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Entanglement entropy at quantum critical points: Can you ... - INFN

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Dimers, heights and effective field theory<br />

Moessner, Sondhi and Fradkin; Ardonne, Fendley and Fradkin<br />

• The QDM can be mapped to a height model<br />

• Plaquette flip changes the height of th<strong>at</strong> plaquette by ±4, and the average height of<br />

the surrounding sites by ±1.<br />

• Equivalent configur<strong>at</strong>ions: h ∼ = h + 4.<br />

• Continuum limit: h ∼ = 4ϕ(x)<br />

Compactific<strong>at</strong>ion Radius: ϕ(x) ∼ = ϕ(x) + 1.<br />

• The Quantum Lifshitz model<br />

Hamiltonian:<br />

H =<br />

This is the Quantum Lifshitz Model.<br />

Z<br />

» 1<br />

d 2 x<br />

2 Π2 + κ2<br />

2<br />

–<br />

`∇2 ϕ´2<br />

(Henley; Moessner, Sondhi and Fradkin)<br />

• Action in imaginary time τ ⇔ smectic layers in 3D classical st<strong>at</strong>istical mechanics <strong>at</strong><br />

the Lifshitz transition.<br />

Z Z » –<br />

1<br />

S = d 2 x dτ<br />

2 (∂ τϕ) 2 + κ2 `∇2 ϕ´2<br />

2<br />

14

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