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