Searching for beauty-fully bound tetraquarks using lattice nonrelativistic QCD

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Abstract

Motivated by multiple phenomenological considerations, we perform the first search for the existence of a bbbb tetraquark bound state with a mass below the lowest noninteracting bottomonium-pair threshold using the first-principles lattice nonrelativistic QCD methodology. We use a full S-wave color/spin basis for the bbbb operators in the three 0++, 1+- and 2++ channels. We employ four gluon field ensembles at multiple lattice spacing values ranging from a=0.06-0.12 fm, all of which include u, d, s and c quarks in the sea, and one ensemble which has physical light-quark masses. Additionally, we perform novel exploratory work with the objective of highlighting any signal of a near threshold tetraquark, if it existed, by adding an auxiliary potential into the QCD interactions. With our results we find no evidence of a QCD bound tetraquark below the lowest noninteracting thresholds in the channels studied.

Figures

  • TABLE I. The color representations of the different quark combinations. Note that, as described in the text, once the color representation of the (anti-) diquark is chosen, the Pauli-exclusion principle enforces certain spin combinations in S-wave. Also given are the SUð3Þ color contractions needed for the b̄b̄bb operators.
  • TABLE II. Fierz relations in the b̄b̄bb system relating the twomeson and the diquark-antidiquark bilinears.
  • FIG. 1. There are four connected Wick contractions for the twomeson-type correlator when the quarks have the same flavor. The grey region represents a color neutral meson, the blue line a quark and the red line an antiquark. We call these the (a) Direct1 contraction where each meson propagates to itself, (b) Xchange2 where an antiquark is exchanged between the meson pair, (c) Direct3 where each meson propagates to the other, and (d) Xchange4 where a quark is exchanged between the meson pair.
  • FIG. 2. There are four connected Wick contractions for the diquark-antidiquark-type correlator when the quarks have the same flavor. The blue shaded region represents a diquark, the red shaded region the antidiquark, a blue line a quark and the red line an antiquark. The uncrossing of the lines in Fig. 2(b) to produce Fig. 2(a) gives a , as discussed in the text, which enforces the Pauli-exclusion principle.
  • TABLE III. Details of the gauge ensembles used in this study. β is the gauge coupling. a (fm) is the lattice spacing [23,24], amq are the sea quark masses, Ns × NT gives the spatial and temporal extent of the lattices in lattice units and ncfg is the number of configurations used for each ensemble. We use 16 time sources on each configuration to increase statistics. Ensembles 1 and 2 are referred to as “coarse,” 3 as “fine,” and 4 as “superfine”.
  • TABLE IV. Parameters used for the valence quarks. amb is the bare b-quark mass in lattice units, u0L is the tadpole parameter and the ci are coefficients of terms in the NRQCD Hamiltonian [see Eq. (13))]. Details of their calculation can be found in [23,32]. c3, c7, c8 and c9 are included at tree level.
  • TABLE V. The b̄b̄bb interpolating operators used in this study. Operators in each column are subduced from the infinite-volume continuum quantum numbers JPC given in the first row. The superscript on each operator denotes the lattice irrep of that operator and the subscript denotes the building blocks of the operator, as explained in the text. We generate each operator with three different spatial configurations as shown in Eq. (4): where the building blocks are separated by a distance rx ¼ 0, 1 or 2 lattice units in the x-direction.
  • FIG. 3. The effective mass plot for the ηb andΥ on the superfine ensemble (set 4 listed in Table III). The effective mass plots on the other ensembles are qualitatively identical.

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Hughes, C., Eichten, E., & Davies, C. T. H. (2018). Searching for beauty-fully bound tetraquarks using lattice nonrelativistic QCD. Physical Review D, 97(5). https://doi.org/10.1103/PhysRevD.97.054505

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