The ground-state properties of the quasi-one-dimensional spin-
1/2 antiferromagnetic Heisenberg model is investigated by using a variational method. Spins on chains along the
x direction are antiferromagnetically coupled with exchange
J>0, while spins between chains in the
y direction are coupled either ferromagnetically (${J}^{\ensuremath{'}}<0$) or antiferromagnetically (${J}^{\ensuremath{'}}>0$). The staggered and the colinear antiferromagnetic magnetizations are computed and their dependence on the anisotropy parameter $\ensuremath{\lambda}=|{J}^{\ensuremath{'}}|/J$ is analyzed. It is found that an infinitesimal interchain coupling parameter is sufficient to stabilize a long-range order with either a staggered magnetization
ms (${J}^{\ensuremath{'}}>0$) or a colinear antiferromagnetic magnetization
mcaf (${J}^{\ensuremath{'}}<0$), both behaving as $\ensuremath{\simeq}{\ensuremath{\lambda}}^{1/2}$ for $\ensuremath{\lambda}\ensuremath{\rightarrow}0$.
Effects of the site dilution on spin-gapped Heisenberg antiferromagnets with
S=21 and
S=1 on a square lattice of coupled dimerized chains are investigated by means of the quantum Monte Carlo method. It is found that effective magnetic moments induced around the diluted sites exhibit the antiferromagnetic long-range order in the medium of spin-singlet pairs. Their microscopic structure is examined in detail and important roles of higher dimensionality other than one in the phenomenon are discussed.