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slides - Lattice Seminar - Desy

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The Need For All-to-all Propagators<br />

All-to-all<br />

Propagators<br />

in <strong>Lattice</strong><br />

Hadron<br />

Spectrum<br />

Calculations<br />

John Bulava<br />

Finite-volume stationary states are comprised of resonance<br />

states as well as scattering states.<br />

Some resonance states may have multi-particle content.<br />

Background<br />

Distillation -<br />

An Exact<br />

All-to-all<br />

Method<br />

Variance-<br />

Reduced<br />

Stochastic<br />

LapH (VRSL)<br />

〈0|B(p = 0, t)B(p = 0, t 0 )|0〉 = (1)<br />

1 ∑<br />

V 2 〈0|ϕ B (x, t)ϕ B (y, t 0 )|0〉<br />

x,y<br />

B(p, t)M(−p, t) = 1 ∑<br />

V 2 ϕ B (x, t)ϕ M (y, t)e ip·(x−y) (2)<br />

x,y<br />

Sum over y can be eliminated in Eq. 1, but not in<br />

correlation functions containing the operator from Eq. 2.<br />

Solving Mφ = η for all y is not feasible.<br />

John Bulava<br />

All-to-all Propagators in <strong>Lattice</strong> Hadron Spectrum Calculations

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