TY - JOUR
T1 - A comprehensive search for the +pentaquark on the lattice
AU - Katz, S. D.
AU - Csikor, F.
AU - Fodor, Z.
AU - Kovács, T. G.
AU - Tóth, B. C.
N1 - Publisher Copyright:
© Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.
PY - 2005
Y1 - 2005
N2 - We study spin 1/2 isoscalar and isovector, even and odd parity candidates for the +(1540) pentaquark particle using large scale lattice QCD simulations. Previous lattice works led to inconclusive results because so far it has not been possible to unambiguously identify the known scattering spectrum and tell whether additionally a genuine pentaquark state also exists. Here we carry out this analysis using several possible wave functions (operators), including spatially non-trivial ones with unit orbital angular momentum. The cross correlator matrix we compute is 14×14 with 60 non-vanishing elements. We can clearly distinguish the lowest scattering state(s) in both parity channels up to above the expected location of the pentaquark, but we find no trace of the latter. We conclude that there are most probably no pentaquark bound states at our quark masses, corresponding to mπ=400-630 MeV. However, we cannot rule out the existence of a pentaquark state at the physical quark masses or pentaquarks with a more exotic wave function.
AB - We study spin 1/2 isoscalar and isovector, even and odd parity candidates for the +(1540) pentaquark particle using large scale lattice QCD simulations. Previous lattice works led to inconclusive results because so far it has not been possible to unambiguously identify the known scattering spectrum and tell whether additionally a genuine pentaquark state also exists. Here we carry out this analysis using several possible wave functions (operators), including spatially non-trivial ones with unit orbital angular momentum. The cross correlator matrix we compute is 14×14 with 60 non-vanishing elements. We can clearly distinguish the lowest scattering state(s) in both parity channels up to above the expected location of the pentaquark, but we find no trace of the latter. We conclude that there are most probably no pentaquark bound states at our quark masses, corresponding to mπ=400-630 MeV. However, we cannot rule out the existence of a pentaquark state at the physical quark masses or pentaquarks with a more exotic wave function.
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M3 - Conference article
AN - SCOPUS:85055839488
SN - 1824-8039
VL - 22
JO - Proceedings of Science
JF - Proceedings of Science
M1 - 008
T2 - 29th Johns Hopkins Workshop on Current Problems in Particle Theory: Strong Matter in the Heavens, JHW 2005
Y2 - 1 August 2005 through 3 August 2005
ER -