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CN105870321A - Nonlinear self-rectifying resistive random access memory and preparation method therefor - Google Patents

Nonlinear self-rectifying resistive random access memory and preparation method therefor Download PDF

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CN105870321A
CN105870321A CN201610183126.6A CN201610183126A CN105870321A CN 105870321 A CN105870321 A CN 105870321A CN 201610183126 A CN201610183126 A CN 201610183126A CN 105870321 A CN105870321 A CN 105870321A
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resistive
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CN105870321B (en
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蔡茂
蔡一茂
王宗巍
黄如
喻志臻
方亦陈
余牧溪
杨雪
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Yanxin Microelectronics Shanghai Co ltd
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Peking University
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    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices having no potential barriers, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/801Constructional details of multistable switching devices
    • HELECTRICITY
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Abstract

The invention provides a nonlinear self-rectifying resistive random access memory. The nonlinear self-rectifying resistive random access memory comprises a substrate and a bottom electrode- resistive random layer-energy band modifying layer-top electrode structure arranged on the substrate. The invention also provides a preparation method for the nonlinear self-rectifying resistive random access memory; the preparation method comprises the following steps of 1) defining a bottom electrode pattern, and preparing the bottom electrode on the substrate according to the pattern; 2) depositing the resistive random layer on the bottom electrode by adopting a PVD method, an ALD method or a CVD method; 3) depositing the energy band modifying layer on the resistive random layer by adopting the PVD method or the ALD method; 4) defining a bottom electrode lead-out hole pattern, and etching the bottom electrode lead-out holes in the resistive random layer and the energy band modifying layer according to the pattern; and 5) defining a top electrode pattern, and preparing the top electrode on the modifying layer according to the pattern.

Description

一种非线性自整流阻变存储器及其制备方法A non-linear self-rectifying resistive variable memory and its preparation method

技术领域technical field

本发明属于半导体和CMOS混合集成电路技术领域,具体涉及一种非线性自整流阻变存储器(resistive random access memory,RRAM)及其制备方法。The invention belongs to the technical field of semiconductor and CMOS hybrid integrated circuits, and in particular relates to a nonlinear self-rectifying resistive random access memory (resistive random access memory, RRAM) and a preparation method thereof.

背景技术Background technique

近年来,随着集成电路的进一步发展,对非易失性存储器的尺寸缩小、功耗降低及高集成度等的要求不断提高,占当前市场主要份额的闪存(flash)由于在尺寸缩小、功耗和速度等方面的限制,已经不能完全满足非易失性存储器发展的要求。In recent years, with the further development of integrated circuits, the requirements for the size reduction, power consumption reduction and high integration of non-volatile memory are continuously increasing. Due to the limitations of power consumption and speed, it can no longer fully meet the requirements of the development of non-volatile memory.

新兴阻变存储器在半导体集成电路领域得到了广泛的关注,阻变存储器在高集成度、低功耗和读写速度等方面的优势使之成为了新一代存储器中的有力竞争者。阻变存储器依靠在不同外加电压激励下实现高阻态(“0”状态)和低阻态(“1”状态)之间可逆的状态转换,在撤除电压激励后可以保持高阻态和低阻态,从而实现数据的非易失性存储。阻变存储器由结构简单的金属-阻变层-金属的三明治结构构成,因此可以通过简单的crossbar结构来实现超大规模和极高密度的阻变存储器阵列,减小了由于增加晶体管作为选择管所带来的面积消耗,其特征尺寸面积可以减小到4F2。此外,集成密度可以进一步通过堆叠多层crossbar结构形成3Dcrossbar结构来提高。Emerging resistive memory has received extensive attention in the field of semiconductor integrated circuits. The advantages of resistive memory in terms of high integration, low power consumption, and read/write speed make it a strong competitor in the new generation of memory. RRAM relies on the reversible state transition between high resistance state ("0" state) and low resistance state ("1" state) under different external voltage excitations, and can maintain high resistance state and low resistance state after the voltage excitation is removed. state, so as to realize the non-volatile storage of data. The RRAM is composed of a simple metal-resistive layer-metal sandwich structure. Therefore, a super-large-scale and extremely high-density RRAM array can be realized through a simple crossbar structure, which reduces the cost of adding transistors as selectors. The resulting area consumption, the characteristic size area can be reduced to 4F 2 . In addition, the integration density can be further improved by stacking multi-layer crossbar structures to form a 3D crossbar structure.

