CN112699628B - OTS + PCM unit simulation system of three-dimensional phase change memory - Google Patents
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Abstract
Description
技术领域technical field
本发明属于微电子学技术领域,更具体地,涉及一种三维相变存储器的OTS+PCM单元模拟系统。The invention belongs to the technical field of microelectronics, and more particularly, relates to an OTS+PCM unit simulation system of a three-dimensional phase change memory.
背景技术Background technique
相变存储器是利用相变材料在晶态和非晶态之间可以快速重复转换且不同态具有巨大性质差异的特性而研究出的一种非易失性存储器,三维相变存储器具有可与CMOS工艺集成、高密度、低成本与非易失等优势,被认为是最有希望成为下一代非挥发性存储器的器件。但是为了解决相变存储器做成crossbar结构存储阵列所具有漏电流的问题,研究者们利用具有与相变存储器相似工艺的OTS选通管配置成1S1R结构的器件,相比于其它选通器件,它具有结构简单、3维可堆叠性、快速的开/关时间和高的耐用性等优点。对于三维相变存储器成功商业化应用而言,良好的芯片电路设计十分重要。电路仿真软件的输入文件一般包括电路结构描述文件和元件模型文件,这两者构成整体电路模型系统。因此,能准确构建电学特性的三维相变存储器的OTS+PCM单元模拟系统对于相变存储器芯片电路设计至关重要。Phase change memory is a kind of non-volatile memory developed by utilizing the characteristics of phase change materials that can be rapidly and repeatedly converted between crystalline and amorphous states, and different states have huge differences in properties. The advantages of process integration, high density, low cost and non-volatile are considered to be the most promising devices for the next generation of non-volatile memory. However, in order to solve the leakage current problem of the crossbar structure storage array of the phase change memory, the researchers used the OTS gate tube with a similar process to the phase change memory to configure the device of the 1S1R structure. Compared with other gate devices, the It has the advantages of simple structure, 3-dimensional stackability, fast on/off time and high durability. For the successful commercial application of 3D phase change memory, good chip circuit design is very important. The input files of circuit simulation software generally include circuit structure description files and component model files, which constitute the overall circuit model system. Therefore, an OTS+PCM cell simulation system that can accurately construct a three-dimensional phase-change memory with electrical characteristics is very important for the circuit design of a phase-change memory chip.
现有的对于三维相变存储器OTS+PCM单元的SPICE模拟系统,单独的OTS单元或者PCM单元的SPICE模型系统的研究有很多,但对于将OTS+PCM单元集成起来的模型系统很少,现有的PCM单元的SPICE模型系统通常以由电学模块、温度模块和晶化模块三大部分构成,而OTS+PCM单元的模型系统中OTS通常采用与PCM单元模型系统中的电学模块一致的模型,由于OTS单元与PCM单元在电流激励下均呈现S型曲线,现有的模型无法在保证精确度的情况下直接同时使用电流和电压激励,而实际的OTS+PCM单元的操作通常采用电流激励进行擦写,电压激励进行读取。因此无法应用于实际的芯片设计。There are many researches on SPICE simulation system of 3D phase change memory OTS+PCM unit, SPICE model system of separate OTS unit or PCM unit, but there are few model systems integrating OTS+PCM unit. The SPICE model system of the PCM unit is usually composed of three parts: the electrical module, the temperature module and the crystallization module, and the OTS in the model system of the OTS+PCM unit usually adopts the same model as the electrical module in the PCM unit model system. Both the OTS unit and the PCM unit show an S-shaped curve under current excitation. The existing model cannot directly use current and voltage excitation at the same time without guaranteeing accuracy. However, the actual operation of the OTS+PCM unit usually uses current excitation for erasing Write, voltage excitation to read. Therefore, it cannot be applied to actual chip design.
发明内容SUMMARY OF THE INVENTION
针对现有技术的以上缺陷或改进需求,本发明提供了一种三维相变存储器的OTS+PCM单元模拟系统,其目的在于解决现有技术无法准确模拟OTS+PCM单元的问题。In view of the above defects or improvement requirements of the prior art, the present invention provides an OTS+PCM cell simulation system of a three-dimensional phase change memory, which aims to solve the problem that the prior art cannot accurately simulate the OTS+PCM cell.
