The temperature-dependence of the magnetization near the surface of a band-ferromagnet is measured with monolayer resolution. The simultaneous application of novel highly surface-sensitive techniques enables one to deduce the layer-dependent magnetization curves at a Fe(100) surface. Analysis of data is based on a simple mean-field approach. Implications for modern theories of itinerant-electron ferromagnetism are discussed.A ferromagnetic material is characterized by a spontaneous magnetization m which decreases with increasing temperature T until the paramagnetic state with m = 0 is reached at the Curie point T c . For very low temperatures the form of the magnetization curve m(T ) is governed by spin-wave excitations according to Bloch's law. For temperatures very close to T c critical fluctuations result in a power-law dependence m(T ) ∝ (T c − T ) β with a critical exponent β. In the wide range of intermediate temperatures the form of m(T ) depends on the specific system. In case of a band-ferromagnetic material, such as Fe as a prototype, the detailed form of m(T ) in this intermediate regime must be explained from the underlying electronic structure [1,2].Density-functional theory within the local-spin-density approximation is known to give a quantitatively accurate description of several ground-state properties [3]. For finite temperatures, however, there is no satisfying implementation available. A microscopic theory must account for the existence of local magnetic moments above T c in particular [4]. This requires to deal with correlations among itinerant valence electrons as, for example, within the framework of an orbitally degenerate Hubbard-type model with realistic parameters [5]. The long history of itinerant-electron ferromagnetism shows that this is a demanding task [2]. On the other hand, comparatively simple mean-field approaches based on spin models are known to provide a successful phenomenological description in many cases (see e. g. Ref.[6]). Remarkably, while the Weiss mean-field theory fails to reproduce the known T → 0 and T → T c limits and substantially overestimates T c , the form of the Fe magnetization curve m(T ) at intermediate reduced temperatures T /T c is reasonably well described: For spin-quantum number S = 1/2 there are deviations from the measured bulk magnetization curve of Fe within a few per cent only [7,8].At the surface of a band-ferromagnet the magnetization may be different for different layers α parallel to the surface because of the reduced translational symmetry. Hence, a key quantity that characterizes the surface magnetic structure is the layer-dependent magnetization curve m α (T ). Within the framework of classical spin models, the lowered surface coordination number implies that certain exchange interactions are missing. This directly leads to a reduced magnetic stability at the surface [9]: The top-layer (α = 1) magnetization is substantially reduced as compared with the bulk. However, significant deviations from the bulk magnetization curve are confined t...