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Journal ArticleDOI

Manipulating the magnetism and resistance state of Mn:ZnO/Pb(Zr0.52Ti0.48)O3 heterostructured films through electric fields

Yongchao Li1, Jun Wu1, Haiyang Pan1, Jue Wang1, Guanghou Wang1, Jun-Ming Liu1, Jianguo Wan1 
23 May 2018-Applied Physics Letters (AIP Publishing LLC AIP Publishing)-Vol. 112, Iss: 21, pp 212902
TL;DR: In this article, an effective method for modulating the magnetism of magnetic semiconductors and providing a promising avenue for multifunctional devices with both electric and magnetic functionalities is presented.
Abstract: Mn:ZnO/Pb(Zr0.52Ti0.48)O3 (PZT) heterostructured films have been prepared on Pt/Ti/SiO2/Si wafers by a sol-gel process. Nonvolatile and reversible manipulation of the magnetism and resistance by electric fields has been realized. Compared with the saturation magnetic moment (Ms) in the +3.0 V case, the modulation gain of Ms can reach 270% in the −3.0 V case at room temperature. The resistance change is attributed to the interfacial potential barrier height variation and the formation of an accumulation (or depletion) layer at the Mn:ZnO/PZT interface, which can be regulated by the ferroelectric polarization direction. The magnetism of Mn:ZnO originates from bound magnetic polarons. The mobile carrier variation in Mn:ZnO, owing to interfacial polarization coupling and the ferroelectric field effect, enables the electric manipulation of the magnetism in the Mn:ZnO/PZT heterostructured films. This work presents an effective method for modulating the magnetism of magnetic semiconductors and provides a promising avenue for multifunctional devices with both electric and magnetic functionalities.
Citations
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Journal ArticleDOI
01 Aug 2019-Small
TL;DR: The mechanism of RS behavior in ferroelectric heterostructures is briefly introduced, the methods used to improve RS performance in recent years are summarized, existing problems in this field are identified, and future development trends are highlighted.
Abstract: Resistive random-access memory (RRAM) is a promising candidate for next-generation nonvolatile random-access memory protocols. The information storage in RRAM is realized by the resistive switching (RS) effect. The RS behavior of ferroelectric heterostructures is mainly controlled by polarization-dominated and defect-dominated mechanisms. Under certain conditions, these two mechanisms can have synergistic effects on RS behavior. Therefore, RS performance can be effectively improved by optimizing ferroelectricity, conductivity, and interfacial structures. Many methods have been studied to improve the RS performance of ferroelectric heterostructures. Typical approaches include doping elements into the ferroelectric layer, controlling the oxygen vacancy concentration and optimizing the thickness of the ferroelectric layer, and constructing an insertion layer at the interface. Here, the mechanism of RS behavior in ferroelectric heterostructures is briefly introduced, and the methods used to improve RS performance in recent years are summarized. Finally, existing problems in this field are identified, and future development trends are highlighted.

40 citations

Journal ArticleDOI
TL;DR: In this article, both resistive and magnetization switching were realized in Pt/NiFe1.95Cr0.05O4 (Cr-NFO)/Pt devices by the manipulation applied electric field process, where a CrNFO switching layer was prepared by a facile chemical solution process method.
Abstract: In this letter, both resistive and magnetization switching were realized in Pt/NiFe1.95Cr0.05O4 (Cr-NFO)/Pt devices by the manipulation applied electric field process, where a Cr-NFO switching layer was prepared by a facile chemical solution process method. The Cr-NFO based devices exhibited stable unipolar switching behavior, uniform operating voltages, good endurance (>103 cycles), large ON/OFF memory window (>102), and excellent retention characteristic time (>105 s at 25 °C). Meanwhile, the saturation magnetization of Cr-NFO based devices showed reversible switching in different resistance states. The significant change between the high magnetization state and the low magnetization state could reach as high as ∼50% during resistive switching operation. The ON-OFF switching can be achieved at room temperature in resistive and magnetization switching. The proposed physical mechanism of resistive and magnetized switching of Cr-NFO based devices was related to the formation and rupture of conduction filaments consisting of oxygen vacancies and cations, which was based on the conversion of Fe (Fe3+ → Fe2+) and Cr (Cr3+ → Cr4+) valence change, redox reaction, and Joule heating effects. The coexistence of resistive and magnetization switching in ferrite thin film based devices has potential application in nonvolatile memory and magneto-electric coupling devices.