为实现上述目的,本发明提供了一种三维相变存储器的OTS+PCM单元模拟系统,包括:OTS单元I-V模块、PCM单元I-V模块、PCM温度模块和PCM相变模块;其中,OTS单元I-V模块和PCM单元I-V模块串联构成OTS+PCM单元I-V模块;OTS+PCM单元包括串联的OTS单元和PCM单元;In order to achieve the above object, the present invention provides an OTS+PCM unit simulation system of a three-dimensional phase change memory, including: an OTS unit I-V module, a PCM unit I-V module, a PCM temperature module and a PCM phase change module; wherein, the OTS unit I-V module It is connected in series with the PCM unit I-V module to form an OTS+PCM unit I-V module; the OTS+PCM unit includes the OTS unit and the PCM unit connected in series;
PCM单元I-V模块用于基于P-F模型和欧姆定律构建OTS+PCM单元I-V特性模型,当OTS+PCM单元I-V模块接收到外界施加的激励后,将外界施加的激励和PCM单元的非晶化率带入OTS+PCM单元I-V特性模型中,计算得到PCM单元上的电流和电压,并输出到PCM温度模块中;其中,外界施加的激励为电流或电压;当外界施加的激励为电压时,OTS单元I-V模块用于对PCM单元I-V模块进行限流;The PCM unit I-V module is used to construct the OTS+PCM unit I-V characteristic model based on the P-F model and Ohm's law. Enter the OTS+PCM unit I-V characteristic model, calculate the current and voltage on the PCM unit, and output them to the PCM temperature module; among them, the external excitation is current or voltage; when the external excitation is voltage, the OTS unit The I-V module is used to limit the current of the PCM unit I-V module;
PCM温度模块用于根据PCM单元上的电流和电压,采用热阻热容RC网络实时计算PCM单元的温度,并输出到PCM相变模块中;The PCM temperature module is used to calculate the temperature of the PCM unit in real time according to the current and voltage on the PCM unit, using the thermal resistance and heat capacity RC network, and output it to the PCM phase change module;
PCM相变模块用于根据PCM单元的温度判断PCM单元处于晶化状态还是非晶化状态,计算PCM单元的晶化速率和非晶化速率,将二者之和作为实时相变速率,并根据所得实时相变速率计算PCM单元的非晶化率,并输出到PCM单元I-V模块中。The PCM phase change module is used to judge whether the PCM unit is in a crystalline state or an amorphized state according to the temperature of the PCM unit, calculate the crystallization rate and amorphization rate of the PCM unit, and use the sum of the two as the real-time phase change rate. The obtained real-time phase transition rate calculates the amorphization rate of the PCM cell and outputs it to the PCM cell I-V module.
进一步优选地,上述OTS+PCM单元I-V特性模型为:Further preferably, the above-mentioned OTS+PCM unit I-V characteristic model is:
IOTS=I1+(-I1+Ion1Fth)Fh I OTS =I 1 +(-I 1 +I on1 F th )F h
I1=2qA(dz/t0)Nt exp(-Et/kT0)sinh(VOTSdz/(2kT0ua))I 1 =2qA(dz/t 0 )N t exp(-E t /kT 0 )sinh(V OTS dz/(2kT 0 u a ))
Ion1=(VOTS-Vh1)/Ron1 I on1 =(V OTS -V h1 )/R on1
IPCM=I2+(-I2+Ion2)Fth I PCM =I 2 +(-I 2 +I on2 )F th
I2=(exp(K(Ca)VPCM)-1)/(K(Ca)R(Ca))I 2 =(exp(K(C a )V PCM )-1)/(K(C a )R(C a ))
Ion2=(VPCM-Vh2)/Ron2 I on2 =(V PCM -V h2 )/R on2
R(Ca)=RaCa+Ron2(1-Ca)R(C a )=R a C a +R on2 (1-C a )
其中,IOTS为OTS单元上的电流,I1为OTS单元的高阻态电流,Ion1为OTS单元的低阻态电流,q为电荷量,A为OTS单元的横截面面积,dz为陷阱间的平均距离,t0是束缚电子的特征逃逸时间,Nt为总陷阱电子浓度,Et为深陷阱与浅陷阱间的距离,k为玻尔兹曼常数,T0为环境温度,ua为OTS单元的厚度,VOTS为OTS单元上的电压,Vh1为OTS单元的保持电压,Ron1为OTS单元的开态电阻,IPCM为PCM单元上的电流,I2为PCM单元的高阻态电流,Ion2为PCM单元的低阻态电流,K(Ca)为当PCM单元的非晶化率为Ca时所对应的拟合系数,Ca为非晶化率,VPCM为PCM单元上的电压,R(Ca)为当PCM单元的非晶化率为Ca时PCM单元的电阻值,Vh2为PCM单元的保持电压,Ron2为PCM单元的开态电阻,I为OTS+PCM单元I-V模块接收到的外界施加的电流,V为OTS+PCM单元I-V模块接收到的外界施加的电压;Ith为预设电流阈值,Vth为预设电压阈值,α为比例系数;Among them, I OTS is the current on the OTS unit, I 1 is the high resistance state current of the OTS unit, I on1 is the low resistance state current of the OTS unit, q is the amount of charge, A is the cross-sectional area of the OTS unit, and dz is the trap The average distance between the two, t 0 is the characteristic escape time of bound electrons, N t is the total trap electron concentration, E t is the distance between the deep trap and the shallow trap, k is the Boltzmann constant, T 0 is the ambient temperature, u a is the thickness of the OTS cell, V OTS is the voltage on the OTS cell, V h1 is the holding voltage of the OTS cell, R on1 is the on-state resistance of the OTS cell, I PCM is the current on the PCM cell, and I 2 is the PCM cell’s High resistance state current, I on2 is the low resistance state current of the PCM cell, K(C a ) is the corresponding fitting coefficient when the amorphization rate of the PCM cell is Ca , Ca is the amorphization rate, V PCM is the voltage on the PCM cell, R(C a ) is the resistance value of the PCM cell when the amorphization rate of the PCM cell is Ca , V h2 is the holding voltage of the PCM cell, and R on2 is the on-state resistance of the PCM cell , I is the externally applied current received by the OTS+PCM unit IV module, V is the externally applied voltage received by the OTS+PCM unit IV module; I th is the preset current threshold, V th is the preset voltage threshold, α is the proportional coefficient;
若外界施加的激励为电压V时,V=VOTS+VPCM;If the external excitation is the voltage V, V=V OTS +V PCM ;
若外界施加的激励为电流I时,I=IOTS=IPCM。If the external excitation is the current I, I=I OTS =I PCM .
