Abstract
We discuss the structure of strong interactions emerging from quark-confining anisotropic chromodynamics (ACD). We show that i) the finite-energy states (the hadrons) are described by quarks, arranged in colour singlets, and moving in linear configurations; ii) a natural perturbative structure emerges which fully supports the ideas of the quark model; and iii) the meson\((q\bar q)\) spectrum is given by a Schrodinger-like equation with relativistic kinematics and a «potential» increasing linearly with the relative distance.
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