然而,由于阵列中器件阻值的读取需要读取流经该器件的电流大小来判断器件是处于高阻态还是低阻态。最坏情况下,如果要读取crossbar阵列中的一个处于高阻的器件,而其周围的器件均处于低阻态时,当读取处于高阻态的器件时,电流会绕过这个处于高阻态的器件,而在周围的低阻器件上形成sneak电流。此时,读取到的电流实际为流过其周围处于低阻态器件的sneak电流值,造成误读。研究表明,阵列的串扰问题会带来器件的误操作,限制阵列的集成度,增加阵列的功耗等一些列问题,极大地限制了crossbar结构的存储密度。However, since the reading of the resistance value of the device in the array needs to read the magnitude of the current flowing through the device to determine whether the device is in a high-resistance state or a low-resistance state. In the worst case, if you want to read a high-impedance device in the crossbar array, while the surrounding devices are in a low-impedance state, when reading the high-impedance device, the current will bypass this high-impedance device. The device in the resistive state forms a sneak current on the surrounding low-resistance devices. At this time, the read current is actually the sneak current value flowing through the surrounding low-resistance devices, causing misreading. Studies have shown that the crosstalk problem of the array will lead to misoperation of devices, limit the integration of the array, increase the power consumption of the array and other issues, which greatly limit the storage density of the crossbar structure.

目前,为了解决阻变存储器crossbar阵列中的串扰问题,阻变存储器的阵列单元结构主要分为两种:有源阵列,1T1R(One Transistor One RRAM)结构单元;无源阵列,1S1R(OneSelector One RRAM)结构单元。有源阵列的1T1R结构的器件单元中,对器件面积起决定性因素的是晶体管的面积,此外为了满足阻变器件较高的reset电流需求,源漏面积的增大会进一步增大晶体管的面积,这就大大限制了存储阵列的集成密度,丧失了阻变存储器可以高密度集成的优势。1S1R(one selector one RRAM)的结构虽然消除了面积的损耗,但是增加了工艺的步骤,同时也要求的选择管与阻变存储器必须有着良好的匹配,在实际应用中有着一定的局限性。At present, in order to solve the crosstalk problem in the crossbar array of resistive memory, the array unit structure of resistive memory is mainly divided into two types: active array, 1T1R (One Transistor One RRAM) structural unit; passive array, 1S1R (OneSelector One RRAM) )Structural units. In the device unit of the 1T1R structure of the active array, the decisive factor for the device area is the area of the transistor. In addition, in order to meet the high reset current demand of the resistive switching device, the increase of the source and drain area will further increase the area of the transistor. This greatly limits the integration density of the storage array, and loses the advantage of high-density integration of the resistive memory. Although the structure of 1S1R (one selector one RRAM) eliminates the loss of area, it increases the number of process steps, and also requires a good match between the selector transistor and the RRAM, which has certain limitations in practical applications.

发明内容Contents of the invention

鉴于上述不足,本发明提出了一种非线性自整流阻变存储器及其制备方法,基于采用传统CMOS工艺来实现具有非线性自整流的阻变存储器件,以期降低甚至消除阻变存储器的crossbar结构中存在的串扰问题。In view of the above deficiencies, the present invention proposes a non-linear self-rectifying resistive variable memory and its preparation method, based on the use of traditional CMOS technology to realize a non-linear self-rectifying resistive variable memory device, in order to reduce or even eliminate the crossbar structure of the resistive variable memory The crosstalk problem that exists in.

为了解决上述技术问题,本发明采用的技术方案如下:In order to solve the problems of the technologies described above, the technical scheme adopted in the present invention is as follows:

一种非线性自整流阻变存储器,包括衬底和位于衬底上的底电极-阻变层-能带修饰层-顶电极结构。A nonlinear self-rectifying resistive variable memory, comprising a substrate and a bottom electrode-resistive variable layer-energy band modification layer-top electrode structure located on the substrate.

进一步地,所述底电极-阻变层-能带修饰层-顶电极结构为金属-绝缘体-绝缘体-金属(Metal-Insulator-Insulator-Metal)电容结构或金属-半导体-半导体-金属(Metal-Semiconductor-Semiconductor-Metal)电容结构。Further, the bottom electrode-resistive layer-band modification layer-top electrode structure is a metal-insulator-insulator-metal (Metal-Insulator-Insulator-Metal) capacitance structure or a metal-semiconductor-semiconductor-metal (Metal- Semiconductor-Semiconductor-Metal) capacitor structure.

进一步地,所述衬底采用硅或玻璃;Further, the substrate is made of silicon or glass;

所述底电极和顶电极采用金属材料,厚度为50nm-200nm;The bottom electrode and the top electrode are made of metal materials with a thickness of 50nm-200nm;

所述阻变层采用具有阻变特性的过渡金属氧化物,厚度为5nm-50nm;或采用有机材料,厚度为200nm-500nm;The resistive layer is made of a transition metal oxide with resistive properties, with a thickness of 5nm-50nm; or an organic material, with a thickness of 200nm-500nm;

所述能带修饰层采用氧化物,厚度为1-20nm。The energy band modifying layer is made of oxide with a thickness of 1-20nm.