进一步优选地,PCM单元的温度表达式为:Further preferably, the temperature expression of the PCM unit is:
其中,IPCM为PCM单元上的电流,VPCM为PCM单元两端的电压,T为PCM单元的温度,T0为环境温度,rtb为下电极热阻,rtgst为PCM单元热阻,rtt为上电极热阻,Ct为PCM单元热容,t为时间。Among them, I PCM is the current on the PCM cell, V PCM is the voltage across the PCM cell, T is the temperature of the PCM cell, T 0 is the ambient temperature, r tb is the lower electrode thermal resistance, r tgst is the PCM cell thermal resistance, r tt is the thermal resistance of the upper electrode, C t is the heat capacity of the PCM cell, and t is the time.
进一步优选地,将PCM单元的温度与PCM单元相变材料熔点以及结晶温度进行比较;若PCM单元的温度高于相变材料熔点时,PCM单元处于非晶化状态,此时,PCM单元的晶化速率为0;若PCM单元的温度低于相变材料熔点且高于结晶温度时,PCM单元处于晶化状态,此时,PCM单元的非晶化速率为0。Further preferably, the temperature of the PCM unit is compared with the melting point and crystallization temperature of the phase change material of the PCM unit; if the temperature of the PCM unit is higher than the melting point of the phase change material, the PCM unit is in an amorphous state, and at this time, the crystal of the PCM unit is in an amorphous state. If the temperature of the PCM unit is lower than the melting point of the phase change material and higher than the crystallization temperature, the PCM unit is in a crystalline state, and at this time, the amorphization rate of the PCM unit is 0.
进一步优选地,上述实时相变速率为:Further preferably, the above-mentioned real-time phase change rate is:
Va=VacFcFac+VaaFaa,V a =V ac F c F ac +V aa F aa ,
其中,Vac为晶化速率,Vaa为非晶化速率, Tc为晶化温度,Ta为熔点温度,α为比例系数。where V ac is the crystallization rate, V aa is the amorphization rate, T c is the crystallization temperature, Ta is the melting point temperature, and α is the proportionality coefficient.
进一步优选地,根据PCM单元温度,基于成核-生长理论,计算成核速率和生长速率之和,得到上述晶化速率。Further preferably, the above-mentioned crystallization rate is obtained by calculating the sum of the nucleation rate and the growth rate based on the nucleation-growth theory according to the temperature of the PCM unit.
进一步优选地,上述非晶化速率Vaa=a(T-Tm)/h1rta;其中,T为PCM单元的温度,Tm为PCM单元的相变层熔点,h 1为PCM单元的熔化潜热,rta为PCM单元非晶化区域的热阻,a为比例系数。Further preferably, the above-mentioned amorphization rate V aa =a(TT m )/h 1 r ta ; wherein, T is the temperature of the PCM unit, T m is the melting point of the phase change layer of the PCM unit, and h 1 is the melting point of the PCM unit Latent heat, r ta is the thermal resistance of the amorphized region of the PCM cell, and a is the scaling factor.
总体而言,通过本发明所构思的以上技术方案与现有技术相比,能够取得下列有益效果:In general, compared with the prior art, the above technical solutions conceived by the present invention can achieve the following beneficial effects:
1、本发明提供了一种三维相变存储器的OTS+PCM单元模拟系统,其中,PCM单元I-V模块基于P-F模型和欧姆定律构建OTS+PCM单元I-V特性模型,当OTS+PCM单元I-V模块接收到外界施加的激励后,将外界施加的激励和PCM单元的非晶化率带入OTS+PCM单元I-V特性模型中,计算得到PCM单元上的电流和电压,与现有技术相比,能够同时采用电流电压激励对于模型进行直接操作,并保证了其精确度,能够准确模拟OTS+PCM单元。1. The present invention provides an OTS+PCM unit simulation system of a three-dimensional phase change memory, wherein the PCM unit I-V module constructs an OTS+PCM unit I-V characteristic model based on the P-F model and Ohm's law. When the OTS+PCM unit I-V module receives the After the external excitation, the external excitation and the amorphization rate of the PCM unit are brought into the I-V characteristic model of the OTS+PCM unit, and the current and voltage on the PCM unit are calculated. Compared with the prior art, it can be used simultaneously. The current and voltage excitation operates directly on the model and ensures its accuracy, which can accurately simulate the OTS+PCM unit.
