threshold at 2363 MeV E = sqrt( p2+mD2 ) + sqrt( p2+mK2 ) We vary continuously the model's coupling constant from a small (0.60) towards a large value (1.2). In the complex-momentum (p) plane we observe that the pole turns purely imaginary somewhere in the lower half-plane. This is typical for S-wave scattering. For any higher angular momentum this happens at p=0. The scattering-matrix singularity represents a bound-state pole when it lies on the positive imaginary axis. On the negative imaginary axis it represents a virtual bound state. |