进一步地,所述金属材料为Ti、Al、Au、W、Cu、Ta、Pt、Ir或TiN、TaN;Further, the metal material is Ti, Al, Au, W, Cu, Ta, Pt, Ir or TiN, TaN;

所述过渡金属氧化物为TaOx、HfOx、SiOx或SrTiO3,所述有机材料为parylene;The transition metal oxide is TaO x , HfO x , SiO x or SrTiO 3 , and the organic material is parylene;

所述氧化物为SiO2、TiO2或HfO2The oxide is SiO 2 , TiO 2 or HfO 2 .

一种非线性自整流阻变存储器的制备方法,包括如下步骤:A method for preparing a non-linear self-rectifying resistive variable memory, comprising the steps of:

1)定义底电极图形,按照该图形在衬底上制备底电极;1) Define the bottom electrode pattern, and prepare the bottom electrode on the substrate according to the pattern;

2)采用PVD(物理气相淀积)、ALD(原子层淀积)或CVD(化学气相淀积)的方法在底电极上淀积阻变层;2) Depositing a resistive variable layer on the bottom electrode by means of PVD (Physical Vapor Deposition), ALD (Atomic Layer Deposition) or CVD (Chemical Vapor Deposition);

3)采用PVD或ALD的方法在阻变层上淀积能带修饰层;3) Depositing an energy band modifying layer on the resistive layer by means of PVD or ALD;

4)定义底电极引出孔图形,按照该图形在阻变层和能带修饰层刻蚀出底电极引出孔;4) Define the bottom electrode lead-out hole pattern, and etch the bottom electrode lead-out hole in the resistive layer and the energy band modification layer according to the pattern;

5)定义顶电极图形,按照该图形在修饰层上制备顶电极。5) Define the pattern of the top electrode, and prepare the top electrode on the modification layer according to the pattern.

进一步地,所述步骤1)、4)和5)中定义图形的方法是,利用光刻技术在光刻胶上定义图形。Further, the method for defining the pattern in the steps 1), 4) and 5) is to define the pattern on the photoresist by using photolithography technology.

进一步地,所述底电极和顶电极的制备方法包括PVD和蒸发淀积方法。Further, the preparation method of the bottom electrode and the top electrode includes PVD and evaporation deposition methods.

进一步地,所述阻变层采用具有阻变特性的过渡金属氧化物,厚度为5nm-50nm;或采用有机材料,厚度为200nm-500nm;Further, the resistive layer adopts a transition metal oxide with resistive properties, with a thickness of 5nm-50nm; or an organic material, with a thickness of 200nm-500nm;

进一步地,所述能带修饰层采用氧化物,厚度为1-20nm。Further, the energy band modifying layer is made of oxide with a thickness of 1-20nm.

本发明提出了一种非线性自整流阻变存储器及其制备方法,将能带修饰层嵌入到阻变存储器中形成双层结构,利用能带修饰层材料的厚度变化,及合理设计阻变层、能带修饰层和电极材料间的能带结构匹配,可以实现对阻变存储器件的电流-电压特性进行优化,使该阻变存储器展现出对称双向非线性自整流的特性。该阻变存储器具有对称双向非线性自整流特性,其组成的crossbar阵列无论是读取低阻态还是高阻态,由于非线性整流区域的存在,原本的串扰电流的路径上的阻值要远大于所要读取的阻值,所以可以有效地抑制串扰电流,从而避免误读,对提高存储阵列的集成密度和阻变存储器的大规模量产有着重要的意义。另外,该制备方法与传统CMOS工艺相兼容,成本低,易投入使用。The present invention proposes a non-linear self-rectifying resistive variable memory and a preparation method thereof. The energy band modification layer is embedded into the resistive variable memory to form a double-layer structure, and the thickness change of the energy band modification layer material is used to rationally design the resistive variable layer. 1. The energy band structure matching between the energy band modification layer and the electrode material can realize the optimization of the current-voltage characteristics of the resistive memory device, so that the resistive memory exhibits the characteristic of symmetrical bidirectional nonlinear self-rectification. The resistive variable memory has a symmetrical bidirectional nonlinear self-rectification characteristic. Whether the crossbar array composed of it reads a low-resistance state or a high-resistance state, due to the existence of the nonlinear rectification region, the resistance value of the original crosstalk current path is much larger. Therefore, the crosstalk current can be effectively suppressed, thereby avoiding misreading, which is of great significance for improving the integration density of the memory array and mass production of the RRAM. In addition, the preparation method is compatible with the traditional CMOS process, has low cost and is easy to put into use.

