We study the properties of spectra and eigenfunctions for a chain of 1/2 sp
ins (qubits) in an external time-dependent magnetic field and under the con
ditions of nonselective excitation (when the amplitude of the magnetic fiel
d is large). This model is known as a possible candidate for experimental r
ealization of quantum computation. We present the theory for finding deloca
lization transitions and show that for the interaction between nearest qubi
ts, the transition is very different from that in quantum chaos. We explain
this phenomena by showing that in the considered region of parameters our
model is close to an integrable one. According to a general opinion, the th
reshold for the onset of quantum chaos due to the interqubit interaction de
creases with an increase of the number of qubits. Contrary to this expectat
ion, for a magnetic field with constant gradient we have found that chaos b
order does not depend on the number of qubits. We give analytical estimates
that explain this effect, together with numerical data supporting our anal
ysis. Random models with long-range interactions have been studied as well.
In particular, we show that in this case the delocalization and quantum ch
aos borders coincide.