$P$-wave coupled-channel scattering of $B_s\pi ,B_s^{\ast }\pi ,B\overline{K},B^{\ast }\overline{K}$ and the puzzling $X(5568)$

Abstract

The D0 Collaboration has recently reported a narrow peak structure in the $B_s^0{\pi }^{\pm }$ invariant-mass spectrum, that is called $X(5568)$. Its proposed quantum numbers $J^P=0^{+}/1^{+}$ are not determined unambiguously, and we show that one can fit the data assuming $J^P=1^{-}$ with the same mass and width for the resonance signal. The corresponding isovector $P$-wave coupled-channel scattering involving the states $B_s\pi$, $B_s^{\ast }\pi$, $B\overline{K}$ and $B^{\ast }\overline{K}$ is studied employing leading-order Heavy Meson Chiral Perturbation Theory, which is then unitarized making use of standard techniques from Unitary Chiral Perturbation Theory. The subtraction constants that appear in the unitarization process are determined by a $u$-channel crossing symmetry constraint or by naturalness arguments, being the numerical values obtained in both cases quite closed, and no further freedom is left in the model. A crucial point is that if the $X(5568)$ is $1^{-}$ and decaying into $B_s^0{\pi }^{\pm }$ then it should appear as a pole in the $T$-matrix elements. It finally turns out that no $X(5568)$ pole is found that can be qualified as dynamically generated from the isovector $P$-wave coupled-channel dynamics. This result disfavors the interpretation of the $X(5568)$ within a "molecular" picture.

Comments: 10 pages, 3 figures