附图说明Description of drawings

图1为本非线性自整流阻变存储器的电流-电压特性曲线图。FIG. 1 is a graph of the current-voltage characteristic curve of the non-linear self-rectifying resistive variable memory.

图中:S1-正向电压的激励下由高阻态向低阻态的跃变过程;S2-低阻态保持过程;S3-正向低阻态非线性整流过程;S4-负向低阻态非线性整流过程;S5-负向电压的激励下由低阻态向高阻态的跃变过程;S6-高阻态保持过程。In the figure: S1-the transition process from high resistance state to low resistance state under the excitation of positive voltage; S2-low resistance state maintenance process; S3-nonlinear rectification process of positive low resistance state; S4-negative low resistance state state nonlinear rectification process; S5-the transition process from low-resistance state to high-resistance state under the excitation of negative voltage; S6-high-resistance state maintenance process.

图2(A)-2(E)对应于各实施例的实施步骤。2(A)-2(E) correspond to the implementation steps of the respective embodiments.

图3为crossbar阵列及串扰电流路径示意图。FIG. 3 is a schematic diagram of a crossbar array and a crosstalk current path.

具体实施方式detailed description

为使本发明的上述特征和优点能更明显易懂,下文特举实施例,并配合所附图作详细说明如下。In order to make the above-mentioned features and advantages of the present invention more comprehensible, the following specific embodiments are described in detail in conjunction with the accompanying drawings.

实施例1Example 1

本实施例1提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器采用硅衬底,采用Pt作为底电极材料,采用Ta2O5(或其非化学配比的氧化物)作为阻变层材料,采用SiO2作为能带修饰层材料,采用Ta作为顶电极材料。This embodiment 1 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The resistive variable memory uses a silicon substrate, uses Pt as the bottom electrode material, and uses Ta 2 O 5 (or its non-stoichiometric oxide ) as the resistive switch layer material, SiO 2 is used as the energy band modification layer material, and Ta is used as the top electrode material.

Ta2O5和SiO2均是与标准CMOS工艺相兼容的材料。基于Ta2O5的阻变存储器有着优异的存储器性能,包括超高的耐久性、超快的开关速度和良好的保持特性。此外,Ta2O5还有着热稳定性高、化学性质不活泼等特点。SiO2作为非常成熟的CMOS工艺中的栅介质材料,材料性质和参数非常明了,制备简单且非常可控。两种材料的优势相结合,加上合理的物理机制层面的设计,既满足兼容CMOS工艺的要求,又能实现阻变存储器双向非线性自整流的特性,对于阻变存储器crossbar结构阵列集成密度的提升和大规模生产有着重要的意义。Both Ta 2 O 5 and SiO 2 are materials compatible with standard CMOS processes. Ta 2 O 5 based RRAM has excellent memory performance, including ultra-high endurance, ultra-fast switching speed and good retention characteristics. In addition, Ta 2 O 5 has the characteristics of high thermal stability and inactive chemical properties. As a gate dielectric material in a very mature CMOS process, SiO 2 has very clear material properties and parameters, and its preparation is simple and very controllable. The combination of the advantages of the two materials, coupled with a reasonable design of the physical mechanism, not only meets the requirements of compatible CMOS technology, but also realizes the bidirectional nonlinear self-rectification characteristics of the resistive memory. Lifting and mass production have significant implications.

该非线性自整流阻变存储器的制备方法如下:The preparation method of the nonlinear self-rectifying resistive variable memory is as follows:

1)利用光刻技术在光刻胶上定义底电极图形,采用PVD方法在硅衬底上淀积Pt底电极材料,厚度为50nm,再去除光刻胶,如图2(A)所示;1) Define the bottom electrode pattern on the photoresist by using photolithography technology, deposit Pt bottom electrode material on the silicon substrate by PVD method, the thickness is 50nm, and then remove the photoresist, as shown in Figure 2 (A);

2)采用PVD方法在底电极上淀积一层Ta2O5阻变层薄膜材料,厚度为20nm,如图2(B)所示;2) Deposit a layer of Ta 2 O 5 resistive layer film material on the bottom electrode by PVD method, with a thickness of 20nm, as shown in Figure 2(B);

3)采用PVD方法在阻变层上淀积一层SiO2能带修饰层材料实现双向非线性自整流,厚度为5nm,如图2(C)所示;3) Deposit a layer of SiO2 energy band modification layer material on the resistive layer by PVD method to realize bidirectional nonlinear self-rectification, with a thickness of 5nm, as shown in Figure 2(C);

