Method for evaluating semiconductor device

Abstract

A first relational expression representing a relationship among gate bias Vd, carrier mobility μ, electric effective channel length Leff and transconductance Gm, and a second relational expression representing a relationship among maximum-transconductance ratio Gmmax L=Lref/Gmmax L=Ltar between a target transistor and a reference transistor and electric effective channel lengths Leff and Lref of the respective transistors are used. Maximum transconductance Gmmax obtained when gate bias Vd is changed is determined and electric effective channel length Leff is estimated by substituting the value of maximum transconductance Gmmax in the second relational expression. The correlation between 1/Gmmax and Lgsem is strong enough to allow maximum transconductance Gmmax to be used in monitoring a process variation of a physical gate length.

Description

CROSS-REFERENCE TO RELATED APPLICATION

This application of Japanese Patent Application No. 2004-038898 filed on Feb. 16, 2004 including specification, drawings and claims is incorporated herein by reference in its entirety.

BACKGROUND OF THE INVENTION

The present invention relates to a method for evaluating a semiconductor device. The method is used to estimate a physical gate length of a MIS transistor based on electric characteristics of the MIS transistor.

The physical gate length of a MIS transistor is an important parameter for evaluating performance and processing conditions of a semiconductor device. The drain current and threshold voltage of a MIS transistor and variations in semiconductor-circuit performance, for example, largely depend on the gate length, and therefore the gate length needs to be accurately evaluated. In view of this, in development of a CMOS device, gate length L of a transistor to be measured is evaluated by measurement using a scanning electron microscope (SEM). However, it is difficult to evaluate all the measurement patterns by actual measurement because of time constraints.

On the other hand, in manufacturing management, dimensions are monitored using rocket marks. However, it is difficult to obtain gate lengths in various transistor sizes in a chip and data on variations within a wafer surface/chip surface. If a technique for enabling evaluation of a physical gate length from electric characteristics of a wafer completed as a sample is established, this technique is useful for simplifying device development, evaluating variations in a manufacturing process and specifying causes of failure. The physical gate length is also referred to as “an electric gate length” because this length is estimated from electric characteristics.

As a technique for evaluating an electric gate length, a Shift and Ratio (S&R) method disclosed in, for example, reference 1 (IEEE transactions on Electron Device, Vol. 47, No. 1, January 2000, 160-169) is generally used. The S&R method is a technique for determining electric effective channel length L_eff based on the assumption that electric effective channel length L_eff is proportional to channel resistance R_ch. With the S&R method, source/drain parasitic resistance R_sd is also estimated by calculation (hereinafter also simply referred to as “estimated”.) Therefore, use of the S&R method in development of a semiconductor device is very effective. Hereinafter, general concepts of the S&R method will be described.

FIG. 13 is an illustration for explaining definitions of dimensions regarding a gate electrode of a MIS transistor. In FIG. 13, L_mask is the size of an etching mask used for patterning the gate electrode, L_gate is an electric gate length, L_met is the metallurgical distance between pn junctions in a region between source and drain, and L_eff is an electric effective channel length.

FIG. 14 is a diagram showing an equivalent circuit including a MIS transistor in consideration of parasitic resistances of drain and source. Total resistance R_tot in the circuit shown in FIG. 14 is given by the following equations (1) and (2): $\begin{array}{cc}{R}_{\mathrm{tot}\left(\mathrm{Vg}\right)}=V_d^{\prime }/I_d& \left(1\right)\\ =R_{\mathrm{sd}}+R_{\mathrm{ch}}& \left(2\right)\end{array}$ where I_d is drain current, V_d is a drain voltage, R_sd is a total parasitic resistance of source and drain and R_ch is a channel region in a linear region.

FIG. 15 is a graph showing the dependence of total resistance R_tot on the gate length. As shown in FIG. 15, total resistance R_tot is proportional to electric gate length L_gate. In FIG. 15, an intersection point P of three lines L1 through L3 associated with different gate biases V_g indicates that R_tot=R_sd, i.e., electric effective channel length L_eff=L_gate−ΔL=0. In this case, R_sd is about 200 Ωμm and ΔL is about 0.04 μm.

