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CN115906723A - Circuit Simulation Method for Metal Work Function Fluctuation of Nanosheet Gate-Round Field-Effect Transistor - Google Patents

Circuit Simulation Method for Metal Work Function Fluctuation of Nanosheet Gate-Round Field-Effect Transistor Download PDF

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CN115906723A
CN115906723A CN202210628379.5A CN202210628379A CN115906723A CN 115906723 A CN115906723 A CN 115906723A CN 202210628379 A CN202210628379 A CN 202210628379A CN 115906723 A CN115906723 A CN 115906723A
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fluctuation
work function
phig
gate
effect transistor
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徐思逸
孙亚宾
石艳玲
李小进
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East China Normal University
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Abstract

The invention discloses a method for simulating a metal work function fluctuation circuit of a nanosheet ring gate field effect transistor, and belongs to the field of microelectronic devices. According to the circuit simulation method, firstly, a global model extraction is carried out on IV and CV data of a nanosheet gate-all-around field effect transistor based on a BSIM-CMG model, then a calculation formula is utilized to obtain the mean value and standard deviation of parameter PHIG fluctuation in the model under the influence of metal work function fluctuation, the mean value and the standard deviation are embedded into a simulation netlist of circuit simulation software to carry out circuit simulation, and then circuit performance parameters caused by metal work function fluctuation can be obtained. The device characteristic fluctuation influence which can be accurately obtained by adopting the invention is consistent with the result precision obtained by TCAD simulation. The traditional TCAD simulation volatility method is slow in speed and high in cost, and the circuit simulation method established by the invention is fast in speed and small in error.

Description

纳米片环栅场效应晶体管金属功函数波动电路仿真方法Circuit Simulation Method for Metal Work Function Fluctuation of Nanosheet Gate-Round Field-Effect Transistor

技术领域technical field

本发明属于微电子器件领域,具体涉及一种纳米片环栅场效应晶体管金属功函数波动电路仿真方法。The invention belongs to the field of microelectronic devices, and in particular relates to a method for simulating a metal work function fluctuation circuit of a nanosheet ring gate field effect transistor.

背景技术Background technique

一方面,环栅场效应晶体管目前的研究热点之一。相较于FinFET而言,环栅场效应晶体管具有更加优越的性能,其栅材料围绕着立体的沟道区域,能够更好地抑制短沟道效应实现更好的开关比并且在沟道中载流子能够沿着准一维的弹道进行传输能够更好地提高器件的驱动电流。在3nm技术节点下,环栅场效应晶体管将成为研究的主流器件。On the one hand, the gate-all-around field effect transistor is one of the current research hotspots. Compared with FinFET, the ring gate field effect transistor has more superior performance. Its gate material surrounds the three-dimensional channel region, which can better suppress the short channel effect, achieve a better switching ratio and carry current in the channel. The electrons can be transported along the quasi-one-dimensional ballistic trajectory, which can better improve the driving current of the device. Under the 3nm technology node, the gate-all-around field effect transistor will become the mainstream device for research.

但另一方面,因为环栅场效应晶体管的制备工艺变得更加复杂,器件中随机涨落的影响变得更加需要重视。器件的随机涨落是由于器件制备过程中,不可避免的工艺不确定性带来的器件电学特性影响,例如阈值电压等参数的涨落。在环栅场效应晶体管中,随机涨落源主要有金属功函数波动(WFV)、线边缘粗糙度(LER)、线宽度边缘粗糙度(LWR)。对于金属功函数波动来说,目前已有有效的集约模型,该模型将WFV的影响看作是对器件有效功函数的影响,根据金属晶粒的直径D、器件栅面积S、晶粒的功函数分布

