The effect of imprinting symmetric and displaced vortex structures into an antiferromagnetic material is investigated in micron-sized disks consisting of exchange coupled ferromagnetic-antiferromagnetic bilayers. The imprint of displaced vortices manifests itself by the occurrence of a new type of asymmetric hysteresis loops characterized by curved, reversible, central sections with nonzero remanent magnetization. Such an imprint is achieved by cooling the disks through the blocking temperature of the system in small fields. Micromagnetic simulations reveal that asymmetric vortexlike loops naturally result from the competition between the different energies involved in the system. DOI: 10.1103/PhysRevLett.97.067201 PACS numbers: 75.60.Jk, 75.50.Ee, 75.70.Cn In ferromagnets and antiferromagnets, there are often domains with differently ordered spin states observed instead of a single homogeneously long-range ordered region. It turns out that domain structures in antiferromagnetic (AFM) materials have been far less studied than domains in ferromagnets [1]. This is partially due to the fact that the staggered AFM spin structure with its lack of a net magnetization makes the detection of domains and domain walls more challenging [2,3]. Moreover, the physical properties of AFM domains differ significantly from ferromagnetic (FM) domains. Domains in a ferromagnet are generally determined by balancing magnetostatic with exchange and anisotropy energies. Thus, in nanostructured systems, ferromagnets can develop welldefined unusual spin states, such as magnetic vortices [4 -9]. The absence of a net magnetization in antiferromagnets means that magnetostatic energy is vanishing, and, therefore, domains in antiferromagnets are generally metastable, since typically the gain in configurational entropy is not sufficient to overcome domain wall energies. Without any direct explicit driver for domain formation, the AFM domains may originate from random nucleation of long-range order due to randomly distributed defects [10]. For these reasons, the formation and evolution of AFM domains remain a research area with many open questions.Nevertheless, domains in antiferromagnets have received increased attention recently due to their role in exchange bias, i.e., the shift of the hysteresis loop observed in FM-AFM coupled systems [11,12], which is a key ingredient in spintronic devices [13]. Many exchange biased systems exhibit unusual properties, one of which is a pronounced asymmetry in the hysteresis loop, caused by different irreversible reversal mechanisms on either side of the hysteresis loop [14 -18]. Since the ferromagnet and the antiferromagnet are exchange coupled, measurements of the FM behavior provide an indirect probe of the properties of the antiferromagnet, for example, the spin-flop field [19], the surface order parameter [20], the crystalline anisotropy [21], or the domain wall width [22,23]. Furthermore, it has recently been demonstrated that nonuniformly magnetized ferromagnets can modify the antiferromagnetic s...