共查询到16条相似文献,搜索用时 62 毫秒
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采用0.18μm标准工艺制备出基于Sn掺杂Ge2Sb2Te5相变材料的相变存储器器件单元,利用自行设计搭建的电学测试系统研究了其存储性能.结果表明:Sn的掺杂没有改变Ge2Sb2Te5的相变特性,其相变阚值电压和阈值电流分别为1.6V和25μA;实现了器件单元的非晶态(高阻)与晶态(低阻)之间的可逆相变过程;器件单元中相变材料结晶所需电流最低为1.78mA(电流宽度固定为100ns)、结晶时间大于80ns(电流高度固定为3mA);相变材料非晶化脉冲电流宽度为30ns时,所需电流大于3.3mA;与Ge2Sb2Te5相比,Sn的掺杂降低了SET操作的脉冲电流宽度,提高了结晶速度,有利于提高相变存储器的存储速度. 相似文献
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溅射功率对Ge2Sb2Te5薄膜光学常数的影响 总被引:1,自引:0,他引:1
研究了溅射功率对Ge2Sb2Te5薄膜的光学常数与波长关系的影响。结果表明,在波长小于500nm的情况下,随溅射功率的增加非晶态薄膜的折射率n先增加然后减小,消光系数k则逐渐减小;在波长大于500nm的情况下,随溅射功率的增加折射率n逐渐减少,消光系数k先减小后增加。对于晶态薄膜样品,在整个波长范围折射率n随溅射功率的增加减小后增加,消光系数k则逐渐减少。薄膜样品的光学常数,在长波长范围随波长变化较大,在短波长范围变化较小。讨论了溅射功率对Ge2Sb2Te5薄膜的光学常数影响的机理。 相似文献
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Ge2Sb2Te5材料与非挥发相转变存储器单元器件特性 总被引:1,自引:0,他引:1
对Ge2Sb2Te5材料的结构、形貌和电学特性进行了表征,将材料应用于不挥发存储单元器件中并研究了器件性能。研究了退火温度对薄膜电阻率的影响,发现在从高阻向低阻状态转变的过程中,电阻率下降的趋势发生变化,形成拐点,分析表明这是由于在拐点处结构由面心立方向密排六方结构转变所致;对不同厚度Ge2Sb2Te5薄膜的电阻率进行了分析,结果表明当厚度薄于70nm时,电阻率随厚度显著上升而迁移率下降,材料晶态电学性能的测量显示,材料有正电阻温度系数并以空穴导电;测量了Ge2Sb2Fe5非挥发相转变存储器单元的I-V曲线,发现有阈值特性,在晶态时电学特性呈欧姆特性,非晶态时I-V低场为线性关系,电场较高时呈指数关系。 相似文献
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采用聚焦脉冲激光研究了Ge2Sb2Te5薄膜在沉积和激光淬火两种非晶态下反射率与激光脉冲宽度变化的关系,发现沉积态的Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而减小,经过激光淬火的非晶态Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而变化平缓。本文借用气-液体系中过饱和度分析液滴形成的原理,从统计物理学角度详细研究了两种非晶态Ge2Sb2Te5薄膜在脉冲激光作用下的晶化过程及机理,结果表明,当Ge2Sb2Te5的非晶态程度处于未饱和或饱和状态时不形成晶核;当Ge2Sb2Te5的非晶态程度处于过饱和状态时,此时的Ge2Sb2Te5为亚稳态,可能形成大小不等的晶核,但只有半径大于临界晶核尺寸时才可能长大成晶粒,而应力降低晶化能垒,增加非晶态Ge2Sb2Te5的过饱和度是导致沉积态与激光淬火态的Ge2Sb2Te5薄膜在晶化触发阶段内反射率随激光脉冲宽度变化规律不一致的根本原因,并据此解释了Ge2Sb2Te5薄膜在这两种状态下的反射率随激光脉冲宽度的变化特点及规律。 相似文献
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采用聚焦脉冲激光研究了Ge2Sb2Te5薄膜在沉积和激光淬火两种非晶态下反射率与激光脉冲宽度变化的关系,发现沉积态的Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而减小,经过激光淬火的非晶态Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而变化平缓.本文借用气-液体系中过饱和度分析液滴形成的原理,从统计物理学角度详细研究了两种非晶态Ge2Sb2Te5薄膜在脉冲激光作用下的晶化过程及机理,结果表明,当Ge2Sb2Te5的非晶态程度处于未饱和或饱和状态时不形成晶核;当Ge2Sb2Te5的非晶态程度处于过饱和状态时,此时的Ge2Sb2Te5为亚稳态,可能形成大小不等的晶核,但只有半径大于临界晶核尺寸时才可能长大成晶粒.而应力降低晶化能垒,增加非晶态Ge2Sb2Te5的过饱和度是导致沉积态与激光淬火态的Ge2Sb2Te5薄膜在晶化触发阶段内反射率随激光脉冲宽度变化规律不一致的根本原因,并据此解释了Ge2Sb2Te5薄膜在这两种状态下的反射率随激光脉冲宽度的变化特点及规律. 相似文献
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Bomy CHEN 《材料科学技术学报》2005,21(1):95-99
The amorphous Ge2Sb2Te5 film with stoichiometric compositions was deposited by co-sputtering of separate Ge, Sb, and Te targets on SiO2/Si (100) wafer in ultrahigh vacuum magnetron sputtering apparatus. The crystallization behavior of amorphous Ge2Sb2Te5 film was investigated by X-ray diffraction (XRD), atomic force microscopy (AFM) and differential scanning calorimetry (DSC). With an increase of annealing temperature, the amorphous Ge2Sb2Te5 film undergoes a two-step crystallization process that it first crystallizes in face-centered-cubic (fcc) crystal structure and finally fcc structure changes to hexagonal (hex) structure. Activation energy values of 3.636±0.137 and 1.579±0.005 eV correspond to the crystallization and structural transformation processes, respectively. From annealing temperature dependence of the film resistivity, it is determined that the first steep decrease of the resistivity corresponds to crystallization while the second one is primarily caused by structural transformation from 相似文献
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J. González-Hernández V. Castaño A. del Real E. Morales-Sánchez E. García-García A. Mendoza-Galván E. F. Prokhorov Yu. V. Vorobiev 《Inorganic Materials》2000,36(12):1219-1227
The kinetics of the amorphous-to-crystalline phase transformation in alloys with compositions around Ge2Sb2Te5, used as erasable optical memories, was investigated by electric impedance, Raman spectroscopy, and optical and transmission electron microscopy. To induce the transformation, isothermal and isokinetic experiments were carried out at various temperatures and various heating rates. The results obtained agree with the Johnson–Mehl–Avrami model and show that the overall activation energy for the transition is about 8 eV, which exceeds previous estimations. The nucleation process changes during the transition and depends on both temperature and heating rate. The available data indicate that nuclei are formed both in the bulk and at the surface of crystallites, and that the structural details of the material (the crystallite size, in particular) depend greatly on the transformation conditions. Intercrystalline inclusions, which appear after the transition, contain Te precipitates within a structurally disordered phase. These inclusions have electrical and optical properties essentially different as compared to the rest of the sample; they could be residual phases formed due to the nonstoichiometric nature of the samples. 相似文献