Figure BDA0003678807900000011
得到器件有效功函数
Figure BDA0003678807900000012
的涨落大小。目前应用于平面MOSFET和FinFET的金属功函数波动的仿真无法直接应用于环栅场效应晶体管,主要是由于环栅场效应晶体管的结构更加复杂,原本的公式无法直接套用,需要进行修正,其次对于每个不同栅长的环栅场效应晶体管都需要做单独集约模型提取,耗费大量时间,而使用同时校准多个栅极长度器件的全局模型能够有效的解决这个问题。But on the other hand, because the fabrication process of gate-all-round field effect transistors has become more complex, the influence of random fluctuations in the device has become more important. The random fluctuation of the device is due to the influence of the electrical characteristics of the device caused by the inevitable process uncertainty during the device manufacturing process, such as the fluctuation of parameters such as threshold voltage. In the gate-all-around field effect transistor, the random fluctuation sources mainly include metal work function fluctuation (WFV), line edge roughness (LER), and line width edge roughness (LWR). For metal work function fluctuations, there is currently an effective intensive model, which regards the influence of WFV as the influence on the effective work function of the device. function distribution
Figure BDA0003678807900000011
Get the effective work function of the device
Figure BDA0003678807900000012
fluctuation size. The current simulation of metal work function fluctuations applied to planar MOSFETs and FinFETs cannot be directly applied to gate-all-around field-effect transistors, mainly because the structure of gate-all-around field effect transistors is more complex, and the original formula cannot be directly applied and needs to be corrected. Secondly, for Each gate-all-around field-effect transistor with different gate lengths requires a separate intensive model extraction, which consumes a lot of time, and using a global model that simultaneously calibrates devices with multiple gate lengths can effectively solve this problem.

正确地研究器件金属功函数波动对提升器件电学性能稳定性,以及评估器件电路性能非常重要。而目前大部分金属功函数波动研究所使用的TCAD仿真存在速度慢并且成本高的问题,所以建立准确的同时具有可预测性的金属功函数波动电路模拟仿真方法是十分必要的。It is very important to correctly study the fluctuation of the metal work function of the device to improve the stability of the electrical performance of the device and evaluate the circuit performance of the device. At present, the TCAD simulation used by most metal work function fluctuation researches has the problems of slow speed and high cost, so it is very necessary to establish an accurate and predictable metal work function fluctuation circuit simulation method.

发明内容Contents of the invention

本发明的目的在于提供一种基于可预测性集约模型的针对环栅场效应晶体管中金属功函数波动的电路仿真方法,该方法能够准确地得到的器件特性涨落影响,与目前使用的TCAD仿真相比速度快,且仿真得到的结果与TCAD精度一致,误差小。The object of the present invention is to provide a kind of circuit simulation method for metal work function fluctuation in ring gate field effect transistor based on predictability intensive model, this method can accurately obtain the influence of device characteristic fluctuation, and the TCAD simulation currently used Compared with the speed, the result obtained by simulation is consistent with the accuracy of TCAD, and the error is small.

实现本发明目的的具体技术方案是:The concrete technical scheme that realizes the object of the invention is:

一种纳米片环栅场效应晶体管金属功函数波动电路仿真方法,该方法包括如下步骤:A nanosheet ring gate field effect transistor metal work function fluctuation circuit simulation method, the method includes the following steps:

1)基于BSIM-CMG模型对纳米片环栅场效应晶体管进行全局参数提取,得到所有Target在工业误差范围内并能够应用于一系列沟道长度Lg变化的器件的全局模型及关键参数PHIG;1) Based on the BSIM-CMG model, the global parameters of the nanosheet ring gate field effect transistor are extracted, and the global model and the key parameter PHIG of all Targets within the industrial error range and which can be applied to a series of devices with channel length Lg changes are obtained;

2)修正关键参数PHIG;金属功函数波动主要影响BSIM-CMG模型中的核心参数PHIG,利用公式2) Correct the key parameter PHIG; metal work function fluctuations mainly affect the core parameter PHIG in the BSIM-CMG model, using the formula

μ(PHIG)=PHIG      (1)μ(PHIG)=PHIG (1)

