We study the interplay between a (quasi) periodic coupling array and an external magnetic field in a spin- The magnetic properties of quasi-crystals have become a fundamental issue of study since their discovery in 1984 [1]. A variety of theoretical efforts, ranging from renormalization group (RG) analysis of Ising models in Penrose lattices [2] to exact solutions of both Ising and XY Fibonacci spin chains [3][4][5] have revealed fairly intricate magnetic orderings associated to the quasi-periodicity of these structures. The non-metallic spin exchange mechanism implicit in those studies has been evidenced in recently synthesized rare earth (R) ZnMg-R quasi-crystals (see e.g. [6]) whose R elements have well localized 4f magnetic moments.Bolstered by these latter findings and as a further step within the line of the local moment descriptions referred to above, here we consider the ordering of quasi-periodic spin-1 2 XXZ chains in a magnetic field to elucidate the quantization conditions of massive spin excitations or magnetization plateaux. In periodic systems, this issue has received systematic attention in the last few years from both experimental and theoretical points of view (see e.g. [7]). In this letter, we are specifically interested in studying the antiferromagnetic systemwhere S x , S y , S z denote the spin-1 2 matrices involved in the standard XXZ Hamiltonian (ǫ n = 0 ) in a magnetic field h applied along the anisotropy direction ( |∆| ≤ 1 ). Here, the coupling modulation is introduced via the ǫ n parameters defined as ǫ n = ν δ ν cos (2π ω ν n ) , so quasi-periodicity arises upon choosing an irrational subset of frequencies ω ν with amplitudes δ ν .The interest of (1) stems partly from the widespread applications of 1d Hamiltonians in the description of artificially grown quasi-periodic heterostructures [8], quantum dot crystals [9] and magnetic multilayers [10]. Also, recent investigations of quasi-periodicity involving either the couplings [11] or the magnetic field [12], have been addressed using Abelian bosonization along with RG and numerical techniques. Here we focus on the combined effect of a quasi-periodic exchange modulation under a uniform magnetic field.Of particular importance are the rational frequencies of (1), not only as a way to approach the quasi-periodic limit, but also because they allow for a thorough numerical verification of a novel situation (see [13][14][15] for related work). As we shall see, although the allowed fractional plateaux predicted in the present case fall into the classification provided by the generalized Lieb-Schultz-Mattis theorem [16], a bosonization approach to (1) yields an alternative scenario not envisaged in previous studies [17,18]. This will be reflected in the appearance of magnetization plateaux associated to each of the frequencies present in (1). To strengthen the potential interest of our results, we show how a simple two frequency model exhibits a magnetization curve with two wide plateaux at