17 citations

Journal ArticleDOI
TL;DR: In this paper, the anomalous photovoltaic effect and resistive switching behaviors in ferroelectric materials attract much attention in recent years, and the conductive mechanisms and research progresses of the two effects were discussed in this study.
Abstract: The anomalous photovoltaic effect and resistive switching behaviors in ferroelectric materials attract much attention in recent years. Dozens of researches revealed that the two effects coexist and affect each other in electrode/ferroelectric/electrode structures. Therefore, the conductive mechanisms and research progresses of the two effects were discussed in this study, which suggested the interface coupling effect caused by polarization states led to switchable photovoltaic and different resistance states. On the other hand, electrode/ferroelectric/electrode structures have great potential in the application of high-density memories, and a novel non-volatile optoelectronic memory which can write multiple storage states and read information non-destructively can be realized by exploiting the two effects properly.

7 citations

Journal ArticleDOI
TL;DR: In this article , the authors present a review of three physical mechanisms which lead to resistive switching: electrochemical metallization, valence change mechanism, and ferroelectric polarization.
Abstract: Resistive random access memory (ReRAM) would be an important component of microelectronics in the era of big data storage due to its efficient characteristics such as low cost, fast operating speed, low power consumption, and high performance in respect of endurance and retention. In this present review, we have focused on surveying three physical mechanisms which lead to resistive switching: electrochemical metallization, valence change mechanism, and ferroelectric polarization. A detailed discussion has been carried out on how these physical mechanisms work in various materials used for resistive switching based on nonvolatile random access memory (NVRAM) elements such as oxides, ferroelectric, chalcogenides, polymers, graphene-based resistive switching, etc. The desirable electrical and optical properties for the representation of analog resistive switching in neuromorphic computing have also been discussed. An extensive report has examined the device requirement of different materials for artificial memristors.

7 citations

Journal ArticleDOI
TL;DR: For the first time, a weak ferromagnetic hysteresis loop at room temperature has been observed in PbZr1−xTixO3 (PZT) single crystals.
Abstract: For the first time, a weak ferromagnetic hysteresis loop at room temperature has been observed in PbZr1−xTixO3 (PZT) single crystals. The occurrence of these properties has been related to the presence of oxygen vacancies and/or lower oxidation state of titanium. This proves that ferroelectric and ferromagnetic properties can occur simultaneously in this “famous” piezoelectric perovskite without any magnetic dopant.

5 citations

References
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Journal ArticleDOI
TL;DR: The semiconductor ZnO has gained substantial interest in the research community in part because of its large exciton binding energy (60meV) which could lead to lasing action based on exciton recombination even above room temperature.
Abstract: The semiconductor ZnO has gained substantial interest in the research community in part because of its large exciton binding energy (60meV) which could lead to lasing action based on exciton recombination even above room temperature. Even though research focusing on ZnO goes back many decades, the renewed interest is fueled by availability of high-quality substrates and reports of p-type conduction and ferromagnetic behavior when doped with transitions metals, both of which remain controversial. It is this renewed interest in ZnO which forms the basis of this review. As mentioned already, ZnO is not new to the semiconductor field, with studies of its lattice parameter dating back to 1935 by Bunn [Proc. Phys. Soc. London 47, 836 (1935)], studies of its vibrational properties with Raman scattering in 1966 by Damen et al. [Phys. Rev. 142, 570 (1966)], detailed optical studies in 1954 by Mollwo [Z. Angew. Phys. 6, 257 (1954)], and its growth by chemical-vapor transport in 1970 by Galli and Coker [Appl. Phys. ...