Figure BDA0003678807900000021
Figure BDA0003678807900000021

分别得到金属功函数影响下PHIG涨落的均值和方差,其中公式中PHIG为已提取好的全局模型中无波动下的核心参数PHIG,

Figure BDA0003678807900000022
为有效功函数的涨落,能够直接反映在PHIG的变化上;D为金属晶粒的直径,nstack为纳米片的层数,W为沟道宽度,L为沟道长度,
Figure BDA0003678807900000023
为金属栅材料两种晶向对应的功函数之差,使用金属TiN<100>和<111>所对应的功函数之差,根据对晶粒统计分布的结果,两种晶向的比例为60%和40%,分别对应公式中晶向比例p1和1-p1的值;μ(PHIG)为PHIG涨落的均值,σ(PHIG)为PHIG涨落的标准差;所使用的计算公式修正了器件栅面积的算法,与目前已有的金属功函数波动计算公式相比更加贴和纳米片环栅场效应晶体管的结构;The mean value and variance of PHIG fluctuations under the influence of the metal work function are respectively obtained, where PHIG in the formula is the core parameter PHIG under no fluctuation in the extracted global model,
Figure BDA0003678807900000022
is the fluctuation of the effective work function, which can be directly reflected in the change of PHIG; D is the diameter of the metal grain, nstack is the number of layers of nanosheets, W is the channel width, L is the channel length,
Figure BDA0003678807900000023
is the difference between the work functions corresponding to the two crystal orientations of the metal gate material, using the difference between the work functions corresponding to the metal TiN<100> and <111>, according to the results of the statistical distribution of the crystal grains, the ratio of the two crystal orientations is 60 % and 40%, respectively corresponding to the value of the crystal orientation ratio p 1 and 1-p 1 in the formula; μ(PHIG) is the mean value of PHIG fluctuation, σ(PHIG) is the standard deviation of PHIG fluctuation; the calculation formula used The algorithm of the gate area of the device is revised, which is more suitable for the structure of the nanosheet ring gate field effect transistor compared with the existing metal work function fluctuation calculation formula;

3)将全局参数提取得到的全局模型以及PHIG涨落的均值和方差嵌入到电路仿真软件的仿真网表中,用电路仿真软件进行电路仿真,得到金属功函数波动影响下的器件漏极电流随栅极电压变化关系曲线Id-Vg图。3) Embed the global model obtained by extracting the global parameters and the mean value and variance of PHIG fluctuation into the simulation netlist of the circuit simulation software, and use the circuit simulation software to perform circuit simulation to obtain the device drain current variation under the influence of metal work function fluctuations. Gate voltage variation curve Id-Vg diagram.

本发明不同于目前的金属功函数波动电路仿真方法所使用的都是单一长度集约模型,而使用的是基于BSIM-CMG模型的全局模型,可以将同一个模型用于仿真多个栅长的器件,而不用针对每一个长度分别做集约模型提取。The present invention is different from the current metal work function fluctuation circuit simulation method that uses a single length intensive model, but uses a global model based on the BSIM-CMG model, and the same model can be used to simulate devices with multiple gate lengths , instead of intensive model extraction for each length.

本发明计算核心参数PHIG时,针对纳米片环栅场效应晶体管的结构修正了金属功函数波动主要影响值PHIG的方差计算公式,由nstack·W·L来计算面积,使结果更加接近真实器件金属功函数波动结果。When the present invention calculates the core parameter PHIG, the variance calculation formula of the main influence value PHIG of the metal work function fluctuation is corrected for the structure of the nanosheet ring gate field effect transistor, and the area is calculated by nstack W L, so that the result is closer to the real device metal Work function fluctuation results.

本发明能够准确地得到的器件特性涨落影响,与目前金属功函数波动研究所使用的TCAD仿真相比速度快,且仿真得到的结果与TCAD精度一致,误差小。而与之目前已有的金属功函数波动电路仿真方法相比,本发明要更加适用纳米片环栅场效应晶体管,并且采用了全局模型而非单一长度集约模型,更加快捷高效。Compared with the TCAD simulation used in the current metal work function fluctuation research, the invention can accurately obtain the influence of the device characteristic fluctuation, and the result obtained by the simulation is consistent with the TCAD accuracy and the error is small. Compared with the existing metal work function fluctuation circuit simulation method, the present invention is more suitable for nanosheet gate-all-around field effect transistors, and adopts a global model instead of a single length-intensive model, which is faster and more efficient.

