We have employed Lorentz TEM (LTEM) and focal series reconstruction at multiple sample tilt angles and applied fields to investigate magnetic structures in amorphous Fe/Gd thin films.Magnetic bubbles, investigated in the 1970s as potential data storage media 1 , have seen a recent surge in scientific inquiry due to the their topological spin textures [1]. A specific type of bubble with whirling magnetic spins (see Fig. 1) called a skyrmion is the major driving force behind these investigations. Skyrmions are characterized by a non-zero chirality or topological charge, given by, where m is the normalized in-plane magnetization = ( , ) | ( , )| â . These spin textures were first observed in MnSi using neutron scattering [2][3][4]. Much of the excitement surrounding skyrmions is due to their high potential for application in spintronics [5,6]. Yu et al. observed skyrmion motion in FeGe using LTEM at current densities as low as 10 Aă»m -2 , ~10 6 orders of magnitude lower than that required to move domain walls in ferromagnetic devices making them promising for racetrack memory applications [5][6][7]. While previous magnetic skyrmion research has largely been focused on non-centrosymmetric crystals where the Dzyaloshinskii-Moriya interaction (DMI) stabilizes the skyrmion phase, here we present a LTEM study of an amorphous ferromagnetic material with perpendicular magnetic anisotropy, consisting of an Fe/Gd multilayer film.Fe a Gd b films with a = 3.4, 3.5, 3.6 Ă
b = 4.0 Ă
and 80 repeating layers were produced by sputter deposition onto a SiN window. Data was recorded in Lorentz mode using an FEI Titan equipped with an image aberration corrector. By preforming transport-of-intensity equation (TIE) analysis, the under-and over-focus LTEM images can be used to determine the in-plane magnetic induction of the sample. At zero applied field all samples have magnetic stripe/labyrinth domains shown in Figures 1b and 1c. Increasing the magnetic field applied out-of-plane causes the stripe or labyrinth domains to break up into magnetic bubble structures shown in Figure 2. These structures can be placed in three categories: type II magnetic bubbles, skyrmions, and biskyrmions, Figure 2 has examples of these three structures. Biskyrmions are a composite state formed by two skyrmions with opposite chirality for which the total topological charge is 2, and they have only been observed in La 2-2x Sr 1+2x Mn2O 7 by Yu et al. [8]. As seen in Figures 2c and j the type II bubbles and biskyrmions have very similar spin textures. Additionally, both these structures form in lines where stripe domains previously resided, similar to what was observed in La 2-2x Sr 1+2x Mn 2 O 7 [8]. The presence of biskyrmions and skyrmions with both helicities indicates that in this material these topological spin textures are stabilized by long range dipole interactions, as opposed to the Dzyaloshinskii-Moriya interaction responsible for stabilizing the skyrmion phase in non-centrosymmetric crystals such as MnSi and FeGe [9].To further investigate the stab...