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1.
余志强  刘敏丽  郎建勋  钱楷  张昌华 《物理学报》2018,67(15):157302-157302
采用简单的一步水热法在FTO导电玻璃上外延生长了锐钛矿TiO_2纳米线,制备了具有Au/TiO_2/FTO器件结构的锐钛矿TiO_2纳米线忆阻器,系统研究了器件的阻变开关特性和开关机理.结果表明,Au/TiO_2/FTO忆阻器具有非易失的双极性阻变开关特性.同时,在103s的时间内,器件在0.1 V的电阻开关比始终保持在20以上,表明器件具有良好的非易失性.此外,器件在低阻态时遵循欧姆导电特性,而在高阻态时则满足陷阱控制的空间电荷限制电流传导机制,同时提出了基于氧空位导电细丝形成与断开机制的阻变开关模型.研究结果表明Au/TiO_2/FTO忆阻器将是一种很有发展潜力的下一代非易失性存储器.  相似文献   

2.
杨帆  韦敏  邓宏  杨胜辉  刘冲 《发光学报》2014,35(5):604-607
以 ZnO:Al为底电极,Cu为顶电极,在同种工艺条件下分别制备了类电容结构的纯ZnO 阻变器件和ZnO:2%Cu阻变器件,分析比较了两种器件的典型I-V特性曲线、置位电压(VSet)和复位电压(VReset)的分布范围、器件的耐久性。结果显示,ZnO:Cu阻变器件较纯ZnO阻变器件有更大的开关比和更稳定的循环性能。另外,研究了 ZnO:Cu阻变器件的阻变机理,通过对其I-V特性曲线分析得出以下结论:ZnO:Cu阻变器件在高阻态遵循空间电荷限制电流效应,低阻态符合欧姆定律。  相似文献   

3.
韦晓莹  胡明  张楷亮*  王芳  刘凯 《物理学报》2013,62(4):47201-047201
采用射频反应溅射法于室温下在Cu/Ti/SiO2/Si基底上制备了氧化钒薄膜. X-射线衍射、X射线光电子能谱分析仪及原子力显微镜结果表明, 室温下制备的氧化钒薄膜除微弱的V2O5 (101)和V2O3 (110)峰外, 没有明显的结晶取向, 是VO2, V2O5, V2O3及VO的混合相薄膜, 且薄膜表面颗粒大小均匀, 表面均方根粗糙度约为1 nm. 采用半导体参数分析仪对薄膜的电开关特性进行测试. 结果表明薄膜具有较低的开关电压(VSet<1 V, VReset<-0.5 V), 并且具有稳定的可逆开关特性. 薄膜从低阻态转变为高阻态的电流(IReset)随限流的增大而增大.通过高低阻态时I-V对数曲线的拟合(高阻态斜率>1, 低阻态斜率=1), 认为Cu离子在薄膜中扩散形成的导电细丝是该体系发生电阻转变的主要机制. 关键词: 氧化钒薄膜 电阻开关 电阻式非挥发存储器 导电细丝  相似文献   

4.
制备了一种具有多级存储效应的密集ZnO纳米棒阵列阻变存储器件,借助I-V曲线和荧光光谱分析了器件的电流传导机制和阻变机制,发现器件在不同的电阻态下分别属于欧姆传导和空间电荷限制电流( SCLC)传导机制。正向电场作用使纳米棒表面耗尽区的氧空位V++密度增大,完善了电子传输的导电细丝通道,器件实现了由高阻态向低阻态的转变;在反向电压作用下,导电通道断裂,器件恢复到高阻态。  相似文献   

5.
采用微波辅助法制备了生物果胶薄膜,并作为缓冲层,制作了Ag/pectin/a-C/Pt阻变存储器.利用原子力显微镜表征薄膜表面的电流分布,探究了果胶薄膜的离子缓冲机理.分析了基于果胶薄膜的阻变存储器的阻变性能和阻变机制.结果表明:该缓冲层能够降低器件开关电压的波动性,提升高低阻态开关比.通过调控限制电流,在单一器件上实现了多阻态信息存储.  相似文献   