附图说明Description of drawings

图1为本发明的流程示意图;Fig. 1 is a schematic flow sheet of the present invention;

图2为本发明使用的环栅场效应晶体管的三维结构;Fig. 2 is the three-dimensional structure of the gate-all-around field effect transistor used in the present invention;

图3为本发明使用的环栅场效应晶体管沿y方向剖面图;Fig. 3 is a sectional view along the y direction of the gate-all-around field effect transistor used in the present invention;

图4为本发明全局模型提取流程示意图;Fig. 4 is a schematic diagram of the global model extraction process of the present invention;

图5为加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的饱和区阈值电压Vtsat对比图;Fig. 5 is the comparison diagram of the threshold voltage Vtsat in the saturation region obtained by simulating the device circuit characteristics under the metal particle diameter of 3nm with traditional TCAD and the present invention using Hspice for adding metal work function fluctuations;

图6为加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的线性区阈值电压Vtlin对比图;Fig. 6 is the comparison diagram of the linear region threshold voltage Vtlin obtained by simulating the device circuit characteristics under the metal particle diameter of 3nm with traditional TCAD and the present invention using Hspice for adding metal work function fluctuation;

图7加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的饱和区亚阈值摆幅SS随饱和区阈值电压Vtasat变化对比图;Fig. 7 adds metal work function fluctuation with traditional TCAD and the present invention uses Hspice to simulate the circuit characteristics of the device under the metal particle diameter of 3nm, and the saturation region sub-threshold swing SS is compared with the saturation region threshold voltage Vtasat change;

图8加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的开启电流Ion随饱和区阈值电压Vtsat变化对比图;Fig. 8 adds metal work function fluctuation and uses traditional TCAD and the present invention uses Hspice to simulate the device circuit characteristics under the metal particle diameter of 3nm, and the turn-on current Ion is compared with the saturation region threshold voltage Vtsat variation diagram;

图9加入金属功函数波动用传统TCAD和本发明用Hspice的仿真器件电路特性得到的金属颗粒直径分别为3nm,5nm,7nm,10nm下饱和区阈值电压Vtsat的波动标准差变化对比图;Fig. 9 adds metal work function fluctuation with traditional TCAD and the present invention obtains with the simulation device circuit characteristic of Hspice and is respectively 3nm, 5nm, 7nm, the comparison chart of the fluctuation standard deviation change of saturation region threshold voltage Vtsat under 10nm;

图10为加入金属功函数波动用传统TCAD和本发明用Hspice的仿真器件电路特性得到的金属颗粒直径分别为3nm,5nm,7nm,10nm下开启电流Ion的波动标准差变化对比图。Fig. 10 is a comparison chart of fluctuation standard deviation variation of turn-on current Ion under 3nm, 5nm, 7nm, and 10nm diameters of metal particles obtained by adding metal work function fluctuations using traditional TCAD and the present invention using Hspice simulation device circuit characteristics.

具体实施方法Specific implementation method

下面将通过实施例并结合附图,详细描述本发明的电路仿真方法。The circuit simulation method of the present invention will be described in detail below through embodiments and in conjunction with the accompanying drawings.

本发明的一种纳米片环栅场效应晶体管金属功函数波动电路仿真方法,包括如下步骤:A method for simulating a metal work function fluctuation circuit of a nanosheet ring gate field effect transistor according to the present invention comprises the following steps:

1)基于BSIM-CMG模型对纳米片环栅场效应晶体管进行全局参数提取,得到所有Target符合产业界误差要求的全局模型,将无波动的模型卡嵌入到电路仿真软件的仿真网表中;1) Based on the BSIM-CMG model, the global parameters of the nanosheet ring gate field effect transistor are extracted to obtain a global model of all targets that meet the error requirements of the industry, and the model card without fluctuation is embedded in the simulation netlist of the circuit simulation software;

2)根据目前已建立的集约模型,将WFV的影响看作是对器件有效功函数的影响,根据金属晶粒的直径D、器件栅面积S、晶粒的功函数分布

Figure BDA0003678807900000048
按照以下公式计算得到器件有效功函数
Figure BDA0003678807900000049
的涨落大小:2) According to the currently established intensive model, the influence of WFV is regarded as the influence on the effective work function of the device. According to the diameter D of the metal grain, the area S of the device gate, and the work function distribution of the grain
Figure BDA0003678807900000048
Calculate the effective work function of the device according to the following formula
Figure BDA0003678807900000049
The fluctuation size of :

