Abstract
We propose a new power counting for the effective field theory describing a near-threshold state with unstable constituents, such as the X(3872) meson. In this counting, the momenta of the heavy particles, the pion mass and the excitation energy of the unstable constituent-the D* in the case of the X-are treated as small scales, of order Q. The difference delta between the excitation energy of the D* and the pion mass is smaller than either by a factor similar to 20. We therefore assign delta an order Q(2) in our counting. This provides a consistent framework for a double expansion in both delta/m(pi) and the ratio of m(pi) to the high-energy scales in this system. It ensures that amplitudes have the correct behavior at the three-body threshold. It allows us to derive, within an effective theory, various results which have previously been obtained using physically motivated approximations.