CN1355417A - Method of Measuring Equivalent Gate Channel Length by C-V Method - Google Patents
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Abstract
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本发明关于一种测量一等效栅极沟道长度的方法,特别是关于一种以一电容-电压法(capacitance-voltage method,C-Vmethod)测量一等效栅极沟道长度的方法。The present invention relates to a method for measuring the length of an equivalent gate channel, in particular to a method for measuring the length of an equivalent gate channel by a capacitance-voltage method (C-V method).
在互补式金属氧化半导体制造技术中,栅极沟道长度是一个关键参数用来设计元件效能(电路模式),短沟道设计,以及制程控制。栅极沟道长度不同于栅极长度取决于栅极微影技术及蚀刻的偏差,而是取决于源极/漏极的侧相扩散。In CMOS fabrication technology, gate channel length is a key parameter for designing device performance (circuit mode), short channel design, and process control. The gate channel length is different from the gate length due to gate lithography and etching deviation, but depends on the source/drain lateral phase diffusion.
通常,栅极沟道长度是使用一电流-电压法(current-voltage method,I-Vmethod)来求得,此I-V法是以一系列成线(或低漏极偏差)的I-V曲线,其中包含了许多不同遮罩长度的元件的I-V曲线加以计算求出。然而,在深次微米区域中金属氧化半导体场效电晶体得栅极沟道长度变得更难去测量。因为,随着栅极电压的变化迁移率(mobility)会有更大的变异,更显著的效应在梯度源极/漏极掺杂(graded source/drain doping)的呈现,以及线宽依赖的微影技术偏差在接近光学上的极限。Usually, the gate channel length is obtained by using a current-voltage method (I-Vmethod). This I-V method is based on a series of lined (or low drain deviation) I-V curves, including The I-V curves of many components with different mask lengths were calculated. However, the gate channel length of MOSFETs becomes more difficult to measure in the deep sub-micron region. Because, with the change of gate voltage, there will be a greater variation in mobility, the more significant effect is in the appearance of graded source/drain doping, and the line width dependent micro The deviation of shadow technology is approaching the limit of optics.
然而,一般I-V法适用于长沟道设计的元件,而并不完全适用于短沟道设计的元件。因此,一种改良的沟道长度提取算法(channel length extractionalgorithm)因应而生,例如一移位和比率法(shift and ratio method,S & Dmethod)。然而,此S & D法在使用上相当复杂繁琐且无法分别求出栅极蚀刻偏差长度Lpb和栅极-漏极覆盖长度Loverlap。However, the general IV method is suitable for components with long channel design, but not completely suitable for components with short channel design. Therefore, an improved channel length extraction algorithm (channel length extraction algorithm), such as a shift and ratio method (S & D method), was born accordingly. However, the S&D method is quite complicated and cumbersome in use and cannot separately calculate the gate etching deviation length L pb and the gate-drain coverage length L overlap .
因此,随着元件不断缩小已知测量沟道长度方法已不符目前的需要,找出一简单又适合的方法就成为一重要课题,特别是用来测量一栅极沟道长度,一栅极蚀刻偏差长度,和一栅极-漏极覆盖长度。Therefore, with the continuous reduction of components, the known method of measuring channel length does not meet the current needs, and finding a simple and suitable method has become an important issue, especially for measuring a gate channel length, a gate etching method, etc. offset length, and a gate-drain overlay length.
本发明的一目的是使用一C-V法来测量一元件的一等效栅极沟道长度。An object of the present invention is to measure an equivalent gate channel length of a device using a C-V method.
本发明的另一目的是使用一C-V法更准确地测量一元件中的一栅极-漏极重叠(gate-to-drain overlap)长度和一栅极蚀刻偏差(gate etch bias)长度。Another object of the present invention is to more accurately measure a gate-to-drain overlap length and a gate etch bias length in a device using a C-V method.
