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

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The Quantum Dimer Model<br />

H RK = ∑ i<br />

(vV i − tF i ), Rokhsar and Kivelson (1988)<br />

V i = ∣ ∣<br />

〉〈 ∣ ∣ + ∣ ∣<br />

〉〈 ∣ ∣ F i = ∣ ∣<br />

〉〈 ∣ ∣ + ∣ ∣<br />

〉〈 ∣ ∣<br />

Here each bar represents a spin singlet bond.<br />

For t = v ⇒ H RK = P i Q† i Q i , with Q i = ` 1 −1<br />

−1 1<br />

´.<br />

• The ground st<strong>at</strong>e wave function |Ψ 0 〉 has E = 0<br />

|Ψ 0 〉 = 1 √<br />

Zcl<br />

X<br />

where Z cl is the sum over all dimer configur<strong>at</strong>ions<br />

C<br />

|C〉 ,<br />

• Equal-time correl<strong>at</strong>ors in the <strong>quantum</strong> dimer model <strong>at</strong> the RK point are given by<br />

correl<strong>at</strong>ors of the classical dimer model.<br />

• This is actually a loop model: loops are the dimer moves from a reference st<strong>at</strong>e. This<br />

is the simplest loop model: the SU(2) 1 fully packed loop model.<br />

13

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