6533b82cfe1ef96bd128edc6

RESEARCH PRODUCT

Decay widths of the spin-2 partners of the X (3872)

M. Pavon ValderramaJuan NievesFeng-kun GuoMiguel AlbaladejoC. Hidalgo-duque

subject

PhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyHadronFOS: Physical sciencesFísicaOrder (ring theory)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Quantum numberHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateHigh Energy Physics::ExperimentEngineering (miscellaneous)X(3872)Bar (unit)Spin-½

description

We consider the $X(3872)$ resonance as a $J^{PC}=1^{++}$ $D\bar D^*$ hadronic molecule. According to heavy quark spin symmetry, there will exist a partner with quantum numbers $2^{++}$, $X_{2}$, which would be a $D^*\bar D^*$ loosely bound state. The $X_{2}$ is expected to decay dominantly into $D\bar D$, $D\bar D^*$ and $\bar D D^*$ in $d$-wave. In this work, we calculate the decay widths of the $X_{2}$ resonance into the above channels, as well as those of its bottom partner, $X_{b2}$, the mass of which comes from assuming heavy flavor symmetry for the contact terms. We find partial widths of the $X_{2}$ and $X_{b2}$ of the order of a few MeV. Finally, we also study the radiative $X_2\to D\bar D^{*}\gamma$ and $X_{b2} \to \bar B B^{*}\gamma$ decays. These decay modes are more sensitive to the long-distance structure of the resonances and to the $D\bar D^{*}$ or $B\bar B^{*}$ final state interaction.

10.1140/epjc/s10052-015-3753-6http://repo.scoap3.org/api