根据以上所述的目的,本发明提供了一种以一C-V法可同时测量一等效栅极沟道长度,一栅极-漏极重叠长度,和一栅极蚀刻偏差长度的方法,此方法至少包含下列步骤。首先,提供一第一元件包含一源极/漏极和一栅极在一衬底上。其中,此栅极具有一预定长度L1,一预定宽度W1,和一预定高度H1,且预定高度垂直于预定长度。然后,提供一负电压在第一元件的栅极上并测量在第一元件的栅极和源极/漏极间的一第一电容。接着,再提供一正电压在第一元件的栅极上并测量在第一元件的栅极和源极/漏极间的一第二电容。之后,使用测量第一电容以求出第一元件的一栅极-漏极重叠(gate-to-drain overlap)长度。接着,继续使用测量第二电容以求出第一元件的一栅极蚀刻偏差(gate etch bias)长度。最后,藉栅极-漏极重叠长度和栅极蚀刻偏差长度计算出第一元件的等效栅极沟道长度。According to the purpose described above, the present invention provides a kind of method that can simultaneously measure an equivalent gate channel length, a gate-drain overlapping length, and a method for gate etching deviation length with a CV method. Include at least the following steps. First, a first device including a source/drain and a gate on a substrate is provided. Wherein, the gate has a predetermined length L 1 , a predetermined width W 1 , and a predetermined height H 1 , and the predetermined height is perpendicular to the predetermined length. Then, apply a negative voltage on the gate of the first element and measure a first capacitance between the gate and source/drain of the first element. Next, provide a positive voltage on the gate of the first device and measure a second capacitance between the gate and source/drain of the first device. Afterwards, a gate-to-drain overlap length of the first element is obtained by measuring the first capacitance. Then, continue to use the measurement of the second capacitance to obtain a gate etch bias length of the first device. Finally, the equivalent gate channel length of the first element is calculated by using the gate-drain overlapping length and the gate etching deviation length.
图1是依据本发明所揭露的方法在一金属氧化半导体元件中定义出不同概念的各种长度。FIG. 1 shows various lengths defining different concepts in a metal oxide semiconductor device according to the method disclosed in the present invention.
图2是第一元件,第二元件,第三元件中各个栅极的预定尺寸。Fig. 2 is the predetermined dimensions of each gate in the first element, the second element, and the third element.
图3是电容-电压(C-V)测量的设定方式。Figure 3 shows how capacitance-voltage (C-V) measurements are set up.
图4是栅极到源极/漏极的测量电容对栅极电压的示图。Figure 4 is a graph of measured capacitance from gate to source/drain versus gate voltage.
图5是栅极到源极/漏极的测量电容每单位宽度对栅极电压的示图。Figure 5 is a graph of measured capacitance per unit width from gate to source/drain versus gate voltage.
主要部分的代表符号:Representative symbols of main parts:
10 衬底10 Substrate
12 源极/漏极12 source/drain
14 等效栅极沟道长度 14 Equivalent Gate Channel Length
16 栅极-漏极重叠长度16 Gate-drain overlap length
20 栅极氧化层20 Gate oxide layer
40 栅极40 grid
42 栅极长度42 Gate length
52 一半栅极蚀刻偏差长度52 half gate etching deviation length
60 栅极蚀刻遮罩60 Gate etch mask
62 栅极蚀刻长度62 Gate etching length
201 第一元件的栅极201 Gate of the first element
202 第二元件的栅极202 Gate of the second element
203 第三元件的栅极203 Gate of the third element
本发明的半导体设计可被广泛地应用到许多半导体设计中,并且可利用许多不同的半导体材料制作,当本发明以一较佳实施例来说明本发明方法时,熟悉此领域的人士应有的认知是许多的步骤可以改变,材料及杂质也可替换,这些一般的替换无疑地亦不脱离本发明的精神及范畴。The semiconductor design of the present invention can be widely applied in many semiconductor designs, and can utilize many different semiconductor materials to make, when the present invention illustrates the method of the present invention with a preferred embodiment, those who are familiar with this field should have It is recognized that many steps can be changed, and materials and impurities can also be replaced, and these general replacements undoubtedly do not depart from the spirit and scope of the present invention.
