
intrahash = {815cd94c876519182a2759f2335f8998},
issn = {1434-6036},
journal = {Eur. Phys. J. B},
keywords = {a},
month = {01},
number = 1,
pages = 8,
timestamp = {2024-09-17T11:55:33.000+0200},
title = {Entanglement entropy of random partitioning},
url = {https://doi.org/10.1140/epjb/e2019-100496-y},
volume = 93,
year = 2020
}