  A heavy hadron traversing Quark-Gluon Plasma and dragged along in rotational
motion is subject to the Lorentz and centrifugal forces. The Lorentz force,
sourced by the valence quarks of heavy-ions, possesses the electric and
magnetic components in the hadron comoving frame. The electric component
renders the hadron unstable by empowering one of its quarks to tunnel through
the potential barrier. Assuming that the magnetic field is parallel to the
plasma vorticity, the hadron dissociation probability is computed using the
Imaginary Time Method and is found to strongly depend on the sign of the quark
electric charge. The dissociation probability monotonically increases as a
function of vorticity for negative electric charges, whereas for positive
charges it exhibits a minimum at a finite value of vorticity. The dissociation
probability for the negative charges is larger than for the positive ones at
the same magnetic field and vorticity. In relativistic heavy-ion collisions
this implies lower abundance of the negatively charged hadrons as compared to
the positively charges ones. This effect is significant at moderate collision
energies where the plasma vorticity is comparable or larger than the
synchrotron frequency.
