We study the antiferromagnetic spin-1/2 Heisenberg model on a two-dimensional bipartite quasiperiodic structure, the octagonal tiling -the aperiodic equivalent of the square lattice for periodic systems. An approximate block spin renormalization scheme is described for this problem. The ground state energy and local staggered magnetizations for this system are calculated, and compared with the results of a recent Quantum Monte Carlo calculation for the tiling. It is conjectured that the ground state energy is exactly equal to that of the quantum antiferromagnet on the square lattice.PACS numbers: 75.10. Jm, 71.23.Ft, 71.27.+a In this paper a renormalization group transformation is used to study the ground state of Heisenberg spins with antiferromagnetic couplings on a two-dimensional quasiperiodic tiling. This system poses a novel theoretical problem, namely, the nature of quantum fluctuations in a structure possessing a number of exact symmetries but no translational invariance. While periodic systems and disordered variants thereof have received much attention, little is known about aperiodic quantum models in two or more dimensions. In particular, the real space magnetic ordering of local moments in systems with quasiperiodic long range order remains to be elucidated, and should present novel and complex features, different from properties of crystalline or disordered systems. The archetypal nonfrustrated two-dimensional antiferromagnetic system is that of spins on the square lattice, an old and until recently controversial problem, while the problem we consider now , with its fundamentally different symmetry properties, aims to understand a new class of unfrustrated systems.Experimental work providing motivation for the study of such systems comes from neutron scattering studies of the magnetic phase in a Zn-Mg-Ho quasicrystal [1]. The magnetic diffuse scattering of the low temperature phase shows an icosahedral symmetry, reflecting the underlying quasiperiodicity of this compound. The nature of the ground state in such a quasicrystalline medium was recently discussed in [2] where Quantum Monte Carlo (QMC) calculations were carried out for an antiferromagnetic Heisenberg model on one of the simplest twodimensional quasiperiodic tilings available, the octagonal tiling. This tiling has been frequently used for numerical investigations of the effects of quasiperiodic modulations in two dimensions. More detailed, analytic and numerical results are available for one dimensional quasiperiodic models, where quantum spins have been considered using real space renormalization transformation [3], and using density matrix renormalization or by using mappings to fermionic models (see [4] and references therein). However, the techniques used are particular to one dimension and not readily generalisable to the two-dimensional structure considered here.The model considered in [2] has a Hamiltonian H = J i,j S i . S j where the spins are located on vertices of the octagonal tiling, and J is coupling along each edge. Spin...