Ground-state energies for plaquette and dimer order in the J(1)-J(2) square
-lattice spin-half Heisenberg model are compared using series expansion met
hods. We find that these energies are remarkably close to each other at int
ermediate values of J(2)/J(1), where the model is believed to have a quantu
m disordered ground state. They join smoothly with those obtained from the
Ising expansions for the two-sublattice Neel state at J(2)/J(1) approximate
to 0.4, suggesting a second-order transition from a Neel state to a quantu
m disordered state, whereas they cross the energy for the four-sublattice o
rdered state at J(2)/J(1) approximate to 0.6 at a large angle, implying a f
irst-order transition to the four-sublattice magnetic state. The strongest
evidence that the plaquette phase is not realized in this model comes from
the analysis of the series for the singlet and triplet excitation spectra,
which suggest an instability in the plaquette phase. Thus our study support
s the recent work of Kotov et nl., which presents a strong picture for colu
mnar dimer order in this model. We also discuss the striped nature of spin
correlations in this phase, with substantial resonance all along columns of
dimers. [S0163-1829(99)06433-4].