Are two nucleons bound in lattice QCD for heavy quark masses? -- Consistency check with Lüscher's finite volume formula --
arXiv:1703.07210 · doi:10.1103/PhysRevD.96.034521
Abstract
On the basis of the Lüscher's finite volume formula, a simple test (consistency check or sanity check) is introduced and applied to inspect the recent claims of the existence of the nucleon-nucleon () bound state(s) for heavy quark masses in lattice QCD. We show that the consistency between the scattering phase shifts at and/or obtained from the lattice data and the behavior of phase shifts from the effective range expansion (ERE) around exposes the validity of the original lattice data, otherwise such information is hidden in the energy shift of the two nucleons on the lattice. We carry out this sanity check for all the lattice results in the literature claiming the existence of the bound state(s) for heavy quark masses, and find that (i) some of the data show clear inconsistency between the behavior of ERE at and that at , (ii) some of the data exhibit singular behavior of the low energy parameter (such as the divergent effective range) at , (iii) some of the data have the unphysical residue for the bound state pole in S-matrix, and (iv) the rest of the data are inconsistent among themselves. Furthermore, we raise a caution of using the ERE in the case of the multiple bound states. Our finding, together with the fake plateau problem previously pointed out by the present authors, brings a serious doubt on the existence of the bound states for pion masses heavier than 300 MeV in the previous studies.
39 pages, 16 figures, and 11 tables, title changed, references and comment added
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