6.
庞华  邓宁 《物理学报》2014,63(14):147301-147301
研究了Ni/HfO2(10 nm)/Pt存储单元的阻变特性和机理.该器件具有forming-free的性质,还表现出与以往HfO2(3 nm)基器件不同的复杂的非极性阻变特性,并且具有较大的存储窗口值(105).存储单元的低阻态阻值不随单元面积改变,符合导电细丝阻变机理的特征.采用X射线光电子能谱仪分析器件处于低阻态时的阻变层HfO2薄膜的化学组分以及元素的化学态,结果表明,Ni/HfO2/Pt阻变存储器件处于低阻态时的导电细丝是由金属Ni导电细丝和氧空位导电细丝共同形成的.  相似文献   

7.
基于高阻ZnO薄膜的光电导型紫外探测器   总被引:1,自引:0,他引:1       下载免费PDF全文
祁晓萌  彭文博  赵小龙  贺永宁 《物理学报》2015,64(19):198501-198501
本文通过射频磁控溅射法在玻璃衬底上沉积一层ZnO薄膜, 制备了Al-ZnO-Al 结构光电导型紫外探测器件, 并在室温下测试了所制备器件的暗场特性及其对紫外线的响应特性. 暗场条件下器件电流特性测试结果表明所制备的ZnO薄膜电阻率达到了3.71×109 Ω · cm, 是一种高阻薄膜. 在波长365 nm, 光强303 μW/cm2的紫外线照射下, 薄膜的电阻率为7.20×106 Ω · cm, 探测器明暗电流比达到了516. 40 V偏置电压条件下周期性开关紫外线照时, 探测器的上升和下降时间分别为199 ms和217 ms, 响应速度快且重复性好, 并利用ZnO半导体表面复合慢过程和体复合快过程对瞬态响应过程进行了理论拟合分析. 本文研究结果表明, 高阻ZnO薄膜紫外探测器具有良好的紫外光电响应特性.  相似文献   

8.
利用自主开发的导电原子力显微镜控制Pt,W探针构成点接触金属/Pr0.7Ca0.3MnO3(PCMO)/Pt三明治结构,对其电流-电压(I-V)及脉冲诱导电阻开关(EPIR)特性进行了研究.研究发现,在10 nA限流下两种电极对应结构的I-V都表现出相当稳定的双极性电阻开关特性,以及大于100的电阻开关比.进一步测试发现,点接触W/PCMO/Pt器件具有在10 nA限流下稳定的EPIR特性以及100 pA限流下重复的双极性电阻开关特性.此电流比已报道的电流低3个数量级,表明此结构在低功耗存储器件方面的潜在应用.通过对比样品不同位置、不同限流、不同接触面积点接触Pt/PCMO/Pt的I-V回滞特性,把点接触器件在低电流下稳定、显著的电阻开关效应归结于小的器件面积导致强的局域电场加强了O离子迁移效应.  相似文献   

9.
利用自主开发的导电原子力显微镜控制Pt,W探针构成点接触金属/Pr0.7Ca0.3MnO3(PCMO)/Pt三明治结构,对其电流-电压(I-V)及脉冲诱导电阻开关(EPIR)特性进行了研究.研究发现,在10 nA限流下两种电极对应结构的I-V都表现出相当稳定的双极性电阻开关特性,以及大于100的电阻开关比.进一步测试发现,点接触W/PCMO/Pt器件具有在10 nA限流下稳定的EPIR特性以及100 pA限流下重复的双极性电阻开关特性.此电流比已报道的电流低3个数量级,表明此结构在低功耗存储器件方面的潜在应用.通过对比样品不同位置、不同限流、不同接触面积点接触Pt/PCMO/Pt的I-V回滞特性,把点接触器件在低电流下稳定、显著的电阻开关效应归结于小的器件面积导致强的局域电场加强了O离子迁移效应. 关键词: 脉冲诱导电阻开关 电场下氧离子迁移 电阻开关  相似文献   