2、本发明所提供的三维相变存储器的OTS+PCM单元模拟系统,通过将OTS单元I-V模块分为两段:高阻态段与低阻态段,高阻态段采用由P-F模型推导出来的载流子传输模型,而且利用阶跃函数的作用将OTS的保持电压保留了下来,由此能够更准确的模拟OTS单元的电学I-V特性;PCM单元I-V模块同样将其分为两段,但与OTS单元高阻态选取的模型不同,PCM单元选取的简易化的P-F模型能够模拟从非晶化比例为0到1的各个部分晶态和完全晶态与完全非晶态的情况,然后在阈值电流与保持电流之间作了忽略,以保证其能在电流激励下完成擦写操作。由于OTS单元I-V模块与PCM单元I-V模块采用分段式模型,在电压激励下能对其准确的进行读擦写操作。在电流激励下,由于OTS单元和PCM单元是串联的,相当于单独对PCM单元进行操作,因此能对其进行电流擦写操作。并在PCM单元的温度模块和相变模块的共同作用下,能准确的模拟PCM单元在单个脉冲或脉冲序列下单元非晶化比例的变化,能给芯片外围电路设计提供可靠的参考以及神经元计算,因此能够大大提高芯片设计的效率和准确性,缩短产品设计周期。2. The OTS+PCM unit simulation system of the three-dimensional phase change memory provided by the present invention divides the I-V module of the OTS unit into two sections: a high-resistance state segment and a low-resistance state segment. The high-resistance state segment is derived from the P-F model. The carrier transport model of the PCM unit is also used to retain the holding voltage of the OTS, so that the electrical I-V characteristics of the OTS unit can be more accurately simulated; the PCM unit I-V module also divides it into two sections, but Different from the model selected for the high resistance state of the OTS cell, the simplified P-F model selected for the PCM cell can simulate various partially crystalline and fully crystalline and fully amorphous states with an amorphization ratio of 0 to 1, and then The threshold current and the holding current are ignored to ensure that it can complete the erasing and writing operations under the current excitation. Because the I-V module of the OTS unit and the I-V module of the PCM unit adopt a segmented model, they can be read, erased and written accurately under voltage excitation. Under current excitation, since the OTS unit and the PCM unit are connected in series, it is equivalent to operating the PCM unit independently, so the current erasing and writing operation can be performed on it. And under the joint action of the temperature module and the phase change module of the PCM unit, it can accurately simulate the change of the amorphization ratio of the PCM unit under a single pulse or pulse sequence, which can provide a reliable reference for the design of the peripheral circuit of the chip and the neuron. Therefore, it can greatly improve the efficiency and accuracy of chip design and shorten the product design cycle.
附图说明Description of drawings
图1是本发明所提供的三维相变存储器的OTS+PCM单元模拟系统的结构示意图;1 is a schematic structural diagram of an OTS+PCM cell simulation system of a three-dimensional phase change memory provided by the present invention;
图2是本发明所提供的对OTS+PCM单元模拟系统进行电压扫描所得的直流I-V曲线示意图;2 is a schematic diagram of a DC I-V curve obtained by performing a voltage scan to the OTS+PCM unit simulation system provided by the present invention;
图3是本发明所提供的对OTS+PCM单元模拟系统施加脉冲序列所得的得到了PCM单元的RI曲线示意图。3 is a schematic diagram of the RI curve of the PCM unit obtained by applying a pulse sequence to the OTS+PCM unit simulation system provided by the present invention.
具体实施方式Detailed ways
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。此外,下面所描述的本发明各个实施方式中所涉及到的技术特征只要彼此之间未构成冲突就可以相互组合。In order to make the objectives, technical solutions and advantages of the present invention clearer, the present invention will be further described in detail below with reference to the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention, but not to limit the present invention. In addition, the technical features involved in the various embodiments of the present invention described below can be combined with each other as long as they do not conflict with each other.
为实现上述目的,本发明提供了一种三维相变存储器的OTS+PCM单元模拟系统,如图1所示,包括:OTS单元I-V模块1、PCM单元I-V模块2、PCM温度模块3和PCM相变模块4;其中,OTS单元I-V模块1和PCM单元I-V模块2串联构成OTS+PCM单元I-V模块;OTS+PCM单元包括串联的OTS单元和PCM单元;In order to achieve the above object, the present invention provides an OTS+PCM unit simulation system of a three-dimensional phase change memory, as shown in FIG.
PCM单元I-V模块1用于基于P-F模型和欧姆定律构建OTS+PCM单元I-V特性模型,当OTS+PCM单元I-V模块接收到外界施加的激励后,将外界施加的激励和PCM单元的非晶化率带入OTS+PCM单元I-V特性模型中,计算得到PCM单元上的电流和电压,并输出到PCM温度模块3中;其中,外界施加的激励为电流或电压;当外界施加的激励为电压时,OTS单元I-V模块2用于对PCM单元I-V模块1进行限流;The PCM
具体的,上述基于P-F模型和欧姆定律构建OTS+PCM单元I-V特性模型的过程如下:Specifically, the above process of constructing the I-V characteristic model of the OTS+PCM unit based on the P-F model and Ohm's law is as follows:
