TY - JOUR
T1 - Mirage in temporal correlation functions for baryon-baryon interactions in lattice QCD
AU - The HAL QCD collaboration
AU - Iritani, T.
AU - Doi, T.
AU - Aoki, S.
AU - Gongyo, S.
AU - Hatsuda, T.
AU - Ikeda, Y.
AU - Inoue, T.
AU - Ishii, N.
AU - Murano, K.
AU - Nemura, H.
AU - Sasaki, K.
N1 - Publisher Copyright:
© 2016, The Author(s).
PY - 2016/10/1
Y1 - 2016/10/1
N2 - Single state saturation of the temporal correlation function is a key condition to extract physical observables such as energies and matrix elements of hadrons from lattice QCD simulations. A method commonly employed to check the saturation is to seek for a plateau of the observables for large Euclidean time. Identifying the plateau in the cases having nearby states, however, is non-trivial and one may even be misled by a fake plateau. Such a situation takes place typically for a system with two or more baryons. In this study, we demonstrate explicitly the danger from a possible fake plateau in the temporal correlation functions mainly for two baryons (ΞΞ and N N), and three and four baryons (3He and 4He) as well, employing (2+1)-flavor lattice QCD at mπ = 0.51GeV on four lattice volumes with L = 2.9, 3.6, 4.3 and 5.8 fm. Caution is required when drawing conclusions about the bound N N , 3N and 4N systems based only on the standard plateau fitting of the temporal correlation functions.[Figure not available: see fulltext.]
AB - Single state saturation of the temporal correlation function is a key condition to extract physical observables such as energies and matrix elements of hadrons from lattice QCD simulations. A method commonly employed to check the saturation is to seek for a plateau of the observables for large Euclidean time. Identifying the plateau in the cases having nearby states, however, is non-trivial and one may even be misled by a fake plateau. Such a situation takes place typically for a system with two or more baryons. In this study, we demonstrate explicitly the danger from a possible fake plateau in the temporal correlation functions mainly for two baryons (ΞΞ and N N), and three and four baryons (3He and 4He) as well, employing (2+1)-flavor lattice QCD at mπ = 0.51GeV on four lattice volumes with L = 2.9, 3.6, 4.3 and 5.8 fm. Caution is required when drawing conclusions about the bound N N , 3N and 4N systems based only on the standard plateau fitting of the temporal correlation functions.[Figure not available: see fulltext.]
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U2 - 10.1007/JHEP10(2016)101
DO - 10.1007/JHEP10(2016)101
M3 - Article
AN - SCOPUS:84992381671
SN - 1126-6708
VL - 2016
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 10
M1 - 101
ER -