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Zhimei Sun 《Journal of Materials Science》2012,47(21):7635-7641
Ge2Sb2Te5 (GST) is a technologically important phase-change material for data storage, where the fast reversible phase transition between crystalline and amorphous states is used for recording information. The encoding is achieved by the large contrast in physical properties between the two states. Ge vacancies (VGe) and Sb antisite atoms (SbTe) are primary point defects in crystalline GST. The effect of VGe and SbTe on the atomic arrangements in amorphous GST is unknown, which, however, has significant effects on the performance of GST. In this work, by means of ab initio molecular dynamics calculations, the atomic arrangements in amorphous ideal and defective GST have been investigated. The results show that the amorphous structure of GST with SbTe (St-GST) or with VGe (V-GST) has the same cubic framework and close chemical ordering to ideal GST, and hence similar fast reversible phase transition behavior is expected in the defective phases. Furthermore, the presence of SbTe or VGe in the crystalline phase will result in much more Ge atoms in a tetrahedral geometry as well as in a fourfold octahedral environment in the amorphous state. Especially in V-GST, around 36 % Ge atoms occupy a fourfold octahedral geometry. As fourfold octahedral Ge atoms can enhance the large contrast in physical properties between the crystalline and amorphous phases, introducing Ge vacancies would be an efficient way to improve the performance of GST phase-change materials. 相似文献
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Julian Pries Shuai Wei Matthias Wuttig Pierre Lucas 《Advanced materials (Deerfield Beach, Fla.)》2019,31(39)
Controlling crystallization kinetics is key to overcome the temperature–time dilemma in phase change materials employed for data storage. While the amorphous phase must be preserved for more than 10 years at slightly above room temperature to ensure data integrity, it has to crystallize on a timescale of several nanoseconds following a moderate temperature increase to near 2/3 Tm to compete with other memory devices such as dynamic random access memory (DRAM). Here, a calorimetric demonstration that this striking variation in kinetics involves crystallization occurring either from the glassy or from the undercooled liquid state is provided. Measurements of crystallization kinetics of Ge2Sb2Te5 with heating rates spanning over six orders of magnitude reveal a fourfold decrease in Kissinger activation energy for crystallization upon the glass transition. This enables rapid crystallization above the glass transition temperature Tg. Moreover, highly unusual for glass‐forming systems, crystallization at conventional heating rates is observed more than 50 °C below Tg, where the atomic mobility should be vanishingly small. 相似文献
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By combining electron microscopy and size-dependent electrical measurements, we demonstrate surface-induced heterogeneous nucleation-dominant mechanism for recrystallization of amorphous phase-change Ge2Sb2Te5 nanowires. Heterogeneous nucleation theory quantitatively predicts the nucleation rates that vary by 5 orders of magnitude from 190 to 20 nm lengthscales. Our work demonstrates that increasing the surface-to-volume ratio of nanowires has two effects: lowering of the activation energy barrier due to phonon instability and providing nucleation sites for recrystallization. The systematic study of the effect of surface in phase-change behavior is critical for understanding nanoscale phase-transitions and design of nonvolatile memory devices. 相似文献
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The Sb2Te3-Ag2Te system has been reinvestigated and the phase relations identified by various independent techniques. An intermediate phase with Ag19Sb29Te52 composition, through incongruently melting can be obtained as a single crystal from melts enriched in Ag2Te. It behaves as a solid solution of narrow homogeneity range (from 42 to 44% Ag2Te). 相似文献