Abstract:We report on the investigation of the exchange bias effect in Fe layers on EuTe͑111͒, an antiferromagnetic semiconductor. For this ferromagnet ͑FM͒/semiconducting antiferromagnet ͑AFM͒ exchange bias system, we have found positive and negative exchange bias effect ͑EB͒. Fresh samples exhibit positive EB, independently of the applied cooling field, indicating antiferromagnetic coupling between the FM and the AFM layers at the Fe/EuTe͑111͒ interface. The change in EB with time, from positive EB for fresh samples … Show more
“…Finally, it provides a novel explanation for the positive exchange bias and the theoretical base which has frequently been discussed in the literature. [6][7][8] This effect has been attributed to a parallel coupling of FM and AFM moments at the interface due to large cooling fields, [9][10][11] antiferromagnetic coupling at the interface, [12][13][14][15] a mainly antiferromagnetic parallel domain wall which is "unwinding" before zero field, 16 spin-glass-like particles formed spontaneously at the interface, 17 or to reversible changes in the interfacial pinning by the antiferromagnet causing an asymmetric magnetization reversal. 18 What is proposed here, however, is the simple possibility to obtain positive exchange bias in a special EB system without the need to consider directly any effects on an atomic scale.…”
The impact of a variation of anisotropy constants on the resulting coercivity and exchange bias has been analyzed modeling the total energy density in thin layered ferromagnetic/antiferromagnetic in-plane systems. For a broad range of fourfold, uniaxial, and unidirectional anisotropies, our results illustrate that the exchange bias can grow significantly for a sample rotation off the cooling field direction, while for other combinations of anisotropies, a positive exchange bias can be found near or even in the cooling field direction. These findings allow identification of anisotropies based on superconducting quantum interference device or magneto-optical Kerr effect measurements as well as tailoring desired angular dependencies for magnetoelectronic applications.
“…Finally, it provides a novel explanation for the positive exchange bias and the theoretical base which has frequently been discussed in the literature. [6][7][8] This effect has been attributed to a parallel coupling of FM and AFM moments at the interface due to large cooling fields, [9][10][11] antiferromagnetic coupling at the interface, [12][13][14][15] a mainly antiferromagnetic parallel domain wall which is "unwinding" before zero field, 16 spin-glass-like particles formed spontaneously at the interface, 17 or to reversible changes in the interfacial pinning by the antiferromagnet causing an asymmetric magnetization reversal. 18 What is proposed here, however, is the simple possibility to obtain positive exchange bias in a special EB system without the need to consider directly any effects on an atomic scale.…”
The impact of a variation of anisotropy constants on the resulting coercivity and exchange bias has been analyzed modeling the total energy density in thin layered ferromagnetic/antiferromagnetic in-plane systems. For a broad range of fourfold, uniaxial, and unidirectional anisotropies, our results illustrate that the exchange bias can grow significantly for a sample rotation off the cooling field direction, while for other combinations of anisotropies, a positive exchange bias can be found near or even in the cooling field direction. These findings allow identification of anisotropies based on superconducting quantum interference device or magneto-optical Kerr effect measurements as well as tailoring desired angular dependencies for magnetoelectronic applications.
We have studied the exchange bias at the ferromagnetic (FM)/antiferromagnetic interface in the zinc-blende transition-metal chalcogenides, CrTe (5 nm)/MnTe(40 nm) bilayer grown on GaAs (100) substrate by molecular-beam epitaxy. A negative exchange bias shift in the hysteresis loop is observed when the bilayer is cooled in the applied magnetic field. The temperature-dependent remanent magnetization shows a clear enhancement of the Curie temperature and magnetization in the bilayer as compared to a single FM layer. The effects of temperature, cooling field, and angular dependence on the exchange bias have been investigated.
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