Can X(5568)X(5568) be described as a BsπB_sπ, BKˉB\bar{K} resonant state?

preprint2016arXivOpen access

Abstract

The D0 Collaboration has recently seen a resonant-like peak in the BsπB_sπ invariant mass spectrum, claimed to be a new state called X(5568)X(5568). Using a BsπB_sπ--BKˉB\bar{K} coupled channel analysis, implementing unitarity, and with the interaction derived from Heavy Meson Chiral Perturbation Theory, we are able to reproduce the reported spectrum, with a pole that can be associated to the claimed X(5568)X(5568) state, and with mass and width in agreement with the ones reported in the experimental analysis. However, if the TT-matrix regularization is performed by means of a momentum cutoff, the value for the latter needed to reproduce the spectrum is Λ=2.80±0.04 GeVΛ= 2.80 \pm 0.04\ \text{GeV}, much larger than a "natural" value Λ≃1 GeVΛ\simeq 1\ \text{GeV}. In view of this, it is difficult to interpret the nature of this new state. This state would not qualify as a resonance dynamically generated by the unitarity loops. Assuming the observed peak to correspond to a physical state, we make predictions for partners in the DD, D∗D^\ast, and B∗B^\ast sectors. Their observation (or lack thereof) would shed light into this issue.

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