10.
李建昌  邵思佳 《物理学报》2017,66(1):17101-017101
有机分子包埋纳米粒子阻变薄膜是信息存储领域的研究热点之一,本文从器件电极、介质层结构、纳米粒子种类、阻变机理和柔性弯折等方面,综述了其近年来的研究进展.电极/分子及分子/纳米粒子界面性质对器件阻变特性影响较大,但影响规律及界面调控机理仍待探究;分子结构与纳米粒子的种类、尺度及分布可改变膜内界面性质进而影响阻变特性;器件阻变机理主要包括导电细丝、电荷俘获与释放和电荷转移三种,其中导电细丝又分金属、氧空位和碳细丝.分子包埋纳米粒子薄膜阻变研究现多停留在小规模和静态器件方面,下一步应从连续卷绕制备、纳米粒子分布精确控制和耐弯扭特性等方面深入研究,为实现大面积、低成本、高柔性阻变存储器奠定基础.  相似文献   

11.
Cu/ZnO/n+-Si structures were prepared by magnetron sputtering of a layer of ZnO thin film onto heavily doped silicon substrate, followed by thermal evaporation of a thin layer of metallic Cu. The resistive switching characteristics of Cu/ZnO/n+-Si structures were investigated as a function of oxygen partial pressure during ZnO deposition. Reproducible resistive switching characteristics were observed in ZnO thin films deposited at 20%, 33% and 50% oxygen partial pressure ratios while ZnO thin film deposited at 10% oxygen partial pressure ratio did not show resistive switching behavior. The conduction mechanisms in high and low resistance states are dominated by space-charge-limited conduction and ohmic behavior respectively, which suggests that resistive switching behaviors in such structures are related to filament formation and rupture. It is also found that the reset current decreases as oxygen partial pressure increases, due to the variation of oxygen vacancy concentration in the ZnO thin films.  相似文献   

12.
Ag/ZnO/Pt structure resistive switching devices are fabricated by radio frequency (RF) magnetron sputtering at room temperature. The memory devices exhibit stable and reversible resistive switching behavior. The ratio of high resistance state to low resistance state can reach as high as 10 2 . The retention measurement indicates that the memory property of these devices can be maintained for a long time (over 10 4 s under 0.1-V durable stress). Moreover, the operation voltages are very low, -0.4 V (OFF state) and 0.8 V (ON state). A high-voltage forming process is not required in the initial state, and multi-step reset process is demonstrated. Resistive switching device with the Ag/ZnO/ITO structure is constructed for comparison with the Ag/ZnO/Pt device.  相似文献   

13.
As an industry accepted storage scheme, hafnium oxide(HfO_x) based resistive random access memory(RRAM)should further improve its thermal stability and data retention for practical applications. We therefore fabricated RRAMs with HfO_x/ZnO double-layer as the storage medium to study their thermal stability as well as data retention. The HfO_x/ZnO double-layer is capable of reversible bipolar switching under ultralow switching current( 3 μA) with a Schottky emission dominant conduction for the high resistance state and a Poole–Frenkel emission governed conduction for the low resistance state. Compared with a drastically increased switching current at 120℃ for the single HfO_x layer RRAM, the HfO_x/ZnO double-layer exhibits excellent thermal stability and maintains neglectful fluctuations in switching current at high temperatures(up to 180℃), which might be attributed to the increased Schottky barrier height to suppress current at high temperatures. Additionally, the HfO_x/ZnO double-layer exhibits 10-year data retention @85℃ that is helpful for the practical applications in RRAMs.  相似文献   

14.
Top electrode (TE) material on the resistive switching behavior of (TE)/CuO/SnO2:F/Si substrate has been studied. We investigated the switching properties of CuO films deposited by sol-gel process. Two kinds of top electrode (TE) material on the resistive switching behaviors have been studied. The nonpolar and bipolar resistive switching phenomenon was observed in CuO thin films with different top electrodes. The filamentary mechanism was used to explain the two kinds of resistive switching behaviors. For the Pt/CuO/ATO device, it showed the nonpolar resistive switching where conducting path is formed and disappear due to the oxygen vacancy. For the Cu/CuO/ATO device, the resistance reduction is due to the existing Cu to form conduction Cu-rich pathways. An opposite bias takes the existing Cu back to the Cu electrode to its high-resistance state. CuO thin films are also observed by XRD, AFM and XPS.  相似文献   

