slides - Lattice Seminar - Desy
slides - Lattice Seminar - Desy
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