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LauraB Candy Doll Collection 8 B CDCL 008 307et\]), and the continuum single-electron and single-hole states merge at filling $N=8$.

![The maximum $2e$-exciton binding energy ($E_{2e}$) \[(a) and (b)\] and the ground-state momentum of the $2e$-exciton ($K_{2e}$) \[(c) and (d)\] as a function of the filling. The data are obtained from unrestricted Hartree-Fock calculations for the cluster-assembled In$_{N_{\rm x}}$Ga$_{N_{\rm x}+1}$As quantum wells. The horizontal line in each panel represents the continuum single-electron ($E_{\rm 1e}$) and single-hole ($E_{\rm 1h}$) threshold energies ($E_{\rm th}$).[]{data-label=”fig:1″}](figure1.eps)

The origin of the formation of the long-lived $2e$-exciton state is due to the weakening of the Coulomb interaction at filling $N=8$ \[Fig. \[fig:1\](a)\]. However, the relationship between the spin and the parity of the $2e$-exciton is different from that in the cluster-assembled electron-hole system, and, in particular, the ground state of the $2e$-exciton is the singlet for $N_{\rm x}=5$ and $N_{\rm x}=6$ even though it has the spin triplet. The details of the $2e$-exciton ground state will be described elsewhere [@comment1]. It is well known that the Coulomb interaction becomes very weak for single-particle states with higher angular momenta ($l>1$). This strong weakening of the Coulomb interaction for higher angular momenta is one of the most common characteristics of the electron-

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