The few-particle state of carriers confined in a quantum dot is controlled
by the balance between their kinetic energy and their Coulomb correlation.
In coupled quantum dots, both can be tuned by varying the inter-dot tunneli
ng and interactions. Using a theoretical approach based on the diagonalizat
ion of the exact Hamiltonian, we show that the transitions between differen
t quantum phases can be induced through the inter-dot coupling both for a s
ystem of few electrons (or holes) and for aggregates of electrons and holes
. We discuss their manifestations, in addition energy spectra (accessible t
hrough capacitance or transport experiments) and optical spectra. (C) 2001
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