OTS+PCM单元包括串联的OTS单元和PCM单元;分别对OTS单元和PCM单元的直流I-V特性进行分析。对于OTS单元,当其处于在低阻态时,由于其迁移率不会发生改变,类似于金属行为,故其I-V特性符合欧姆定律。当其处于在高阻态时,电流随着电压呈现指数型变化,这种变化通常描述为P-F模型。但是在OTS单元的直流I-V特性中除了上述的高阻态和低阻态两段稳态阶段外,还有一段在阈值电压之后电压随着电流的增大反而减小的转换特性,称为S形负微分特性,但这段I-V特性是不稳定的,而且只在激励为电流时直流I-V测试时才会被捕捉到。实际上,实际的OTS+PCM单元的擦写操作不管是用电压还是电流都不会利用到这段特性,而读操作一般采用电压控制。在阵列中为了限制漏电流,未被选择的OTS单元选通管将被偏置在关断状态(高阻态),被选择的OTS单元选通管被偏置在导通状态(低阻态),以达到在目标存储单元上有足够的存取电压降。因此,实际在三维相变存储器中的OTS选通管的稳态特性比转换更重要,它决定了阵列的性能。所以这里将S形负微分特性这段转换特性忽略掉,然后利用阶跃函数将两段稳态特性的I-V联合起来。The OTS+PCM unit includes the OTS unit and the PCM unit connected in series; the DC I-V characteristics of the OTS unit and the PCM unit are analyzed respectively. For an OTS cell, when it is in a low-resistance state, its I-V characteristics conform to Ohm's law because its mobility does not change, similar to metal behavior. When it is in a high resistance state, the current changes exponentially with the voltage, and this change is often described as the P-F model. However, in the DC I-V characteristics of the OTS unit, in addition to the two steady-state stages of the high-resistance state and the low-resistance state, there is also a transition characteristic in which the voltage decreases with the increase of the current after the threshold voltage, which is called S shape negative differential characteristic, but this I-V characteristic is unstable, and will only be captured in the DC I-V test when the excitation is current. In fact, the actual erasing and writing operations of the OTS+PCM cells will not take advantage of this feature regardless of whether they use voltage or current, and the read operation generally adopts voltage control. To limit leakage current in the array, the unselected OTS cell strobes will be biased in the off state (high impedance state), and the selected OTS cell strobes will be biased in the on state (low impedance state) ) to achieve sufficient access voltage drop across the target memory cell. Therefore, the steady-state characteristics of the OTS strobes actually in the 3D phase change memory are more important than the switching, which determines the performance of the array. Therefore, the conversion characteristic of the S-shaped negative differential characteristic is ignored here, and the step function is used to combine the I-V of the two steady-state characteristics.
对于PCM单元,由于PCM单元与OTS单元都是采用的硫系化合物材料,在结构与材料上都具有相似性,所以PCM单元的直流I-V特性与OTS单元直流I-V特性类似,PCM单元的低阻态直流I-V特性同样采用欧姆定律;PCM单元的高阻态直流I-V这里同样采用P-F模型计算PCM单元的高阻态I-V,但由于PCM单元会发生晶态转变,需要考虑PCM单元的非晶化率,所以将P-F模型简易化,来表示PCM单元的高阻态直流I-V特性。For the PCM unit, since both the PCM unit and the OTS unit are made of chalcogenide materials, they are similar in structure and material, so the DC I-V characteristics of the PCM unit are similar to the DC I-V characteristics of the OTS unit. The low resistance state of the PCM unit The DC I-V characteristics also use Ohm's law; the high-resistance DC I-V of the PCM unit is also calculated by the P-F model. Therefore, the P-F model is simplified to represent the high-impedance DC I-V characteristics of the PCM cell.
在分析了PCM单元与OTS单元的直流I-V特性后,利用阶跃函数将PCM单元与OTS单元不同阶段的直流I-V联合起来,得到OTS+PCM单元I-V特性模型:After analyzing the DC I-V characteristics of the PCM unit and the OTS unit, the step function is used to combine the DC I-V of the PCM unit and the OTS unit at different stages, and the I-V characteristic model of the OTS+PCM unit is obtained:
IOTS=I1+(-I1+Ion1Fth)Fh I OTS =I 1 +(-I 1 +I on1 F th )F h
I1=2qA(dz/t0)Nt exp(-Et/kT0)sinh(VOTSdz/(2kT0ua))I 1 =2qA(dz/t 0 )N t exp(-E t /kT 0 )sinh(V OTS dz/(2kT 0 u a ))
Ion1=(VOTS-Vh1)/Ron1 I on1 =(V OTS -V h1 )/R on1
IPCM=I2+(-I2+Ion2)Fth I PCM =I 2 +(-I 2 +I on2 )F th
I2=(exp(K(Ca)VPCM)-1)/(K(Ca)R(Ca))I 2 =(exp(K(C a )V PCM )-1)/(K(C a )R(C a ))
Ion2=(VPCM-Vh2)/Ron2 I on2 =(V PCM -V h2 )/R on2
R(Ca)=RaCa+Ron2(1-Ca)R(C a )=R a C a +R on2 (1-C a )