15.
In situ and ex situ oxygen plasma treatment (OPT) were applied to treat ZnO thin films deposited by thermal atomic layer deposition (T-ALD), and the resistive switching (RS) behaviors of the films were investigated. For the in situ OPT, the treatment was applied after each T-ALD cycle. For the ex situ OPT, the treatment was applied on the as-grown film. The T-ALD-grown ZnO films were defect-rich and conductive with no RS behavior. After the OPT process, the resistivity of the films increased drastically, which is believed to be mainly due to the removal of hydrogen impurities, and the films showed bipolar RS characteristics. The dominant conduction mechanisms are the trap-controlled space charge limited current and ohmic behavior at different field regions. The RS behavior was induced upon the formation/disruption of the conducting filaments. Owing to the homogeneous chemical composition and fewer defects, the resistance ratio of the in situ OPT ZnO film is higher than that of the ex situ OPT film, implying that the in situ OPT method is an efficient way to fabricate resistive random access memory devices using the ALD-grown ZnO films.  相似文献   

16.
张志超  王芳  吴仕剑  李毅  弭伟  赵金石  张楷亮 《物理学报》2018,67(5):57301-057301
采用射频磁控溅射的方法,基于不同氧分压制备的氧化铪构建了Ni/HfO_x/TiN结构阻变存储单元.研究发现,随着氧分压的增加,薄膜表面粗糙度略有降低;另一方面,阻变单元功耗降低,循环耐受性能可达10~3次,且转变电压分布的一致性得到改善.结合电流-电压曲线线性拟合结果及外加温度测试探究了器件的转变机理,得出在低阻态的传导机理为欧姆传导机理,在高阻态的传导机理为肖特基发射机理,并根据氧空位导电细丝理论,对高低阻态的阻变机理进行了详细的理论分析.  相似文献   

17.
In this study, unipolar resistive switching (URS) characteristics in ZnO thin film memory devices were systematically investigated with variable defect content. ZnO films displayed typically URS behavior while oxygen-deficient ZnO1?x films did not show resistive switching effects. The devices with two intentional Ohmic interfaces still show URS. These results show that appearance of URS behavior can be dominated by initial oxygen vacancy content in ZnO thin films. Modest increase in oxygen vacancy content in ZnO films will lead to forming-free and narrower distributions of switching parameters (set and reset voltage, high and low resistance states). It indicates that controlling the initial oxygen vacancy content was an effective method to enhance the URS performance.  相似文献   

18.
采用电泳沉积法在FTO导电玻璃基片上制备Zn1-xCuxO薄膜,并对其微观结构、光致发光谱、伏安特性、保持特性和转换电压分布进行探讨。PL谱表明,Cu掺杂在禁带中引入深受主能级,降低氧空位浓度,导致ZnO薄膜的紫外发光、蓝光发光和绿光发光峰强度降低。所得薄膜的晶粒细小、致密、均匀,具有稳定的双极性阻变特性,开关比Roff/Ron最高达到105,其低阻态(LRS)和高阻态(HRS)的阻变机理分别符合欧姆定律和空间电荷限制传导理论。器件经100次循环测试后开关比无明显变化,呈现出较为良好的抗疲劳特性。Cu掺杂对LRS影响不大,但显著改善了HRS的分散性以及转换电压VSET的分散性。当Cu掺杂量x=0.04时,器件表现出良好的综合性能:Roff≈106 Ω,Roff/Ron≈104,VSET介于0.4~3.03 V之间。  相似文献   

19.
Polycrystalline LaCrO_3(LCO) thin films are deposited on Pt/Ti/SiO_2/Si substrates by pulsed laser deposition and used as the switching material to construct resistive random access memory devices. The unipolar resistive switching(RS) behavior in the Au/LCO/Pt devices exhibits a high resistance ratio of ~104 between the high resistance state(HRS) and low resistance state(LRS) and exhibits excellent endurance/retention characteristics.The conduction mechanism of the HRS in the high voltage range is dominated by the Schottky emission, while the Ohmic conduction dictates the LRS and the low voltage range of HRS. The RS behavior in the Au/LCO/Pt devices can be understood by the formation and rupture of conducting filaments consisting of oxygen vacancies,which is validated by the temperature dependence of resistance and x-ray photoelectron spectroscopy results.Further analysis shows that the reset current I_R and reset power P_R in the reset processes exhibit a scaling law with the resistance in LRS(R_0), which indicates that the Joule heating effect plays an essential role in the RS behavior of the Au/LCO/Pt devices.  相似文献   

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