Ideally, the current-voltage characteristic in the linear region is given by the following equation (3): I_d=W·μ_eff·C_o{(V_g−V_th)V_d−(1/2)V_d²}  (3) In a low drain bias region, the second term in Equation (3) can be disregarded, so that R_tot is given by the following equation (4): R_tot(Vg)=R_sd+[L_eff/{μ_eff·C_o·W(V_g−V_th)}]  (4) where μ_eff is effective carrier mobility, C_o is a capacitance of a gate oxide film, W is a gate width, V_d and V_g are a drain voltage and a gate bias, respectively, of a MIS transistor and V_th is a threshold voltage. If Equation (3) is generalized on the assumption that R_ch is proportional to electric effective channel length L_eff and is a function of (V_g−V_th), the following equation (5) is established R_tot(Vg)=R_sd+L_eff·f(V_g−V_th)  (5) The dependence of parasitic resistance R_sd on gate bias (V_g) is small. Accordingly, suppose parasitic resistance R_sd is not a function of gate bias (V_g), both sides of Equation (5) are differentiated with respect to V_g, and then Equations (6) and (7) from which an influence of parasitic resistance R_sd is removed are obtained as follows: $\begin{array}{cc}\begin{array}{c}{S}_{\left(\mathrm{Vg}\right)}^i=\frac{d{R}_{\mathrm{tot}}^i}{d{V}_g}\\ =L_{\mathrm{eff}}^i·\frac{df\left(V_g-V_{\mathrm{th}}^i\right)}{d{V}_g}\end{array}& \left(6\right)\\ \begin{array}{c}{S}_{\left(\mathrm{Vg}\right)}^O=\frac{d{R}_{\mathrm{tot}}^0}{d{V}_g}\\ =L_{\mathrm{eff}}^0·\frac{df\left(V_g-V_{\mathrm{th}}^0\right)}{d{V}_g}\end{array}& \left(7\right)\end{array}$ where superscript i means a target device and superscript 0 means a reference device.

In Equations (6) and (7), suppose Vⁱ_th=V⁰, df(V_g−Vⁱ_th)/dV_g=df(V_g−V⁰_th)/dV_g, ratio Sⁱ/S⁰ is equal to Lⁱ_eff/L⁰_eff.

In the S&R method, a shift corresponding to ΔV_th (the difference in V_th) is provided such that ratio r(S⁰=Sⁱ) with respect to S(=dR_tot/dV_g) between the target device and the reference device is constant, i.e., functions f(V_g−V_th) of the dependences of channel resistances on gate biases (V_g) in these devices are the same, and then a simple proportion, r=L⁰_eff/Lⁱ_eff, is established, thereby determining electric effective channel length L_eff. ΔV_th is determined by statistical calculation. Since R_tot is given by V_d/I_d, only data on the I_d−V_g characteristic in the linear region of the MIS transistor is needed. For the foregoing description, see reference 1, reference 2 (Proc. of IEDM, 1999, pp. 827-830) and reference 3 (Proc. of IEDM, 2002, pp. 117-120).

Though the S&R method has the foregoing advantages, problems described below arise when a large amount of data is analyzed and the gate length of a transistor used in a standard library cell is estimated. These problems are:

(1) An estimation algorithm is complicated and electric effective channel length L_eff needs to be calculated after measurement. Accordingly, a large amount of measurement data on the I_d−V_g characteristic needs to be accumulated and an enormous amount of calculation is required. Therefore, in the case of analyzing a large amount of data, it is difficult to apply the S&R method.

(2) Methods for estimating electric effective channel length L_eff are disclosed in references such as reference 1. However, no method for estimating a physical gate length has been found.

(3) The S&R method is used on the assumption that the target device and the reference device exhibit the same carrier mobility. However, as disclosed in reference 2, for example, the carrier mobility changes greatly depending on stress caused by an STI. The amount of this change is inversely proportional to the distance (finger length) from the interface between the STI and an active region to a center of the channel region, as disclosed in reference 3. In a transistor used in a standard library cell, the finger length has an arbitrary value, and thus the carrier mobility in a MIS transistor can take various values. Therefore, electric effective channel length L_eff obtained by estimation using the S&R method is affected by the layout dependence of the carrier mobility.

FIGS. 16A through 16C are a plan view showing a layout of a target device, a plan view showing a layout of a reference device and a plan view showing a layout of a standard cell having a complex configuration, respectively. In FIGS. 16A and 16B, FA and FB denote distances each from the interface between an STI and an active region to a center of channel. As shown in FIGS. 16A and 16B, FA<FB, so that μA<μB in an n-MIS transistor and μA>μB in a p-MIS transistor. Accordingly, the assumption that the carrier mobilities immediately under the channels of the respective MIS transistors are the same is not true in itself, and thus the mobility might cause an error in estimating electric effective channel length L_eff. As shown in FIG. 16C, in the standard cell having a complex active region, it is necessary to estimate electric effective channel length L_eff by correcting the carrier mobility.

SUMMARY OF THE INVENTION

It is therefore an object of the present invention to provide a method for quickly evaluating a physical parameter of a transistor from electric characteristics of the transistor with high accuracy, based on the finding that the maximum value of transconductance obtained when a gate bias of the transistor is changed hardly changes by a variation of a threshold voltage.

A first method for evaluating a semiconductor device according to the present invention is a method using a first relational expression and a second relational expression. The first relational expression represents a relationship among a gate bias, carrier mobility, an electric effective channel length and transconductance of a transistor. The second relational expression represents a relationship among a maximum-transconductance ratio between a target transistor and a reference transistor and electric effective channel lengths of the respective transistors. In this method, the maximum value of transconductance obtained when a gate bias of the target transistor is changed is determined as the maximum transconductance; and substitution of the value of the maximum transconductance in the second relational expression is performed, thereby estimating the electric effective channel length.

