The energies of the bound states and energies and widths of autoionizi
ng resonant states of helium are calculated within the s-wave model, w
here the individual orbital angular momenta of both electrons are zero
. The energies of the bound 1sns states differ from the corresponding
energies in real helium only via a small n-independent shift Delta mu
in the quantum defects, which amounts to Delta mu=0.011 for singlet st
ates and Delta mu=0.004 for triplet states. The quantum defects of mor
e than 50 bound and resonant states with singlet or triplet symmetry a
re reproduced by an empirical four-parameter formula to within an rms
deviation of less than 0.016. The normalized widths of the autoionizin
g Nsns resonant states increase with the smaller quantum number N, and
the widths of the singlet states tend to become larger than the separ
ation of successive resonances in the Rydberg series for N approximate
to 8. Effects of interference of Rydberg series can be described in t
he framework of multichannel quantum-defect theory. In the 7sns single
t series of resonances, interference due to the 8s8s perturber inhibit
s autoionization by more than three powers of IO. Semiclassical quanti
zation based on unstable periodic orbits reproduces the energies of st
ates with equal or similar quantum numbers rather well in a standard a
pplication of the cycle-expansion technique and very well in an applic
ation using only three nonretracing periodic orbits.