4)先用光刻技术在光刻胶上定义出来的底电极引出孔图形,再采用干法刻蚀的方法在阻变层和能带修饰层刻蚀出底电极引出孔,并去除光刻胶,如图2(D)所示;4) First use photolithography technology to define the bottom electrode lead-out hole pattern on the photoresist, and then use dry etching to etch the bottom electrode lead-out hole in the resistive layer and energy band modification layer, and remove the photoresist. Glue, as shown in Figure 2 (D);

5)利用光刻技术在光刻胶上定义顶电极图形,采用PVD方法在能带修饰层上淀积Ta顶电极材料,厚度为200nm,再去除光刻胶即得到该阻变存储器,如图2(E)所示。5) Use photolithography to define the top electrode pattern on the photoresist, and use the PVD method to deposit Ta top electrode material on the energy band modification layer with a thickness of 200nm, and then remove the photoresist to obtain the resistive variable memory, as shown in the figure 2(E).

实施例2Example 2

本实施例2提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器采用硅衬底,采用TaN作为底电极材料,采用SrTiO3作为阻变层材料,采用HfO2作为能带修饰层材料,采用TaN作为顶电极材料。This embodiment 2 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The resistive variable memory uses a silicon substrate, TaN is used as the bottom electrode material, SrTiO is used as the resistive layer material, and HfO is used as the energy band As the material of the modification layer, TaN is used as the top electrode material.

该非线性自整流阻变存储器的制备方法如下:The preparation method of the nonlinear self-rectifying resistive variable memory is as follows:

1)利用光刻技术在光刻胶上定义底电极图形,采用蒸发淀积方法在硅衬底上淀积TaN底电极材料,厚度为200nm,再去除光刻胶;1) Defining the bottom electrode pattern on the photoresist by using photolithography technology, depositing TaN bottom electrode material on the silicon substrate by evaporation deposition method, with a thickness of 200nm, and then removing the photoresist;

2)采用PVD方法在底电极上淀积一层SrTiO3阻变层薄膜材料,厚度为50nm; 2 ) Deposit a layer of SrTiO3 resistive layer film material on the bottom electrode by PVD method, with a thickness of 50nm;

3)采用ALD方法在阻变层上淀积一层HfO2能带修饰层材料实现双向非线性自整流,厚度为20nm;3) Deposit a layer of HfO2 energy band modification layer material on the resistive layer by ALD method to realize bidirectional nonlinear self-rectification, with a thickness of 20nm;

4)先用光刻技术在光刻胶上定义出来的底电极引出孔图形,再采用干法刻蚀的方法在阻变层和能带修饰层刻蚀出底电极引出孔,并去除光刻胶;4) First use photolithography technology to define the bottom electrode lead-out hole pattern on the photoresist, and then use dry etching to etch the bottom electrode lead-out hole in the resistive layer and energy band modification layer, and remove the photoresist. glue;

5)利用光刻技术在光刻胶上定义顶电极图形,采用PVD方法在能带修饰层上淀积TaN顶电极材料,厚度为50nm,再去除光刻胶即得到该阻变存储器。5) Defining the top electrode pattern on the photoresist by photolithography technology, depositing TaN top electrode material on the energy band modifying layer by PVD method with a thickness of 50nm, and then removing the photoresist to obtain the resistive variable memory.

实施例3Example 3

本实施例3提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器采用玻璃衬底,采用Ir作为底电极材料,采用HfO2作为阻变层材料,采用TiO2作为能带修饰层材料,采用TiN作为顶电极材料。This embodiment 3 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The resistive variable memory uses a glass substrate, uses Ir as the bottom electrode material, uses HfO as the resistive layer material, and uses TiO as the energy band The modification layer material adopts TiN as the top electrode material.

该非线性自整流阻变存储器的制备方法如下:The preparation method of the nonlinear self-rectifying resistive variable memory is as follows:

1)利用光刻技术在光刻胶上定义底电极图形,采用蒸发淀积方法在玻璃衬底上淀积Ir底电极材料,厚度为100nm,再去除光刻胶;1) Defining the bottom electrode pattern on the photoresist by using photolithography technology, depositing Ir bottom electrode material on the glass substrate by evaporation deposition method, the thickness is 100nm, and then removing the photoresist;

2)采用ALD方法在底电极上淀积一层HfO2阻变层薄膜材料,厚度为5nm; 2 ) Deposit a layer of HfO on the bottom electrode by ALD method Resistive layer thin film material with a thickness of 5nm;

3)采用PVD方法在阻变层上淀积一层TiO2能带修饰层材料实现双向非线性自整流,厚度为1nm;3) Deposit a layer of TiO2 energy band modification layer material on the resistive layer by PVD method to realize bidirectional nonlinear self-rectification, with a thickness of 1nm;

