Zusammenfassung
It was shown in [2] that the energy of the relativistic electron-positron field interacting via a second quantized Coulomb potential in Hartree-Fock approximation is positive provided the fine structure constant is not bigger than 4/pi. We show that it is instable if the fine structure constant is above this critical value. We do this partially by adapting an idea of Chair, Iracane, and Lions [4] leading to an instability problem similar to the one of the no-pair hydrogen hamiltonian [5].

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