其中,IOTS为OTS单元上的电流,I1为OTS单元的高阻态电流,Ion1为OTS单元的低阻态电流,q为电荷量,A为OTS单元的横截面面积,dz为陷阱间的平均距离,t0是束缚电子的特征逃逸时间,Nt为总陷阱电子浓度,Et为深陷阱与浅陷阱间的距离,k为玻尔兹曼常数,T0为环境温度,ua为OTS单元的厚度,VOTS为OTS单元上的电压,Vh1为OTS单元的保持电压,Ron1为OTS单元的开态电阻,IPCM为PCM单元上的电流,I2为PCM单元的高阻态电流,Ion2为PCM单元的低阻态电流,K(Ca)为当PCM单元的非晶化率为Ca时所对应的拟合系数,Ca为非晶化率,VPCM为PCM单元上的电压,R(Ca)为当PCM单元的非晶化率为Ca时PCM单元的电阻值,Vh2为PCM单元的保持电压,Ron2为PCM单元的开态电阻,I为OTS+PCM单元I-V模块接收到的外界施加的电流,V为OTS+PCM单元I-V模块接收到的外界施加的电压;Ith为预设电流阈值,Vth为预设电压阈值,α为比例系数;Among them, I OTS is the current on the OTS unit, I 1 is the high resistance state current of the OTS unit, I on1 is the low resistance state current of the OTS unit, q is the amount of charge, A is the cross-sectional area of the OTS unit, and dz is the trap The average distance between the two, t 0 is the characteristic escape time of bound electrons, N t is the total trap electron concentration, E t is the distance between the deep trap and the shallow trap, k is the Boltzmann constant, T 0 is the ambient temperature, u a is the thickness of the OTS cell, V OTS is the voltage on the OTS cell, V h1 is the holding voltage of the OTS cell, R on1 is the on-state resistance of the OTS cell, I PCM is the current on the PCM cell, and I 2 is the PCM cell’s High resistance state current, I on2 is the low resistance state current of the PCM cell, K(C a ) is the corresponding fitting coefficient when the amorphization rate of the PCM cell is Ca , Ca is the amorphization rate, V PCM is the voltage on the PCM cell, R(C a ) is the resistance value of the PCM cell when the amorphization rate of the PCM cell is Ca , V h2 is the holding voltage of the PCM cell, and R on2 is the on-state resistance of the PCM cell , I is the externally applied current received by the OTS+PCM unit IV module, V is the externally applied voltage received by the OTS+PCM unit IV module; I th is the preset current threshold, V th is the preset voltage threshold, α is the proportional coefficient;
若外界施加的激励为电压V时,V=VOTS+VPCM;If the external excitation is the voltage V, V=V OTS +V PCM ;
若外界施加的激励为电流I时,I=IOTS=IPCM。If the external excitation is the current I, I=I OTS =I PCM .
PCM温度模块3用于根据PCM单元上的电流和电压,采用热阻热容RC网络实时计算PCM单元的温度,并输出到PCM相变模块4中;具体的,PCM温度模块3采用热阻热容RC网络,以环境温度作为初始条件计算脉冲信号期间PCM单元最高点温度,也可模拟连续施加的脉冲序列,环境温度在每个脉冲结束时刻更新为实时温度;The
PCM单元的温度与施加激励下电流电阻产生的焦耳热和单元热阻热容散热以及环境温度相关。计算PCM单元所有点的温度并不现实,而有限元分析表明,在T型结构下操作过程中PCM单元温度最高点主要集中于PCM单元与下电极区域,因此在简化计算中只计算最高点的温度,本发明采用热电类比的方法通过热阻和热容构成的RC电路计算最高点温度。由此,温度计算模块模拟PCM单元温度的计算表达式为:The temperature of the PCM unit is related to the Joule heat generated by the current resistance under excitation, the heat dissipation of the unit thermal resistance, the heat capacity, and the ambient temperature. It is not realistic to calculate the temperature of all points of the PCM cell, and the finite element analysis shows that the highest point of the temperature of the PCM cell is mainly concentrated in the PCM cell and the lower electrode area during the operation under the T-shaped structure, so in the simplified calculation, only the highest point is calculated. Temperature, the present invention adopts the method of thermoelectric analogy to calculate the highest point temperature through an RC circuit composed of thermal resistance and thermal capacitance. Therefore, the calculation expression of the temperature calculation module to simulate the temperature of the PCM unit is:
其中,IPCM为PCM单元上的电流,VPCM为PCM单元两端的电压,T为PCM单元的温度,T0为环境温度,rtb为下电极热阻,rtgst为PCM单元热阻,rtt为上电极热阻,Ct为PCM单元热容,t为时间。Among them, I PCM is the current on the PCM cell, V PCM is the voltage across the PCM cell, T is the temperature of the PCM cell, T 0 is the ambient temperature, r tb is the lower electrode thermal resistance, r tgst is the PCM cell thermal resistance, r tt is the thermal resistance of the upper electrode, C t is the heat capacity of the PCM cell, and t is the time.
具体的,PCM单元热阻的计算公式为:Specifically, the formula for calculating the thermal resistance of the PCM unit is:
PCM单元热容的计算公式为:The formula for calculating the heat capacity of the PCM unit is:
Ct=τ/[1/rtb+1/(rtgst+rtt)]C t =τ/[1/r tb +1/(r tgst +r tt )]
其中,Ca为PCM单元的非晶化率,dgst为PCM单元的厚度,S是下电极与PCM单元的接触面积,ka和kc分别为PCM单元处于非晶态和晶态的热导率,τ为热时间常数。Among them, Ca is the amorphization rate of the PCM unit, d gst is the thickness of the PCM unit, S is the contact area between the lower electrode and the PCM unit, and ka and k c are the heat of the PCM unit in the amorphous and crystalline states, respectively. conductivity, and τ is the thermal time constant.
