Figure 1
From: Revealing noncollinear magnetic ordering at the atomic scale via XMCD
(a) Mass-to-charge spectrum of cluster ions up to n=2, produced from the FeV target. (b) Left: sketch of the soft landing procedure. Right: schematic view of the measurement geometry after the Kr buffer is removed by flash heating to 120 K. The angle \(\theta \) between the surface normal and the incoming photon beam is varied between 0 \(^{\circ }\) and 70 \(^{\circ }\). The magnetic field strength B was alternated between \(-7\) and \(+7\) T. Background corrected white line spectra taken at \(\theta \)=0\(^\circ \) and \(\theta \)=70\(^\circ \) for V\(_1\)/Cu(001) (c) and Fe\(_1\)/Cu(001) (d). (e) and (f) are the XMCD spectra corresponding to (c) and (d). All spectra are normalized to the \(L_3\) peak value of the corresponding white line spectrum and vertically offset for better visibility.
