Abstract:Pairing two-dimensional semiconductors with ferroelectric films may allow for the development of hybrid electronic devices that would not only exhibit a combination of the functional properties of both material groups but would also reveal unusual characteristics emerging from coupling between these properties. Here, we report the observation of a considerable (up to 103 at 0.8 V read bias) polarization-mediated tunneling electroresistance (TER) effect in Hf0.5Zr0.5O2 (HZO) ferroelectric tunnel junctions (FTJs… Show more
“…[2] Already, a few technological developments using HfO 2based films have been demonstrated: ferroelectric field effect in transistors with the 28-nm gate length, [3] fast and hysteresis-free negative capacitance, [4][5][6][7][8] as well as tunneling electroresistance effect. [9][10][11][12][13][14] Since functionality of the FE-based devices in most cases depends on the electrical switching of the spontaneous polarization, increasing application of the HfO 2 -based FE films calls for a better understanding of the mechanism of polarization reversal in these materials, which is far from being understood. [15][16][17][18] For example, hysteresisfree negative capacitance can only occur if the polarization switches intrinsically, i.e., without domain nucleation and growth.…”
One of the general features of ferroelectric systems is a complex nature of polarization reversal, which involves domain nucleation and motion of domain walls. Here, time‐resolved nanoscale domain imaging is applied in conjunction with the integral switching current measurements to investigate the mechanism of polarization reversal in yttrium‐doped HfO2 (Y:HfO2)—currently one of the most actively studied ferroelectric systems. More specifically, the effect of film microstructure on the nucleation process is investigated by performing a comparative study of the polarization switching behavior in the epitaxial and polycrystalline Y:HfO2 thin film capacitors. It is found that although the epitaxial Y:HfO2 capacitors tend to switch slower than their polycrystalline counterparts, they exhibit a significantly higher nucleation density and rate, suggesting that this is a rate‐limiting mechanism. In addition, it is observed that under the external fields approaching the activation field value, the switching kinetics can be described equally well by the nucleation limited switching and the Kolmogorov‐Avrami‐Ishibashi models for both types of capacitors. This signifies convergence of two different mechanisms implying that the polarization reversal proceeds via a homogeneous nucleation process unaffected by the film microstructure, which can be considered as approaching the intrinsic switching limit.
“…[2] Already, a few technological developments using HfO 2based films have been demonstrated: ferroelectric field effect in transistors with the 28-nm gate length, [3] fast and hysteresis-free negative capacitance, [4][5][6][7][8] as well as tunneling electroresistance effect. [9][10][11][12][13][14] Since functionality of the FE-based devices in most cases depends on the electrical switching of the spontaneous polarization, increasing application of the HfO 2 -based FE films calls for a better understanding of the mechanism of polarization reversal in these materials, which is far from being understood. [15][16][17][18] For example, hysteresisfree negative capacitance can only occur if the polarization switches intrinsically, i.e., without domain nucleation and growth.…”
One of the general features of ferroelectric systems is a complex nature of polarization reversal, which involves domain nucleation and motion of domain walls. Here, time‐resolved nanoscale domain imaging is applied in conjunction with the integral switching current measurements to investigate the mechanism of polarization reversal in yttrium‐doped HfO2 (Y:HfO2)—currently one of the most actively studied ferroelectric systems. More specifically, the effect of film microstructure on the nucleation process is investigated by performing a comparative study of the polarization switching behavior in the epitaxial and polycrystalline Y:HfO2 thin film capacitors. It is found that although the epitaxial Y:HfO2 capacitors tend to switch slower than their polycrystalline counterparts, they exhibit a significantly higher nucleation density and rate, suggesting that this is a rate‐limiting mechanism. In addition, it is observed that under the external fields approaching the activation field value, the switching kinetics can be described equally well by the nucleation limited switching and the Kolmogorov‐Avrami‐Ishibashi models for both types of capacitors. This signifies convergence of two different mechanisms implying that the polarization reversal proceeds via a homogeneous nucleation process unaffected by the film microstructure, which can be considered as approaching the intrinsic switching limit.
“…The proposed approach could be useful not only for the design of conventional highdensity FRAM and FTJ memory but also for the development of novel devices based on tunnel-transparent ferroelectrics, which require functional materials that suppress ferroelectricity in hafnium oxide (e.g., graphene and other two-dimensional materials [25][26][27]).…”
The development of the new generation of non-volatile high-density ferroelectric memory requires the utilization of ultrathin ferroelectric films. The most promising candidates are polycrystalline-doped HfO2 films because of their perfect compatibility with silicon technology and excellent ferroelectric properties. However, the remanent polarization of HfO2 films is known to degrade when their thickness is reduced to a few nanometers. One of the reasons for this phenomenon is the wake-up effect, which is more pronounced in the thinner the film. For the ultrathin HfO2 films, it can be so long-lasting that degradation occurs even before the wake-up procedure is completed. In this work, an approach to suppress the wake-up in ultrathin Hf0.5Zr0.5O2 films is elucidated. By engineering internal built-in fields in an as-prepared structure, a stable ferroelectricity without a wake-up effect is induced in 4.5 nm thick Hf0.5Zr0.5O2 film. By analysis of the functional characteristics of ferroelectric structures with a different pattern of internal built-in fields and their comparison with the results of in situ piezoresponse force microscopy and synchrotron X-ray micro-diffraction, the important role of built-in fields in ferroelectricity of ultrathin Hf0.5Zr0.5O2 films as well as the origin of stable ferroelectric properties is revealed.
“…Semiconductors are also crucial for forming a Schottky barrier to obtain a higher TER, which is essential for the FTJ. [19][20][21][22][23][24] For vertical structured FTJ devices, an enhanced TER (∼ 10 3 -10 4 ) can be obtained using the ferroelectric/semiconductor heterojunction. [22][23][24] To the best of our knowledge, no lateral structured ferroelectric/semiconductor FTJ with a higher TER (> 10 4 ) has been reported.…”
Modulation between optical and ferroelectric properties was realized in a lateral structured ferroelectric CuInP2S6 (CIPS)/semiconductor MoS2 van der Waals (vdW) heterojunction. The ferroelectric hysteresis loop area was modulated by the optical field. Two types of photodetection properties were realized in a device by changing the ON and OFF states of the ferroelectric layer. The device was used as a photodetector in the OFF state but not in the ON state. Higher tunnelling electroresistance (TER) (~1.4×104) in a lateral structured ferroelectric tunnelling junction was crucial, and it was analyzed and modulated by the barrier height and width of the ferroelectric CIPS/semiconductor MoS2 Schottky junction. The new parameter of the ferroelectric hysteresis loop area as a function of light intensity was introduced to analyze the relationship between the ferroelectric and photodetection properties. The proposed device has potential application as optoelectronic sensory cells in the biological nervous system or as a new type of photodetector.
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