I'm studying the holographic entanglement entropy (HEE) in this paper (Ryu-Takayanagi, 2006). In section 6.3 they compute the HEE for a segment in a 2D CFT. To do so, they obtain the corresponding geodesic in the bulk (in the Poincaré patch) and compute its length.
I understand all that process, but I'm having some trouble when they introduce the cutoff. The metric diverges when z→0 so we introduce a cutoff ϵ>0, I understand that. But then they say
Since eρ∼xi/z near the boundary, we find z∼a
Here, ρ is the hiperbolic radial coordinate un the global coordinates for AdS,
ds2=R2(−cosh2ρ dτ2+dρ2+sinh2ρ dΩ2)
xi and z are coordinates in the Poincaré patch,
ds2=R2z2(dz2−dt2+∑i(dxi)2)
And a is the inverse of the UV cutoff of the CFT in the boundary, that is, the spacing between sites.
I have two problems:
1) First, I don't see why near the boundary eρ∼xi/z. I made up the relations between both coordinate systems and I find more complicated relations than that (even setting z∼0).
2) Even assuming the previous point, I don't understand why we obtain that relation between the CFT and the z cutoff.
This post imported from StackExchange Physics at 2014-09-02 07:57 (UCT), posted by SE-user David Pravos