Figure BDA0003678807900000041
Figure BDA0003678807900000041

Figure BDA0003678807900000042
Figure BDA0003678807900000042

其中

Figure BDA0003678807900000043
in
Figure BDA0003678807900000043

则可得

Figure BDA0003678807900000044
由于环栅场效应晶体管中的面积应该由WL改为nstack·W·L,所以公式改写做:
Figure BDA0003678807900000045
得到金属功函数波动影响下有效功函数
Figure BDA0003678807900000047
涨落的均值和方差;then you can get
Figure BDA0003678807900000044
Since the area in the ring gate field effect transistor should be changed from WL to nstack W L, the formula is rewritten as:
Figure BDA0003678807900000045
Get the effective work function under the influence of metal work function fluctuation
Figure BDA0003678807900000047
Mean and variance of fluctuations;

3)有效功函数的涨落可以直接反映到最终的阈值电压Vth涨落上,影响BSIM-CMG中的核心参数PHIG,利用公式3) The fluctuation of the effective work function can be directly reflected in the fluctuation of the final threshold voltage V th , which affects the core parameter PHIG in BSIM-CMG, using the formula

μ(PHIG)=PHIGμ(PHIG)=PHIG

Figure BDA0003678807900000046
Figure BDA0003678807900000046

得到金属功函数波动影响下PHIG的涨落的均值和方差;Obtain the mean value and variance of the fluctuation of PHIG under the influence of metal work function fluctuation;

4)根据上述计算公式,得到金属功函数波动影响下的PHIG涨落的均值和方差,加入到电路仿真的网表中,用电路仿真软件进行电路仿真,即可得到金属功函数波动所造成的器件电学特性涨落影响,进而得到电路性能参数的涨落影响。4) According to the above calculation formula, the mean value and variance of PHIG fluctuations under the influence of metal work function fluctuations are obtained, which are added to the netlist of circuit simulation, and circuit simulation is performed with circuit simulation software to obtain the fluctuations caused by metal work function fluctuations. The influence of the fluctuation of the electrical characteristics of the device, and then the influence of the fluctuation of the circuit performance parameters.

实施例Example

本实施例考虑基于3nm环栅场效应晶体管中金属功函数波动对器件电路特性的影响,整体流程如图1电路仿真方法的流程示意图所示。3nm环栅场效应晶体管的基本结构如图2,本发明使用的环栅场效应晶体管的三维结构和图3沿y方向剖面图所示。This embodiment considers the influence of metal work function fluctuations in a 3nm gate-all-round field effect transistor on device circuit characteristics. The overall process is shown in FIG. The basic structure of a 3nm gate-all-round field effect transistor is shown in FIG. 2 , and the three-dimensional structure of the surround gate field effect transistor used in the present invention is shown in FIG. 3 along the y-direction cross-sectional view.

具体步骤:Specific steps:

1)如图4全局模型提取流程示意图所示,基于BSIM-CMG模型对纳米片环栅场效应晶体管进行全局参数提取,得到所有Target符合产业界误差要求的全局模型,将无波动的模型卡嵌入到电路仿真软件的仿真网表中;1) As shown in the schematic diagram of the global model extraction process in Figure 4, based on the BSIM-CMG model, the global parameters of the nanosheet ring gate field effect transistor are extracted to obtain a global model that meets the error requirements of the industry for all targets, and the model card without fluctuations is embedded to the simulation netlist of the circuit simulation software;

2)根据目前已有的集约模型,根据金属晶粒的直径D、器件栅面积S、晶粒的功函数分布

Figure BDA0003678807900000055
代入如下公式计算得到器件有效功函数
Figure BDA0003678807900000054
的涨落大小:2) According to the existing intensive model, according to the diameter D of the metal grain, the area S of the device gate, and the work function distribution of the grain
Figure BDA0003678807900000055
Substituting the following formula to calculate the effective work function of the device
Figure BDA0003678807900000054
The fluctuation size of :