其次,本发明用示意图详细描述如下,在详述本发明实施例时,表示半导体结构的剖面图在半导体制程中会不依一般比例作局部放大以利说明,然不应以此作为有限定的认知。此外,在实际的制作中,应包含长度、宽度及深度的三维空间尺寸。Secondly, the present invention is described in detail with schematic diagrams as follows. When describing the embodiments of the present invention in detail, the cross-sectional view showing the semiconductor structure will not be partially enlarged according to the general scale in the semiconductor manufacturing process for the convenience of explanation, but it should not be used as a limited definition. Know. In addition, in actual production, the three-dimensional space dimensions of length, width and depth should be included.
本发明的一些实施例会详细描述如下。然而,除了详细描述外,本发明还可以广泛地在其他的实施例施行,且发明的范围不受限定,以所附的权利要求书为准。Some embodiments of the present invention are described in detail as follows. However, the invention may be practiced broadly in other embodiments than those described in detail, and the scope of the invention is not limited except by the appended claims.
参照图1,在此图上定义出一金属氧化半导体元件中各种不同概念的长度。其中,Lmask62系为一栅极蚀刻遮罩60的一设计长度,并且通过微影和蚀刻等制程会复制到衬底10上一栅极40的长度Lgate42。然而,Lgate可能比Lmask长或是比Lmask短,这完全取决于微影技术和蚀刻的偏差。另外,Lpb被定义为一栅极蚀刻偏差长度(gateetchbias),且图1中一长度52系为一半的栅极蚀刻偏差长度(Lpb/2)。虽然,Lgate是一重要的参数用来操作控制制程的品质,却没有简单的方式去获得此一参数。通常,Lgate的获得来自于电子式显微扫描器和剖开整个晶片。另外,随着缩小化的趋势在金属氧化半导体元件中一栅极-漏极重叠(gate-to-drainoverlap)长度Loverlap对元件的操作和效能影响越来越大,而Loverlap取决于衬底10内一源极/漏极12的侧相扩散。此外,Leff被定义为一等效栅极沟道长度(effectivegate channel length)在源极/漏极间,且Leff必须通过测量金属氧化半导体元件的一些电子信号来获得。Lgate和Leff可以一方程式(1)和一方程式(1)来表示Referring to FIG. 1 , the lengths of various concepts in a metal oxide semiconductor device are defined in this figure. Wherein, L mask 62 is a designed length of a
Lpb=Lmask-Lgate(1)L pb =L mask -L gate (1)
Leff=Lmask-Lpb-2*Loverlap(2)L eff =L mask -L pb -2*L overlap (2)
其中Lpb系为一栅极蚀刻偏差长度,Lmask是栅极蚀刻遮罩上一预设长度,Lgate系为一栅极长度,以及Loverlap系为一栅极-漏极重叠长度。Where L pb is a gate etching offset length, L mask is a predetermined length on the gate etching mask, L gate is a gate length, and L overlap is a gate-drain overlap length.
