We model an isolated quantum computer as a two-dimensional lattice of qubit
s (spin halves) with fluctuations in individual qubit energies and residual
short-range inter-qubit couplings. In the limit when fluctuations and coup
lings are small compared to the one-qubit energy spacing, the spectrum has
a band structure and we study the quantum computer core (central band) with
the highest density of states. Above a critical inter-qubit coupling stren
gth, quantum chaos sets in, leading to quantum ergodicity of eigenstates in
an isolated quantum computer. The onset of chaos results in the interactio
n induced dynamical thermalization and the occupation numbers well describe
d by the Fermi-Dirac distribution. This thermalization destroys the noninte
racting qubit structure and sets serious requirements for the quantum compu
ter operability.