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Journal ArticleDOI
17 Aug 2006-Nature
TL;DR: A ferroelectric crystal exhibits a stable and switchable electrical polarization that is manifested in the form of cooperative atomic displacements that arises through the quantum mechanical phenomenon of exchange.
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6,813 citations

Journal ArticleDOI
TL;DR: In this article, the status of zinc oxide as a semiconductor is discussed and the role of impurities and defects in the electrical conductivity of ZnO is discussed, as well as the possible causes of unintentional n-type conductivity.
Abstract: In the past ten years we have witnessed a revival of, and subsequent rapid expansion in, the research on zinc oxide (ZnO) as a semiconductor. Being initially considered as a substrate for GaN and related alloys, the availability of high-quality large bulk single crystals, the strong luminescence demonstrated in optically pumped lasers and the prospects of gaining control over its electrical conductivity have led a large number of groups to turn their research for electronic and photonic devices to ZnO in its own right. The high electron mobility, high thermal conductivity, wide and direct band gap and large exciton binding energy make ZnO suitable for a wide range of devices, including transparent thin-film transistors, photodetectors, light-emitting diodes and laser diodes that operate in the blue and ultraviolet region of the spectrum. In spite of the recent rapid developments, controlling the electrical conductivity of ZnO has remained a major challenge. While a number of research groups have reported achieving p-type ZnO, there are still problems concerning the reproducibility of the results and the stability of the p-type conductivity. Even the cause of the commonly observed unintentional n-type conductivity in as-grown ZnO is still under debate. One approach to address these issues consists of growing high-quality single crystalline bulk and thin films in which the concentrations of impurities and intrinsic defects are controlled. In this review we discuss the status of ZnO as a semiconductor. We first discuss the growth of bulk and epitaxial films, growth conditions and their influence on the incorporation of native defects and impurities. We then present the theory of doping and native defects in ZnO based on density-functional calculations, discussing the stability and electronic structure of native point defects and impurities and their influence on the electrical conductivity and optical properties of ZnO. We pay special attention to the possible causes of the unintentional n-type conductivity, emphasize the role of impurities, critically review the current status of p-type doping and address possible routes to controlling the electrical conductivity in ZnO. Finally, we discuss band-gap engineering using MgZnO and CdZnO alloys.

3,291 citations

Journal ArticleDOI
TL;DR: In this paper, the fundamental physics behind the scarcity of ferromagnetic ferroelectric coexistence was explored and the properties of known magnetically ordered ferro-electric materials were examined.
Abstract: Multiferroic magnetoelectrics are materials that are both ferromagnetic and ferroelectric in the same phase. As a result, they have a spontaneous magnetization that can be switched by an applied magnetic field, a spontaneous polarization that can be switched by an applied electric field, and often some coupling between the two. Very few exist in nature or have been synthesized in the laboratory. In this paper, we explore the fundamental physics behind the scarcity of ferromagnetic ferroelectric coexistence. In addition, we examine the properties of some known magnetically ordered ferroelectric materials. We find that, in general, the transition metal d electrons, which are essential for magnetism, reduce the tendency for off-center ferroelectric distortion. Consequently, an additional electronic or structural driving force must be present for ferromagnetism and ferroelectricity to occur simultaneously.

3,146 citations

Journal ArticleDOI
TL;DR: It is proposed thatferromagnetic exchange here, and in dilute ferromagnetic nitrides, is mediated by shallow donor electrons that form bound magnetic polarons, which overlap to create a spin-split impurity band.
Abstract: Dilute ferromagnetic oxides having Curie temperatures far in excess of 300 K and exceptionally large ordered moments per transition-metal cation challenge our understanding of magnetism in solids. These materials are high-k dielectrics with degenerate or thermally activated n-type semiconductivity. Conventional super-exchange or double-exchange interactions cannot produce long-range magnetic order at concentrations of magnetic cations of a few percent. We propose that ferromagnetic exchange here, and in dilute ferromagnetic nitrides, is mediated by shallow donor electrons that form bound magnetic polarons, which overlap to create a spin-split impurity band. The Curie temperature in the mean-field approximation varies as (xdelta)(1/2) where x and delta are the concentrations of magnetic cations and donors, respectively. High Curie temperatures arise only when empty minority-spin or majority-spin d states lie at the Fermi level in the impurity band. The magnetic phase diagram includes regions of semiconducting and metallic ferromagnetism, cluster paramagnetism, spin glass and canted antiferromagnetism.

2,743 citations