Abstract
We carry out a systematic study of entanglement entropy in relativistic
quantum field theory. This is defined as the von Neumann entropy S\_A=-Tr rho\_A
log rho\_A corresponding to the reduced density matrix rho\_A of a subsystem A.
For the case of a 1+1-dimensional critical system, whose continuum limit is a
conformal field theory with central charge c, we re-derive the result
S\_A\sim(c/3) log(l) of Holzhey et al. when A is a finite interval of length l
in an infinite system, and extend it to many other cases: finite systems,finite
temperatures, and when A consists of an arbitrary number of disjoint intervals.
For such a system away from its critical point, when the correlation length \xi
is large but finite, we show that S\_AA(c/6)łog\xi, where A is
the number of boundary points of A. These results are verified for a free
massive field theory, which is also used to confirm a scaling ansatz for the
case of finite-size off-critical systems, and for integrable lattice models,
such as the Ising and XXZ models, which are solvable by corner transfer matrix
methods. Finally the free-field results are extended to higher dimensions, and
used to motivate a scaling form for the singular part of the entanglement
entropy near a quantum phase transition.
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