The problem of electron-electron lifetime in a quantum dot is studied
beyond perturbation theory by mapping onto the problem of localization
in the Fock space. Localized and delocalized regimes are identified,
corresponding to quasiparticle spectral peaks of zero and finite width
, respectively. In the localized regime, quasiparticle states are sing
le-particle-like. In the delocalized regime, each eigenstate is a supe
rposition of states with very different quasiparticle content. The tra
nsition energy is epsilon(c) similar or equal to Delta(g/ln g)(1/2), w
here Delta is mean level spacing, and g is the dimensionless conductan
ce. Near epsilon(c) there is a broad critical region not described by
the golden rule.