Unlike X, the wave function extent of XX is determined mainly by the diameter of the embedded QRs.
This means that the wave function extent of X is determined mainly by the confinement of the potential valley and the Coulomb interaction.
Furthermore, the difference was found to scale as the cube of its single-particle wave function extent and therefore can be a sensitive probe to the electron-hole wave function asymmetry.
The anomalous behavior is attributed to the apparent change in the electron wave function extent after photon emission due to the strong Coulomb attraction by the hole in its initial state.
Such anomalous behaviors for X− were explained by the apparent change in the electron wave function extent after photon emission due to the strong Coulomb attraction induced by the hole in its initial state.
As for the magnetic response of X− in QDs, we observe an anomalous diamagnetic behavior, which cannot be described by the conventional quadratic energy shift with the applied B. Such anomalous behaviors for X− can be attributed to the apparent change in the electron wave function extent after photon emission due to the strong Coulomb attraction by the hole in its initial state.
To explain this behavior, we consider here a 2D parabolic potential as the effective lateral confinement for both electrons and holes in the QDs, with a quantization energy of ℏω β and a wave function extent of, where β denotes e or h and m β are the effective masses [20, 21].
Age, sex, preoperative pulmonary function, extent of resection, diagnosis, need for reoperation and inotropic requirements were not predictors of poor outcome.
Figure 6 shows the results of simulations of the focal intensity distributions when only accounting for the aberrations of the parabolic mirror but neglecting the trapped ion's wave function finite extent.
This phenomenon is not expected for X+ in QDs, since the wave function extents of the initial- and final-state holes are almost identical due to the fact that hole has a larger effective mass, such that the hole wave function remains well confined even in small QDs.
