Entanglement Entropy of Non Unitary Conformal Field Theory

Understand

In this letter we show that the R\'enyi entanglement entropy of a region of large size $\ell$ in a one-dimensional critical model whose ground state breaks conformal invariance (such as in those described by non-unitary conformal field theories), behaves as $S_n \sim \frac{c_{\mathrm{eff}}(n+1)}{6n} \log \ell$, where $c_{\mathrm{eff}}=c-24\Delta>0$ is the effective central charge, $c$ (which may be negative) is the central charge of the conformal field theory and $\Delta\neq 0$ is the lowest holomorphic conformal dimension in the theory.

• We also obtain results for models with boundaries, and with a large but finite correlation length, and we show that if the lowest conformal eigenspace is logarithmic ($L_0 = \Delta I + N$ with $N$ nilpotent), then there is an additional term proportional to $\log(\log \ell)$.
• These results generalize the well known expressions for unitary models.
• We provide a general proof, and report on numerical evidence for a non-unitary spin chain and an analytical computation using the corner transfer matrix method for a non-unitary lattice model.