PCM相变模块4用于PCM相变模块用于根据PCM单元的温度判断PCM单元处于晶化状态还是非晶化状态,计算PCM单元的晶化速率和非晶化速率,将二者之和作为实时相变速率,并根据所得实时相变速率计算PCM单元的非晶化率,并输出到PCM单元I-V模块中。The PCM
具体的,将PCM单元的温度与PCM单元相变材料熔点以及结晶温度进行比较;若PCM单元的温度高于相变材料熔点时,PCM单元处于非晶化状态,此时,PCM单元的晶化速率为0;若PCM单元的温度低于相变材料熔点且高于结晶温度时,PCM单元处于晶化状态,此时,PCM单元的非晶化速率为0;计算PCM单元的晶化速率和非晶化速率,并将二者之和作为实时相变速率,并根据所得实时相变速率计算PCM单元的非晶化率,并输出到PCM单元I-V模块中。Specifically, the temperature of the PCM unit is compared with the melting point and crystallization temperature of the phase change material of the PCM unit; if the temperature of the PCM unit is higher than the melting point of the phase change material, the PCM unit is in an amorphous state, and at this time, the crystallization of the PCM unit The rate is 0; if the temperature of the PCM unit is lower than the melting point of the phase change material and higher than the crystallization temperature, the PCM unit is in a crystalline state, at this time, the amorphization rate of the PCM unit is 0; calculate the crystallization rate of the PCM unit and The amorphization rate is calculated, and the sum of the two is taken as the real-time phase transition rate, and the amorphization rate of the PCM unit is calculated according to the obtained real-time phase transition rate, and is output to the PCM unit I-V module.
进一步地,PCM相变模块包括相变速率计算电路和电容;其中,相变速率计算电路用于计算PCM单元的晶化速率和非晶化速率,并将二者之和作为实时相变速率,输出到电容中;电容用于对实时相变速率进行积分运算,计算非晶化率。Further, the PCM phase change module includes a phase change rate calculation circuit and a capacitor; wherein, the phase change rate calculation circuit is used to calculate the crystallization rate and amorphization rate of the PCM unit, and the sum of the two is used as the real-time phase change rate, Output to the capacitor; the capacitor is used to integrate the real-time phase transition rate and calculate the amorphization rate.
具体的,晶化速率为单位时间内发生晶化的PCM单元体积的变化;根据PCM单元温度,基于成核-生长理论,计算成核速率和生长速率之和,得到晶化速率;Specifically, the crystallization rate is the change in the volume of the PCM unit that is crystallized in unit time; according to the temperature of the PCM unit, based on the nucleation-growth theory, the sum of the nucleation rate and the growth rate is calculated to obtain the crystallization rate;
具体的,晶化速率的计算公式为:Specifically, the formula for calculating the crystallization rate is:
Vac=-(PnVnVa/Vm+SaVg),V ac =-(P n V n V a /V m +S a V g ),
f=exp[-0.8/(1-T/Tm)]f=exp[-0.8/(1-T/T m )]
其中,Pn为单位时间的成核概率,Vn为成核体积,Va为非晶化区域体积,Vm为相变材料的分子体积,Sa为非晶化区域与晶化区域的界面面积,Vg是生长速率;α为原子振动的频率因子,Ea1为成核活化能,γ为单位面积的过剩自由能,ΔG为过量吉布斯自由能,kB为波尔兹曼常数,T为PCM单元温度;Ca为PCM单元的非晶化率,dgst是PCM单元的厚度,f是生长模式因子,a0是原子跃迁距离,Ea2是原子散射活化能;Tm是PCM单元的相变层熔点,h1为PCM单元材料的熔化潜热。Among them, P n is the nucleation probability per unit time, V n is the nucleation volume, Va is the volume of the amorphized region, V m is the molecular volume of the phase change material, and Sa is the difference between the amorphized region and the crystalline region. interfacial area, V g is the growth rate; α is the frequency factor of atomic vibration, E a1 is the nucleation activation energy, γ is the excess free energy per unit area, ΔG is the excess Gibbs free energy, k B is Boltzmann constant, T is the temperature of the PCM cell; C a is the amorphization rate of the PCM cell, d gst is the thickness of the PCM cell, f is the growth mode factor, a 0 is the atomic transition distance, E a2 is the atomic scattering activation energy; T m is the melting point of the phase change layer of the PCM cell, and h 1 is the latent heat of fusion of the PCM cell material.
非晶化速率为单位时间内发生非晶化的PCM单元体积的变化;具体的,非晶化速率的计算公式为:Vaa=a(T-Tm)/h1rta;其中,a为比例系数,T为PCM单元的温度,Tm为PCM单元的相变层熔点,h1为PCM单元的熔化潜热,rta为PCM单元非晶化区域的热阻,具体的,rta=Cadgst/Ska,Ca为PCM单元的非晶化率,dgst为PCM单元的厚度,S为下电极与PCM单元的接触面积,ka为PCM处于非晶态的热导率。The amorphization rate is the change in the volume of the amorphized PCM unit in unit time; specifically, the calculation formula of the amorphization rate is: V aa =a(TT m )/h 1 r ta ; where a is the ratio coefficient, T is the temperature of the PCM unit, T m is the melting point of the phase change layer of the PCM unit, h 1 is the latent heat of fusion of the PCM unit, r ta is the thermal resistance of the amorphized region of the PCM unit, specifically, r ta =C a d gst /Ska , Ca is the amorphization rate of the PCM cell, d gst is the thickness of the PCM cell, S is the contact area between the lower electrode and the PCM cell, and ka is the thermal conductivity of the PCM in the amorphous state.
