Abstract:We report on the properties of ultrathin ͑2, 4, 6, and 8 nm͒ epitaxial films of magnetite, Fe 3 O 4 , grown on MgO ͑100͒. Atomic force microscopy image and V-I curves suggest that the films at this thickness are still continuous. The resistivity versus temperature results imply that the conductivity mechanism in all these films is similar. The resistivity of 4 nm thick film is much greater than that of 6 and 8 nm films. The films show ferrimagnetic instead of reported superparamagnetic behavior. The dead layer… Show more
“…We find that all the films down to 2 nm thickness exhibit a ferromagnetic behavior. Observation of a substantial (Giant) increase (95%) in magnetization for a 5-nm Fe O films is in stark contrast to the earlier notion of a reduction in magnetization or a superparamagnetic behavior [5], [9], [11]. Lower surface roughness of the substrates is a key to the nonobservation of superparamagnetism as opposed to previous reports.…”
Section: Resultscontrasting
confidence: 54%
“…The positive intercept on the y axis (1483 nm.emu/cm ) is the magnetic contribution to the film arising from thickness dependent contributions. Our data suggests that the earlier proposition of a dead layer model for the Fe O /MgO interface was an oversimplification [11]. The inverse thickness dependence of effective magnetization (M) given by the model (1) to separate out distinct bulk and interface contributions is questionable, in particular for the case of Fe O films on MgO (100) [11].…”
Section: Resultsmentioning
confidence: 68%
“…Our data suggests that the earlier proposition of a dead layer model for the Fe O /MgO interface was an oversimplification [11]. The inverse thickness dependence of effective magnetization (M) given by the model (1) to separate out distinct bulk and interface contributions is questionable, in particular for the case of Fe O films on MgO (100) [11]. Apart from the interfaceand surface-related contribution for ultrathin films, an additional thickness dependent magnetization contribution could result from a totally different origin, i.e., from the thickness dependence of antiphase domain size.…”
Section: Resultsmentioning
confidence: 76%
“…As the film thickness increases, the magnetization decreases. This is a curious observation in a sense that much of the earlier published work related to ultra thin magnetite films suggested either the formation of a magnetically dead layer or the presence of superparamagnetism [9], [11]. In these earlier investigations, reduction in the magnetization was ascribed to the frustrated exchange at the APBs.…”
Section: Resultsmentioning
confidence: 82%
“…A recent report by Zhou et al [11] Digital Object Identifier 10.1109/TMAG. 2008.2003173 Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org.…”
Magnetic properties as a function of film thickness (2-55 nm) for magnetite (Fe 3 O 4 ) thin films grown on MgO (100) substrates show that the small thickness films ( 5 nm) are ferromagnetic and possess magnetization values which are much greater than that of bulk Fe 3 O 4 . The inverse thickness dependence of the magnetization points to an interface related mechanism. Whereas, our detailed spin polarized density functional theoretical calculations suggests that there is only a marginal enhancement in the local spin moments of Fe-atom in the vicinity of the Fe 3 O 4 -MgO interface and it turns out that the noncompensation of spin moments between the two magnetic sublattices of spinel Fe 3 O 4 is a major factor contributing to the enhancement of magnetization.
“…We find that all the films down to 2 nm thickness exhibit a ferromagnetic behavior. Observation of a substantial (Giant) increase (95%) in magnetization for a 5-nm Fe O films is in stark contrast to the earlier notion of a reduction in magnetization or a superparamagnetic behavior [5], [9], [11]. Lower surface roughness of the substrates is a key to the nonobservation of superparamagnetism as opposed to previous reports.…”
Section: Resultscontrasting
confidence: 54%
“…The positive intercept on the y axis (1483 nm.emu/cm ) is the magnetic contribution to the film arising from thickness dependent contributions. Our data suggests that the earlier proposition of a dead layer model for the Fe O /MgO interface was an oversimplification [11]. The inverse thickness dependence of effective magnetization (M) given by the model (1) to separate out distinct bulk and interface contributions is questionable, in particular for the case of Fe O films on MgO (100) [11].…”
Section: Resultsmentioning
confidence: 68%
“…Our data suggests that the earlier proposition of a dead layer model for the Fe O /MgO interface was an oversimplification [11]. The inverse thickness dependence of effective magnetization (M) given by the model (1) to separate out distinct bulk and interface contributions is questionable, in particular for the case of Fe O films on MgO (100) [11]. Apart from the interfaceand surface-related contribution for ultrathin films, an additional thickness dependent magnetization contribution could result from a totally different origin, i.e., from the thickness dependence of antiphase domain size.…”
Section: Resultsmentioning
confidence: 76%
“…As the film thickness increases, the magnetization decreases. This is a curious observation in a sense that much of the earlier published work related to ultra thin magnetite films suggested either the formation of a magnetically dead layer or the presence of superparamagnetism [9], [11]. In these earlier investigations, reduction in the magnetization was ascribed to the frustrated exchange at the APBs.…”
Section: Resultsmentioning
confidence: 82%
“…A recent report by Zhou et al [11] Digital Object Identifier 10.1109/TMAG. 2008.2003173 Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org.…”
Magnetic properties as a function of film thickness (2-55 nm) for magnetite (Fe 3 O 4 ) thin films grown on MgO (100) substrates show that the small thickness films ( 5 nm) are ferromagnetic and possess magnetization values which are much greater than that of bulk Fe 3 O 4 . The inverse thickness dependence of the magnetization points to an interface related mechanism. Whereas, our detailed spin polarized density functional theoretical calculations suggests that there is only a marginal enhancement in the local spin moments of Fe-atom in the vicinity of the Fe 3 O 4 -MgO interface and it turns out that the noncompensation of spin moments between the two magnetic sublattices of spinel Fe 3 O 4 is a major factor contributing to the enhancement of magnetization.
Topological insulators (TIs) are of particular interest in the recent solid‐state research because of their exceptional features stemming from the conducting, topologically protected surface states. The exotic properties include the occurrence of novel quantum phenomena and make them promising materials for spintronics and quantum computing applications. Theoretical studies have provided a vast amount of valuable predictions and proposals, whose experimental observation and implementation, to date, are often hindered by an insufficient sample quality. The effect of even a relatively low concentration of defects can make the access to purely topological surface states impossible. This points out the need of high‐quality bulk‐insulating materials with ultra‐clean surfaces/interfaces, which requires sophisticated sample/device preparations as well as special precautions during the measurements. Herein, the challenging work on 3D TI thin films with a focus on is reported. It covers the optimization of the molecular beam epitaxy growth process, the in situ characterization of surface states and transport properties, the influence of exposure to ambient gases and of capping layers, as well as the effect of interfacing TI thin film with magnetic materials.
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