本发明的方法至少包含下列步骤。首先,提供一第一元件,一第二元件,和一第三元件。每一个元件系包含一源极/漏极和一栅极在一衬底上,如图1所示。参照图2,此图系为第一元件,第二元件,第三元件中各个栅极的预定尺寸,其栅极201,202,和203的一预定长度,一预定宽度,和一预定高度L1,W1,H1;L2,W2,H2;L3,W3,H3;分别为L,W,H;(L/2),W,H;以及L,(W/2),H。第一元件和第二元件的不同处在栅极的宽度不同,而第一元件和第三元件的不同在栅极的长度不同。这些元件系包含一固有电容每单位宽度Ctotal在栅极和源极/漏极间当栅极给予一个定电压时,且其中Ctotal可如方程式(3)所示The method of the present invention comprises at least the following steps. First, a first element, a second element, and a third element are provided. Each device includes a source/drain and a gate on a substrate, as shown in FIG. 1 . With reference to Fig. 2, this figure is the first element, the second element, the predetermined size of each grid in the third element, its grid 201,202, and a predetermined length of 203, a predetermined width, and a predetermined height L 1 , W 1 , H 1 ; L 2 , W 2 , H 2 ; L 3 , W 3 , H 3 ; L, W, H; (L/2), W, H; and L, (W/ 2), H. The difference between the first element and the second element lies in the width of the gate, and the difference between the first element and the third element lies in the length of the gate. These devices contain an inherent capacitance per unit width C total between the gate and source/drain when a constant voltage is applied to the gate, and where C total can be expressed as equation (3)
Ctotal=Cgate+2*Coverlap+2*Cfringing+(Coffset/W)(3)C total =C gate +2*C overlap +2*C fringing +(C offset /W)(3)
其中Cgate为一内部栅极-沟道(gate-to-channel)电容每单位宽度,Coverlap为一栅极-漏极重叠(gate-to-drain overlap)电容每单位宽度,Cfringing为一边缘(fringing)电容每单位宽度,Coffset为来自一测量装置的一偏差(deviation)电容,以及W为栅极的预定宽度。其中,方程式(3)中的边缘电容每单位宽度Cfringing又可表示为一方程式(4)Where C gate is an internal gate-to-channel capacitance per unit width, C overlap is a gate-to-drain overlap capacitance per unit width, and C fringing is a The fringing capacitance per unit width, C offset is a deviation capacitance from a measurement device, and W is the predetermined width of the gate. Among them, the fringing capacitance per unit width C fringing in equation (3) can be expressed as an equation (4)
Cfringing=2*εoxide/π*ln[1+(Hgate/Hgateoxide)](4)C fringing =2*ε oxide /π*ln[1+(H gate /H gateoxide )](4)
其中Hgate系为栅极的一预定高度,Hgateoxide系为如图1所示一栅极氧化层20的高度,以及εoxide系为栅极氧化层的一电场。在本方法中,Hgate,Hgateoxide,以及εoxide都为已知定值,所以Cfringing也是一定值。Wherein H gate is a predetermined height of the gate, H gate oxide is the height of a
下一步,进行一电子序号测试程序以获得一些元件的特征参数用来测量元件的等效栅极沟道长度。此电子信号测试程序结果如图4所示为栅极到源极/漏极的测量电容对栅极电压的作图,而电子信号测试程序的设定则如图3所示。当固有电容每单位宽度Ctotal在栅极被给予一负电压下时可表示为一累积(acculumation)电容每单位宽度Cacculumation,如下一方程式(5)所示In the next step, an electronic serial number test procedure is performed to obtain some characteristic parameters of the device for measuring the equivalent gate channel length of the device. The result of the electronic signal test procedure is shown in FIG. 4 as a plot of the measured capacitance from gate to source/drain versus gate voltage. The setup of the electronic signal test procedure is shown in FIG. 3 . When the inherent capacitance per unit width C total is given a negative voltage on the gate, it can be expressed as an accumulation (acculumation) capacitance per unit width C acculumation , as shown in the following equation (5)
Cacculumation=2*Coverlap+2*Cfringing+(Coffset/W)(5)C accumulation =2*C overlap +2*C fringing +(C offset /W)(5)
其中Cacculumation系为一累积电容每单位宽度在栅极被给予一负电压下时。参照图5,此图为栅极到源极/漏极的测量电容每单位宽度对栅极电压的作图。由图上可知栅极-漏极重叠电容每单位宽度Coverlap在累积区域时的变化相当小。Where C acculumation is an accumulative capacitance per unit width when the gate is given a negative voltage. Referring to Figure 5, this graph plots the measured capacitance from gate to source/drain per unit width versus gate voltage. It can be seen from the figure that the change of the gate-drain overlap capacitance per unit width C overlap in the accumulation area is quite small.