进一步地,根据PCM温度模块输出的PCM单元温度判断PCM单元发生晶化还是非晶化,这里采用阶跃函数来计算,再由晶化速率与非晶化速率之和作为实时相变速率,具体为:Va=VacFcFac+VaaFaa,其中,Vac为晶化速率,Vaa为非晶化速率,Fc、Fac和Faa分别是与结晶温度与熔点相关的阶跃函数,用来判断发生晶化还是非晶化;具体的, Tc为晶化温度,Ta为熔点温度,α为比例系数;然后把PCM单元体积作为电容,用于积分运算,得到PCM单元的非晶化率。其计算式为:其中电容值dgst为PCM单元的厚度,t为时间。Further, according to the temperature of the PCM unit output by the PCM temperature module, it is determined whether the PCM unit is crystallized or amorphized. Here, a step function is used to calculate, and then the sum of the crystallization rate and the amorphization rate is used as the real-time phase transition rate. Specifically, is: V a =V ac F c F ac +V aa F aa , where V ac is the crystallization rate, V aa is the amorphization rate, and F c , F ac and F aa are related to the crystallization temperature and melting point, respectively The step function of , which is used to determine whether crystallization or amorphization occurs; specifically, T c is the crystallization temperature, Ta is the melting point temperature, and α is the proportional coefficient; then the volume of the PCM unit is used as a capacitance for integral operation to obtain the amorphization rate of the PCM unit. Its calculation formula is: where capacitance value d gst is the thickness of the PCM cell and t is the time.
为了进一步说明本发明所提供的三维相变存储器的OTS+PCM单元模拟系统的准确性,下面结合实验进行详述:In order to further illustrate the accuracy of the OTS+PCM unit simulation system of the three-dimensional phase-change memory provided by the present invention, the following details are described in conjunction with experiments:
在OTS+PCM单元两端施加电压激励进行模拟仿真,同样将初始温度设为室温300K,在HSPICE仿真环境中的分别在PCM单元在晶态和非晶态状态下执行扫描范围为0~5V的电压扫描,OTS+PCM单元在OTS+SET状态下阈值电压VtS为2.7V,OTS+RESET状态下阈值电压为3.7V,保持电压为2.4V,得到如图2所示的直流I-V曲线;其中,正方形的曲线为本发明所提供的模拟系统(记为model)仿真得到的结果,而圆形的曲线为参考文献中实际器件(reference)的测试结果,可以看到,两条曲线基本重合,本发明所提供的模拟系统的阈值电压VtS和VtR与文献实际测试结果相差0.1V以内,证实了此本发明所提供的模拟系统的精确度。Apply voltage excitation at both ends of the OTS+PCM unit for simulation simulation, and also set the initial temperature to room temperature 300K. In the HSPICE simulation environment, the PCM unit is in the crystalline and amorphous states to perform the scanning range of 0~5V. Voltage scanning, the threshold voltage VtS of the OTS+PCM cell in the OTS+SET state is 2.7V, the threshold voltage in the OTS+RESET state is 3.7V, and the holding voltage is 2.4V, and the DC I-V curve shown in Figure 2 is obtained; among them, The square curve is the result obtained by the simulation of the simulation system (referred to as model) provided by the present invention, and the circular curve is the test result of the actual device (reference) in the reference. It can be seen that the two curves basically overlap, and this The threshold voltages VtS and VtR of the simulation system provided by the invention are within 0.1V of the actual test results in the literature, which confirms the accuracy of the simulation system provided by the invention.
进一步地,在HSPICE仿真环境中执行瞬态分析,初始温度设为室温300K,初始非晶化比例为1,施加脉宽为1000ns的脉冲序列。脉冲的初始幅值为120uA,以5uA的递增量,逐步增加脉冲幅值。图3所示为仿真得到的PCM的R-I曲线,由于非晶化比例变化趋势与阻值一致,这里将阻值用非晶化比例替代,电流超过0.13mA后,PCM单元非晶化比例降低;电压超过0.19mA后,随着脉冲幅值逐渐增加,PCM非晶化比例不再降低,说明此时电流脉冲产生的热量使得PCM单元温度接近或大于融化温度。在图中可以观察到,在非晶化比例下降过程中,电阻值逐渐变化,呈现多值分布,符合真实器件的特性。Further, the transient analysis was performed in the HSPICE simulation environment, the initial temperature was set to 300K at room temperature, the initial amorphization ratio was 1, and a pulse sequence with a pulse width of 1000 ns was applied. The initial amplitude of the pulse is 120uA, and the pulse amplitude is gradually increased in increments of 5uA. Figure 3 shows the R-I curve of the PCM obtained by simulation. Since the change trend of the amorphization ratio is consistent with the resistance value, the resistance value is replaced by the amorphization ratio. After the current exceeds 0.13mA, the amorphization ratio of the PCM unit decreases; After the voltage exceeds 0.19mA, as the pulse amplitude gradually increases, the amorphization ratio of PCM no longer decreases, indicating that the heat generated by the current pulse at this time makes the temperature of the PCM cell close to or greater than the melting temperature. It can be observed in the figure that in the process of decreasing the amorphization ratio, the resistance value gradually changes, showing a multi-valued distribution, which is in line with the characteristics of the real device.
本领域的技术人员容易理解,以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明的保护范围之内。Those skilled in the art can easily understand that the above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalent replacements and improvements made within the spirit and principles of the present invention, etc., All should be included within the protection scope of the present invention.
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