4)先用光刻技术在光刻胶上定义出来的底电极引出孔图形,再采用干法刻蚀的方法在阻变层和能带修饰层刻蚀出底电极引出孔,并去除光刻胶;4) First use photolithography technology to define the bottom electrode lead-out hole pattern on the photoresist, and then use dry etching to etch the bottom electrode lead-out hole in the resistive layer and energy band modification layer, and remove the photoresist. glue;

5)利用光刻技术在光刻胶上定义顶电极图形,采用蒸发淀积方法在能带修饰层上淀积TiN顶电极材料,厚度为100nm,再去除光刻胶即得到该阻变存储器。5) Defining the top electrode pattern on the photoresist by using photolithography technology, depositing TiN top electrode material on the energy band modifying layer by evaporation deposition method, with a thickness of 100nm, and then removing the photoresist to obtain the resistive variable memory.

实施例4Example 4

本实施例4提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器的各层材料组成及厚度与实施例1完全相同,其制备方法不同之处在于阻变层和能带修饰层均采用ALD方法淀积制成。This embodiment 4 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The material composition and thickness of each layer of the resistive variable memory are exactly the same as those in embodiment 1. The difference in the preparation method lies in the resistive variable layer and the energy band The modification layers are deposited by ALD method.

实施例5Example 5

本实施例5提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器的阻变层材料选用有机材料parylene,采用CVD方法进行制备,厚度为500nm,其它的组成、制备方法及参数与实施例1完全相同。This embodiment 5 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The resistive variable layer of the resistive variable memory is made of organic material parylene, prepared by CVD method, and the thickness is 500nm. Other compositions, preparation methods and Parameters are exactly the same as in Example 1.

实施例6Example 6

本实施例6提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器的阻变层材料选用有机材料parylene,采用CVD方法进行制备,厚度为350nm,其它的组成、制备方法及参数与实施例4完全相同。This embodiment 6 provides a non-linear self-rectifying resistive variable memory and its preparation method. The resistive variable layer of the resistive variable memory is made of organic material parylene, prepared by CVD method, and the thickness is 350nm. Other compositions, preparation methods and Parameters are exactly the same as in Example 4.

实施例7Example 7

本实施例7提供一种非线性自整流阻变存储器及其制备方法,该阻变存储器的阻变层材料选用有机材料parylene,采用CVD方法进行制备,厚度为200nm,其它的组成、制备方法及参数与实施例4完全相同。This embodiment 7 provides a nonlinear self-rectifying resistive variable memory and its preparation method. The resistive variable layer of the resistive variable memory is made of organic material parylene and prepared by CVD method with a thickness of 200nm. Other compositions, preparation methods and Parameters are exactly the same as in Example 4.

由上述实施例可知,制备过渡金属氧化物阻变层薄膜材料和能量修饰层材料,既可以采用PVD方法,也可以采用ALD方法,与PVD方法相比,ALD方法能够制备更薄;制备有机材料作阻变层采用CVD方法。It can be seen from the above examples that the preparation of the transition metal oxide resistive layer thin film material and the energy modification layer material can either use the PVD method or the ALD method. Compared with the PVD method, the ALD method can be thinner; the preparation of organic materials The CVD method is used as the resistive layer.

对于本发明提供的一种非线性自整流阻变存储器,采用DC Sweep方式得到的其阻变过程的电流-电压(I-V)特性如图1所示,图中,S1—正向电压的激励下由高阻态向低阻态的跃变过程;S2—低阻态保持过程;S3—正向低阻态非线性整流过程;S4—负向低阻态非线性整流过程;S5—负向电压的激励下由低阻态向高阻态的跃变过程;S6—高阻态保持过程。通过使该阻变存储器的底电极接地,则顶电极的电压可以控制该阻变存储器的阻值,使其发生高阻和低阻之间的转换,即该阻变存储器“0”,“1”两个状态之间的转换,证明可以实现阻变效应,在正向和负向电压的操作下,其电流-电压特性曲线可以展现出近似对称的非线性整流作用。For a kind of non-linear self-rectifying resistive variable memory provided by the present invention, the current-voltage (I-V) characteristic of its resistive change process that adopts DC Sweep mode to obtain is as shown in Figure 1, among the figure, under the excitation of S1-forward voltage The transition process from high resistance state to low resistance state; S2—low resistance state maintenance process; S3—positive low resistance state nonlinear rectification process; S4—negative low resistance state nonlinear rectification process; S5—negative voltage The transition process from low-resistance state to high-resistance state under the excitation; S6—high-resistance state maintenance process. By grounding the bottom electrode of the RRAM, the voltage of the top electrode can control the resistance value of the RRAM, making it switch between high resistance and low resistance, that is, the RRAM "0", "1" "The conversion between the two states proves that the resistive switching effect can be realized. Under the operation of positive and negative voltages, its current-voltage characteristic curve can show an approximately symmetrical nonlinear rectification effect.

