Abstract
Ground state entanglement quantified using the von Neumann entropy is
known to obey a universal scaling law in some one-dimensional
critical spin systems with and without disorder. The scaling behavior of
the entanglement entropy in higher dimensions is far less clear. This
poster contribution will present our findings in the entanglement
entropy of the random quantum Ising model in two dimensions, obtained by
a numerical implementation of the strong disorder renormalization group.
Our results show that the asymptotic behavior of the entropy per surface
area diverges at and only at the quantum phase transition that is
governed by an infinite-randomness fixed point. Here we identify a
double-logarithmic multiplicative correction to the area law for the
entanglement entropy. For the diluted quantum Ising model in higher
dimensions, the pure area law is found to be valid at the percolation
threshold, also governed by infinite randomness. The structure of the
strongly correlated spin clusters observed in the ground state of
the random quantum Ising model is fundamentally different from the
one in the diluted case, which reflects the different degrees of
quantum entanglement of the two systems.
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