Figure BDA0003678807900000051
Figure BDA0003678807900000051

Figure BDA0003678807900000052
Figure BDA0003678807900000052

本实施例中采用的环栅场效应晶体管的Lg为12nm到18nm,W为21nm,nstack为三层,搭建器件基本结构为Lg为15nm的环栅场效应晶体管如图2所示;栅极金属为TiN,晶粒的直径D为3nm,TiN<111>(功函数为4.6eV)与TiN<100>(功函数为4.4eV)的比例约为60%和40%.因此,计算得到

Figure BDA0003678807900000053
The Lg of the gate-all-around field effect transistor adopted in this embodiment is 12nm to 18nm, the W is 21nm, and the nstack is three layers. For TiN, the grain diameter D is 3nm, and the ratio of TiN<111> (work function is 4.6eV) to TiN<100> (work function is 4.4eV) is about 60% and 40%. Therefore, the calculated
Figure BDA0003678807900000053

3)利用环栅场效应晶体管金属功函数波动集约模型中的PHIG的计算公式和已提取的全局模型,得到PHIG的均值和方差如下:3) Using the calculation formula of PHIG in the metal work function fluctuation intensive model of the gate-all-round field effect transistor and the extracted global model, the mean value and variance of PHIG are obtained as follows:

均值:μ(PHIG)=4.652421Mean value: μ(PHIG)=4.652421

方差:σ(PHIG)=0.009562Variance: σ(PHIG)=0.009562

4)将PHIG涨落的均值和方差加入到电路仿真的网表中,用电路仿真软件进行电路仿真,即可得到金属功函数波动所造成的器件电学特性涨落影响,进而得到电路性能参数的涨落影响。4) Add the mean value and variance of PHIG fluctuations to the netlist of circuit simulation, and use circuit simulation software to perform circuit simulation to obtain the influence of fluctuations in the electrical characteristics of the device caused by metal work function fluctuations, and then obtain the circuit performance parameters. Fluctuations affect.

图5为加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的饱和区阈值电压Vtsat对比图,其中TCAD仿真出来的Vtsat均值为0.11961V,标准差为9.09344E-4V,Hspice仿真出来的Vtsat均值为0.11405V,标准差为8.55199E-4V。Fig. 5 is the comparison diagram of threshold voltage Vtsat in the saturation region obtained by simulating the circuit characteristics of the device under the metal particle diameter of 3nm with traditional TCAD and the present invention using Hspice for adding metal work function fluctuations, wherein the Vtsat mean value of TCAD simulation is 0.11961V, standard deviation is 9.09344E-4V, the average value of Vtsat simulated by Hspice is 0.11405V, and the standard deviation is 8.55199E-4V.

图6为加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的线性区阈值电压Vtlin对比图,其中TCAD仿真出来的Vtlin均值为0.13622V,标准差为9.09322E-4V,Hspice仿真出来的Vtlin均值为0.13431V,标准差为7.58836E-4V。Fig. 6 is the comparison diagram of the threshold voltage Vtlin in the linear region obtained by using traditional TCAD and Hspice in the present invention to simulate the device circuit characteristics under the metal particle diameter of 3nm for adding metal work function fluctuations, wherein the Vtlin mean value of TCAD simulation is 0.13622V, standard deviation is 9.09322E-4V, the average value of Vtlin simulated by Hspice is 0.13431V, and the standard deviation is 7.58836E-4V.

图7加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的饱和区亚阈值摆幅SS随饱和区阈值电压Vtasat变化对比图,其中TCAD仿真出来的SS均值为66.381,Hspice仿真出来的SS均值为68.377。Fig. 7 adds metal work function fluctuation with traditional TCAD and the present invention uses Hspice to simulate the device circuit characteristics under the metal particle diameter of 3nm and compares the sub-threshold swing SS in the saturation region with the threshold voltage Vtasat in the saturation region. Among them, the TCAD simulated The mean value of SS is 66.381, and the mean value of SS simulated by Hspice is 68.377.