另一状态下,固有电容每单位宽度Ctotal在栅极被给予一正电压下时可表示为一反转(inversion)电容每单位宽度Cinversion,如下一方程式(6)所示In another state, the inherent capacitance per unit width C total can be expressed as an inversion capacitance per unit width C inversion when the gate is given a positive voltage, as shown in the following equation (6)
Cinversion=Cgate+2*Cfringing+(Coffset/W)(6)C inversion =C gate +2*C fringing +(C offset /W)(6)
其中Cinversion是反转电容每单位宽度当栅极被给予一正电压下时。where C inversion is the inversion capacitance per unit width when the gate is given a positive voltage.
接下来,测量一等效栅极沟道长度至少包含列步骤。首先,在第一元件和第二元件提供一负电压在栅极上。然后,在第一元件中量出一第一电容在栅极和源极/漏极间Cacculumation,measured,1和在第二元件中量出一第二电容在栅极和源极/漏极间Cacculumation,measured,2。下一步,将Cacculumation,measured,1和Cacculumation,measured,2代入方程式(5)中转换成一方程式(5-1)和一方程式(5-2)Next, measuring an equivalent gate channel length includes at least one row of steps. First, apply a negative voltage on the gate of the first element and the second element. Then, measure a first capacitance between the gate and source/drain in the first element C acculumation, measured, 1 and measure a second capacitance between the gate and source/drain in the second element Between C acculumation, measured, 2 . In the next step, C accumulation, measured, 1 and C accumulation, measured, 2 are substituted into equation (5) and converted into one equation (5-1) and one equation (5-2)
Caccumulation,measured,1=2Coverlap,1*W1+2Cfringing,1*W1+Coffset,1(5-1)C accumulation, measured, 1 = 2C overlap, 1 *W 1 +2C fringing, 1 *W 1 +C offset, 1 (5-1)
Caccumulation,measured,2=2Coverlap,2*W2+2Cfringing,2*W2+Coffset,2(5-2)C accumulation, measured, 2 = 2C overlap, 2 *W 2 +2C fringing, 2 *W 2 +C offset, 2 (5-2)
其中W1和W2系为已知,而Cfringing,1和Cfringing,2系为相同定值。因为栅极-漏极重叠电容每单位宽度在累积区域时的变化相当小,故Coverlap,1和Coverlep,1视为相等。因此,对方程式(5-1)和方程式(5-2)解联立即可获得第一元件的Coverlap和Coffset。Among them, W 1 and W 2 are known, while C fringing, 1 and C fringing, 2 are the same fixed value. C overlap, 1 and C overlep, 1 are considered equal because the gate-drain overlap capacitance per unit width varies relatively little over the accumulation area. Therefore, C overlap and C offset of the first element are immediately obtained by uncoupling Equation (5-1) and Equation (5-2).
然后,第一元件的一栅极-漏极重叠长度Loverlap可由一方程式(7)获得Then, a gate-drain overlap length L overlap of the first element can be obtained by an equation (7)
Loverlap=(Hgateoxide*Coverlap)/εoxide(7)L overlap =(H gateoxide *C overlap )/ε oxide (7)
其中Hgateoxide是如图1所示一栅极氧化层20的高度,以及εoxide是栅极氧化层的一电场。Where H gateoxide is the height of a
下一步,在第一元件和第三元件提供一正电压在栅极上。在第一元件中量出在栅极和源极/漏极间的一第三电容Cinversion,measured,1和在第二元件中量出在栅极和源极/漏极间的一第四电容Cinversion,measured,3。下一步,将Cinversion,measured,1和Cinversion,measured,3代入方程式(6)中转换成一方程式(6-1)和一方程式(6-2)Next, apply a positive voltage on the gates of the first element and the third element. A third capacitance C inversion,measured,1 is measured between gate and source/drain in the first element and a fourth capacitance is measured between gate and source/drain in the second element Capacitance C inversion, measured, 3 . In the next step, C inversion, measured, 1 and C inversion, measured, 3 are substituted into equation (6) and converted into an equation (6-1) and an equation (6-2)
