“…The possibility of vibration-mediated attractive interaction among confined electrons has been discussed, e.g., in the context of amorphous semiconductors [8], vacancies in silicon [9,10], fullerenes [11], and molecular junctions [12][13][14][15]. Figure 1a depicts the simplest model capturing the basic ingredients of the effect: it involves (i) a single vibrational mode (phonon), characterized by a mass m and frequency ω, (ii) a single electronic orbital that can be occupied by one or two electrons, i.e., the occupation number is N ∈ {0, 1, 2}; this orbital is characterized by an on-site energy and a repulsive Coulomb energy U > 0, (iii) the coupling between the phonon and the confined charge, characterized by the force λ encoding the coupling strength, and (iv) a (zero-temperature) electron reservoir, with Fermi energy * Corresponding author: matthias.droth@mail.bme.hu µ = 0, which can supply electrons to the orbital.…”