I critically overview my research on strongly correlated fermion systems for almost five decades. It concentrated on: (i) the first derivation of what is now called the \(t\)–\(J\) model, comprising both the limit of Anderson kinetic exchange of spin–spin interaction in the Mott–Hubbard insulator and taking into account real-space pairing, subsequently applied to high-temperature superconductivity; (ii) the concept of spin-dependent heavy mass of quasiparticles in heavy-fermion systems, and (iii) the first nontrivial model of statistical thermodynamics of the Mott–Hubbard transition. Those three features, together with the specific quantum critical phenomena provide, in my view, fundamental components of the theory of strongly correlated fermions established in the 1960s. Some related questions such as introduction of atomicity in the chemical bonding (iv), and specific properties of correlated nanosystems within rigorous EDABI approach (v) are also briefly elaborated at the end. Abstract Published by the Jagiellonian University 2026 authors
J. Spałek (Fri,) studied this question.