通过将能带修饰层嵌入到阻变存储器中形成双层结构,利用能带修饰层材料的厚度变化,及合理设计阻变层、能带修饰层和电极材料间的能带结构匹配,可以实现对阻变存储器件的电流-电压特性进行优化。这是因为,如果能带修饰层选择禁带宽度大于阻变层禁带宽度的材料,且能带修饰层材料的导带底高于阻变材料的导带底,同时金属电极选择功函数较大的材料,则能带修饰层会与电极形成较高的势垒,此时如果能带修饰层材料厚度较薄,电子可以通过隧穿的方式到达阻变层,而隧穿电流有着非线性的特性,因此,可以实现非线性自整流的特性。By embedding the energy band modification layer into the resistive switch memory to form a double-layer structure, using the thickness change of the energy band modification layer material, and rationally designing the band structure matching between the resistance switch layer, the energy band modification layer and the electrode material, it can realize The current-voltage characteristics of resistive memory devices are optimized. This is because, if the energy band modification layer chooses a material with a larger band gap than the resistive layer, and the conduction band bottom of the energy band modification layer material is higher than that of the resistive material, and the metal electrode selects a lower work function If the material is large, the energy band modification layer will form a higher potential barrier with the electrode. At this time, if the material thickness of the energy band modification layer is thin, electrons can reach the resistive layer through tunneling, and the tunneling current has a nonlinear Therefore, the characteristics of nonlinear self-rectification can be realized.

图3为crossbar阵列及串扰电流路径示意图,由图可知,由于阵列中该器件阻值的读取,需要读取流经该器件的电流大小来判断器件是处于高阻态还是低阻态。最坏情况下,如果要读取crossbar阵列中的一个处于高阻的器件,而其周围的器件均处于低阻态时,当读取处于高阻态的器件时,电流会绕过这个处于高阻态的器件,而在周围的低阻器件上形成sneak电流。这种情况下,在crossbar结构中,串扰电流会流经的最短路径如图中的未选中的三个器件,即当选中器件(图中虚线内的器件)为Vread电压时,串扰路径上每个器件实际上的分压为三分之一Vread,读取到的电流实际为流过其周围处于低阻态器件的sneak电流值,造成误读。如果器件采用本发明提供的非线性自整流阻变存储器,从图1电流电压曲线上可以看出Vread读取的高阻态时的电流要大于三分之一Vread读取的低阻态电流,即由于低阻态的非线性自整流效应,读取路径的电阻要小于串扰路径,所以有效地抑制了串扰,负向电压时亦然。由此可知,低阻态时双向非线性自整流效应可以有效地抑制crossbar阵列中的串扰。Figure 3 is a schematic diagram of the crossbar array and the crosstalk current path. It can be seen from the figure that due to the reading of the resistance value of the device in the array, it is necessary to read the current flowing through the device to determine whether the device is in a high resistance state or a low resistance state. In the worst case, if you want to read a high-impedance device in the crossbar array, while the surrounding devices are in a low-impedance state, when reading the high-impedance device, the current will bypass this high-impedance device. The device in the resistive state forms a sneak current on the surrounding low-resistance devices. In this case, in the crossbar structure, the shortest path through which the crosstalk current will flow is the three unselected devices in the figure, that is, when the selected device (the device in the dotted line in the figure) is at the Vread voltage, each crosstalk path The actual voltage division of each device is one-third of Vread, and the read current is actually the sneak current value flowing through its surrounding devices in a low-impedance state, causing misreading. If the device adopts the nonlinear self-rectifying resistive memory provided by the present invention, it can be seen from the current-voltage curve in Fig. 1 that the current in the high-impedance state read by Vread will be greater than the low-impedance state current read by one third of Vread, That is, due to the non-linear self-rectification effect of the low resistance state, the resistance of the read path is smaller than that of the crosstalk path, so the crosstalk is effectively suppressed, even when the voltage is negative. It can be seen that the bidirectional nonlinear self-rectification effect in the low resistance state can effectively suppress the crosstalk in the crossbar array.

以上实施例仅用以说明本发明的技术方案而非对其进行限制,本领域的普通技术人员可以对本发明的技术方案进行修改或者等同替换,而不脱离本发明的精神和范围,本发明的保护范围应以权利要求所述为准。The above embodiments are only used to illustrate the technical solution of the present invention and not to limit it. Those of ordinary skill in the art can modify or equivalently replace the technical solution of the present invention without departing from the spirit and scope of the present invention. The scope of protection should be determined by the claims.