图8加入金属功函数波动用传统TCAD和本发明用Hspice在金属颗粒直径为3nm下仿真器件电路特性得到的开启电流Ion随饱和区阈值电压Vtsat变化对比图,其中TCAD仿真出来的Ion均值为1.52E-04,Hspice仿真出来的Ion均值为1.52006E-4A。Fig. 8 adds metal work function fluctuation and uses traditional TCAD and the present invention uses Hspice to simulate the circuit characteristics of the device under the metal particle diameter of 3nm. The comparison diagram of the turn-on current Ion obtained by simulating the device circuit characteristics with the threshold voltage Vtsat in the saturation region, wherein the average value of Ion simulated by TCAD is 1.52 E-04, the average Ion value simulated by Hspice is 1.52006E-4A.

图9加入金属功函数波动用传统TCAD和本发明用Hspice的仿真器件电路特性得到的金属颗粒直径分别为3nm,5nm,7nm,10nm下饱和区阈值电压Vtsat的波动标准差变化对比图。Fig. 9 adds metal work function fluctuation and uses traditional TCAD and the present invention uses the simulation device circuit characteristic of Hspice to obtain, and the metal particle diameter is respectively 3nm, 5nm, 7nm, the contrast chart of fluctuation standard deviation change of threshold voltage Vtsat in the saturation region under 10nm.

图10为加入金属功函数波动用传统TCAD和本发明用Hspice的仿真器件电路特性得到的金属颗粒直径分别为3nm,5nm,7nm,10nm下开启电流Ion的波动标准差变化对比图。Fig. 10 is a comparison chart of fluctuation standard deviation variation of turn-on current Ion under 3nm, 5nm, 7nm, and 10nm diameters of metal particles obtained by adding metal work function fluctuations using traditional TCAD and the present invention using Hspice simulation device circuit characteristics.

Claims (3)

1. A method for simulating a metal work function fluctuation circuit of a nanosheet ring gate field effect transistor is characterized by comprising the following steps:
1) Carrying out global parameter extraction on the nanosheet gate all-around field effect transistor based on a BSIM-CMG model to obtain a global model and a core parameter PHIG of all devices with targets within an industrial error range and capable of being applied to channel length Lg variation;
2) Correcting a core parameter PHIG; respectively obtaining the mean value and the variance of the fluctuation of the core parameter PHIG under the influence of the metal work function by using a formula (1) and a formula (2):
μ(PHIG)=PHIG (1)
Figure FDA0003678807890000011
wherein, the PHIG in the formula is the core parameter PHIG under no fluctuation in the obtained global model,
Figure FDA0003678807890000012
the fluctuation of the effective work function can be directly reflected on the change of the PHIG; d is the diameter of the metal crystal grain, nstack is the number of the layers of the nanosheets, W is the width of the channel, L is the length of the channel, and the channel is selected according to the length of the channel>
Figure FDA0003678807890000013
For the difference of work functions corresponding to two crystal orientations of the metal gate material, metal TiN is used<100>And<111>the corresponding work function difference is that according to the result of statistical distribution of crystal grains, the proportion of two crystal orientations is 60 percent and 40 percent, which respectively correspond to the crystal orientation proportion p in the formula 1 And 1-p 1 A value of (d); mu (PHIG) is the mean value of the fluctuation of the PHIG, and sigma (PHIG) is the standard deviation of the fluctuation of the PHIG;
3) And embedding the global model obtained by extracting the global parameters and the mean value and variance of the fluctuation of the core parameter PHIG into a simulation netlist of circuit simulation software, and performing circuit simulation by using the circuit simulation software to obtain a device drain current variation relation curve Id-Vg graph along with the gate voltage under the influence of metal work function fluctuation.
2. The method for simulating a metal work function fluctuation circuit of a nanosheet ring gate field effect transistor of claim 1, wherein the global model is capable of using the same model for simulating devices of multiple gate lengths.
3. The nanosheet gate all-around field effect transistor metal work function fluctuation circuit simulation method of claim 1, wherein when a core parameter PHIG is calculated, a calculation formula of the nanosheet gate all-around field effect transistor is corrected according to the structure of the nanosheet gate all-around field effect transistor, and the area is calculated by nstack W L, so that the result is closer to a real device metal work function fluctuation result.
CN202210628379.5A 2022-06-06 2022-06-06 Circuit Simulation Method for Metal Work Function Fluctuation of Nanosheet Gate-Round Field-Effect Transistor Pending CN115906723A (en)

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