文摘
We have studied the structure of K−pp by solving this system in a variational treatment, starting from Ansatz that x39b;(1405) is a K−p quasi-bound state, x39b;* with mass 1405 MeV/c2. The structure of K−pp reveals a molecular feature, namely, the K− in an “atomic center”, x39b;*, plays a key role in producing strong covalent bonding with the other proton. Deeply bound nuclear systems are formed by this “super-strong” nuclear force due to migrating real bosons, , a la Heitler-London-Heisenberg, which overcompensates the stiff nuclear incompressibility. Theoretical background of the x39b;(1405) Ansatz is discussed in connection with the double-pole picture of x39b;(1405) based on chiral SU(3) dynamics. Detailed analysis reveals single-pole nature of the observable x39b;(1405). There are two kinds of Σπ invariant masses experimentally observable, the usual T22 invariant mass and the conversion T21 invariant mass. It is of virtual importance to determine whether the x39b;* mass is 1405 MeV or 1420 MeV. The T21 invariant mass from K− absorption at rest in deuteron can provide decisive information about this x39b;* mass problem.