Claims (9)

1.一种非线性自整流阻变存储器,其特征在于,包括衬底和位于衬底上的底电极-阻变层-能带修饰层-顶电极结构。 1. A nonlinear self-rectifying resistive variable memory, characterized in that it comprises a substrate and a bottom electrode-resistive variable layer-energy band modification layer-top electrode structure on the substrate. 2.根据权利要求1所述的非线性自整流阻变存储器,其特征在于,所述底电极-阻变层-能带修饰层-顶电极结构为金属-绝缘体-绝缘体-金属电容结构或金属-半导体-半导体-金属电容结构。 2. The nonlinear self-rectifying resistive variable memory according to claim 1, wherein the bottom electrode-resistive layer-band modification layer-top electrode structure is a metal-insulator-insulator-metal capacitor structure or a metal - Semiconductor-semiconductor-metal capacitor structure. 3.根据权利要求1所述的非线性自整流阻变存储器,其特征在于, 3. The non-linear self-rectifying resistive variable memory according to claim 1, characterized in that, 所述衬底采用硅或玻璃; The substrate is made of silicon or glass; 所述底电极和顶电极采用金属材料,厚度为50nm-200nm; The bottom electrode and the top electrode are made of metal materials with a thickness of 50nm-200nm; 所述阻变层采用具有阻变特性的过渡金属氧化物,厚度为5nm-50nm;或采用有机材料,厚度为200nm-500nm; The resistive layer is made of a transition metal oxide with resistive properties, with a thickness of 5nm-50nm; or an organic material, with a thickness of 200nm-500nm; 所述能带修饰层采用氧化物,厚度为1-20nm。 The energy band modifying layer is made of oxide with a thickness of 1-20nm. 4.根据权利要求3所述的非线性自整流阻变存储器,其特征在于, 4. The non-linear self-rectifying resistive variable memory according to claim 3, characterized in that, 所述金属材料为Ti、Al、Au、W、Cu、Ta、Pt、Ir或TiN、TaN; The metal material is Ti, Al, Au, W, Cu, Ta, Pt, Ir or TiN, TaN; 所述过渡金属氧化物为TaOx、HfOx、SiOx或SrTiO3,所述有机材料为parylene; The transition metal oxide is TaOx, HfOx, SiOx or SrTiO 3 , and the organic material is parylene; 所述氧化物为SiO2、TiO2或HfO2The oxide is SiO 2 , TiO 2 or HfO 2 . 5.一种非线性自整流阻变存储器的制备方法,包括如下步骤: 5. A method for preparing a non-linear self-rectifying resistive variable memory, comprising the steps of: 1)定义底电极图形,按照该图形在衬底上制备底电极; 1) Define the bottom electrode pattern, and prepare the bottom electrode on the substrate according to the pattern; 2)采用PVD、ALD或CVD的方法在底电极上淀积阻变层; 2) Depositing a resistive layer on the bottom electrode by PVD, ALD or CVD; 3)采用PVD或ALD的方法在阻变层上淀积能带修饰层; 3) Depositing an energy band modifying layer on the resistive layer by means of PVD or ALD; 4)定义底电极引出孔图形,按照该图形在阻变层和能带修饰层刻蚀出底电极引出孔; 4) Define the bottom electrode lead-out hole pattern, and etch the bottom electrode lead-out hole in the resistive layer and the energy band modification layer according to the pattern; 5)定义顶电极图形,按照该图形在修饰层上制备顶电极。 5) Define the pattern of the top electrode, and prepare the top electrode on the modification layer according to the pattern. 6.根据权利要求5所述的制备方法,其特征在于,所述步骤1)、4)和5)中定义图形的方法是,利用光刻技术在光刻胶上定义图形。 6. The preparation method according to claim 5, characterized in that, the method of defining the pattern in the steps 1), 4) and 5) is to define the pattern on the photoresist by using photolithography technology. 7.根据权利要求5所述的制备方法,其特征在于,所述底电极和顶电极的制备方法包括PVD和蒸发淀积方法。 7. The preparation method according to claim 5, characterized in that, the preparation methods of the bottom electrode and the top electrode include PVD and evaporation deposition methods. 8.根据权利要求5所述的制备方法,其特征在于,所述阻变层采用具有阻变特性的过渡金属氧化物,厚度为5nm-50nm;或采用有机材料,厚度为200nm-500nm。 8 . The preparation method according to claim 5 , wherein the resistive layer is a transition metal oxide with resistive properties, with a thickness of 5nm-50nm; or an organic material, with a thickness of 200nm-500nm. 9.根据权利要求5所述的制备方法,其特征在于,所述能带修饰层采用氧化物,厚度为1-20nm。 9. The preparation method according to claim 5, characterized in that the energy band modifying layer is made of an oxide with a thickness of 1-20 nm.
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