Cinversion,measured,1=Cgate,1*W1+2Cfringing,1*W1+Coffset,1(6-1)C inversion, measured, 1 = C gate, 1 *W 1 +2C fringing, 1 *W 1 +C offset, 1 (6-1)
Cinversion,measured,3=Cgate,3*W3+2Cfringing,3*W3+Coffset,3(6-2)C inversion, measured, 3 = C gate, 3 *W 3 +2C fringing, 3 *W 3 +C offset, 3 (6-2)
其中W1和W3是已知的,而Cfringing,1和Cfringing,3是定值。Coverlap和Coffset可由方程式(5-1)和方程式(5-2)解联立即可获得。因此,可由方程式(6-1)和方程式(6-2)获得Cgate,1和Cgate,3。更进一步,可由一方程式(8)可求出第一元件的栅极长度Lgate where W 1 and W 3 are known, while C fringing, 1 and C fringing, 3 are fixed values. C overlap and C offset can be obtained immediately by solving equation (5-1) and equation (5-2). Therefore, C gate,1 and C gate,3 can be obtained from Equation (6-1) and Equation (6-2). Furthermore, the gate length L gate of the first element can be obtained from an equation (8)
.Lgate=(Cgate*W)*(L1-L3)/[(Cgate,1-Cgate,3)*W](8).L gate = (C gate *W)*(L 1 -L 3 )/[(C gate, 1 -C gate, 3 )*W] (8)
其中Lgate系为第一元件的栅极长度,Cgate是相当于第一元件的Cgate,1,以及W相当于W1和W3。Wherein L gate is the gate length of the first element, C gate is equivalent to the C gate, 1 of the first element, and W is equivalent to W 1 and W 3 .
接着,可以由方程式(1)Lpb=Lmask-Lgate获得栅极蚀刻偏差长度Lpb。最后,再由方程式(2)Leff=Lmask-Lpb-2*Loverlap获得等效栅极沟道长度Leff。Next, the gate etching deviation length L pb can be obtained from the equation (1) L pb =L mask −L gate. Finally, the equivalent gate channel length L eff is obtained from the equation (2) L eff =L mask -L pb -2*L overlap .
综合以上所述,本发明提供了一电容-电压法来测量一元件中的等效栅极沟道长度,并且可同时获得元件中的一栅极蚀刻偏差长度和一一栅极-漏极重叠长度。本方法中,使用本方法测量出的一栅极长度和实际电子显微式扫描器所量出的实际栅极长度误差低于5%。更甚者,本发明所使用的计算方法仅为简单的联立方程式,使用人工计算或电脑就可求出。随着设计法则的不断缩小化,本发明提供一简单的方法以求出元件中重要的参数。Based on the above, the present invention provides a capacitance-voltage method to measure the equivalent gate channel length in an element, and can simultaneously obtain a gate etching deviation length and a gate-drain overlap in the element length. In the method, the error between the grid length measured by the method and the actual grid length measured by the actual electron microscope scanner is less than 5%. What's more, the calculation method used in the present invention is only simple simultaneous equations, which can be obtained by manual calculation or computer. With the continuous miniaturization of design rules, the present invention provides a simple method to obtain important parameters in components.
以上所述仅为本发明之较佳实施例而已,并非用以限定本发明之申请专利范围;凡其它未脱离本发明所揭示之精神下所完成之等效改变或修饰,均应包含在下述的申请专利范围内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the patent scope of the present invention; all other equivalent changes or modifications that do not deviate from the spirit disclosed in the present invention should be included in the following within the scope of the patent application.
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CN110400668A (en) * | 2018-04-24 | 2019-11-01 | 莫列斯有限公司 | Electronic component |
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CN110400668A (en) * | 2018-04-24 | 2019-11-01 | 莫列斯有限公司 | Electronic component |
US11037895B2 (en) | 2018-04-24 | 2021-06-15 | Molex, Llc | Electronic component |
CN110400668B (en) * | 2018-04-24 | 2022-02-08 | 莫列斯有限公司 | Electronic component |
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