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| Journal Article | PUBDB-2023-05309 |
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2023
Inst.
Woodbury, NY
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Please use a persistent id in citations: doi:10.1103/PhysRevD.108.034507 doi:10.3204/PUBDB-2023-05309
Report No.: ADP-23-12/T1221; DESY-23-059; Liverpool LTH 1340; arXiv:2305.05491
Abstract: The Feynman-Hellmann approach to computing matrix elements in lattice QCD by first adding a perturbing operator to the action is described using the transition matrix and the Dyson expansion formalism. This perturbs the energies in the two-point baryon correlation function, from which the matrix element can be obtained. In particular at leading order in the perturbation we need to diagonalize a matrix of near-degenerate energies. While the method is general for all hadrons, we apply it here to a study of a sigma to nucleon baryon transition vector matrix element.
Keyword(s): higher-order: 0 ; baryon: correlation function ; lattice field theory ; perturbation ; hadron ; nucleon ; Feynman
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Preprint
Feynman-Hellmann approach to transition matrix elements and quasi-degenerate energy states
[10.3204/PUBDB-2023-02965]
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