With this method, based on the finding that the maximum value of transconductance obtained when a gate bias of a transistor is changed hardly changes by a variation of a threshold voltage, easy algorithms are used and a short period of time is sufficient for measurement, as compared to a method for obtaining an electric effective channel length using an S&R method. That is, a method for evaluating a semiconductor device suitable for evaluating an electric effective channel length quickly and for evaluating a large amount of data is achieved. Use of this method enables quick monitoring of a process variation of gate length L_gate.

In this case, the second relational expression may be obtained by using actually-measured data and the second relational expression may be stored in the storage means.

If a physical gate length of the target transistor is estimated from the calculated electric effective channel length by using a correlation between the electric effective channel length and the physical gate length of the transistor, the physical gate length is easily determined, as a so-called electric gate length, from a transconductance characteristic of the target transistor.

If the carrier mobility of the target transistor is more accurately calculated using layout information and transconductance is corrected, electric effective channel length L_eff independent of a layout is calculated, thus enhancing accuracy in estimating the electric effective channel length.

If the value of the maximum transconductance is corrected in accordance with parasitic resistances of source and drain of the target transistor, the accuracy in estimating an electric effective channel length is enhanced. The method for the correction is preferably appropriately selected depending on a layout shape of the target transistor.

A second method for evaluating a semiconductor device according to the present invention is a method utilizing a correlation between an electric effective channel length of a transistor and a physical gate length of the transistor to calculate an electric effective channel length of a target transistor and thereby calculate a physical gate length of the target transistor as an electric gate length.

With this method, if an electric effective channel length of the target transistor is determined by a means, a physical gate length of the target transistor is obtained quickly.

As described above, with a method for evaluating a semiconductor device according to the present invention, an electric effective channel length and an electric gate length are quickly estimated with ease using simple algorithms.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a graph showing a correlation between the inverse of transconductance and critical-dimension (CD) SEM gate length L_gsem of a target device in a sample wafer.

FIG. 2 is a graph showing a result of actual measurement on the gate-bias dependence of transconductance obtained based on a first relational expression.

FIG. 3 is a graph showing a result of a simulation performed to determine how the dependence of transconductance on a gate bias changes when a substrate concentration is varied within the range of a variation in an actual process.

FIG. 4 is a graph showing a relationship between electric effective channel length L_eff and CD-SEM gate length L_gsem.

FIG. 5 is a graph showing a comparison between electric gate length L_gate obtained by a G_mmax method as a combination of first and second embodiments of the present invention and electric gate length L_gate obtained by a conventional S&R method.

FIG. 6 is a graph showing data on V_th roll-off of an n-MIS transistor with CD-SEM gate length L_gsem and electric gate length L_gate plotted on the abscissa.

FIG. 7 is a graph showing data on V_th roll-off of a p-MIS transistor with CD-SEM gate length L_gsem and electric gate length L_gate plotted on the abscissa.

FIG. 8 is a plan view schematically showing a layout of a MIS transistor in which finger lengths are asymmetric.

FIG. 9 is a plan view schematically showing a layout of a MIS transistor in which an active region is not rectangular in the plan view.

FIG. 10 is an equivalent circuit diagram showing a MIS transistor in consideration of parasitic resistance R_d of drain and parasitic resistance R_s of source.

FIGS. 11A and 11B are plan views schematically showing two examples of transistors with layouts in which gates are of the same shape and active regions are of different shapes and in each of which the shape of source and drain is symmetric with respect to the gate in the plan views.

FIGS. 12A and 12B are plan views schematically showing examples of transistors with layouts in which gates are of the same shape and active regions are of different shapes and in each of which the active region is asymmetric with respect to the gate.

FIG. 13 is an illustration for explaining definitions of dimensions regarding a gate electrode of a MIS transistor.

FIG. 14 is a diagram showing an equivalent circuit including a MIS transistor in consideration of parasitic resistances of drain and source.

FIG. 15 is a graph showing the dependence of the total resistance on the gate length.

FIGS. 16A through 16C are a plan view showing a layout of a target device, a plan view showing a layout of a reference device and a plan view showing a layout of a standard cell having a complex configuration, respectively.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Methods for evaluating a semiconductor device which will be described in the following embodiments of the present invention are based on the assumption that all the calculations are conducted by a computer.

Embodiment 1

Drain current I_d in a linear region of a MIS transistor is given by the following equation (20): I_d=(W·μ_eff·C_o/L_eff)·{(V_g−V_th)V_d−V_d²/2}  (20) and transconductance G_m, which is obtained by differentiating drain current with respect to a gate voltage, is given by a first relational expression of the following equation (21): G_m=δI_d/δV_g=(W·μ_eff·C_o/L_eff)V_d  (21) (where δ means a partial differentiation.)

In this case, drain current I_d is inversely proportional to electric effective channel length L_eff but threshold voltage V_th greatly depends on gate length L_gate, so that a comparison between the devices is not conducted in a simple manner. In view of this, in a first embodiment of the present invention, in order to minimize an error in estimating electric effective channel length L_eff due to a variation of threshold voltage V_th, maximum value G_mmax (maximum transconductance) of transconductance G_m of a target device is calculated so that electric effective channel length L_eff of the target device is calculated from the ratio of the calculated maximum value G_mmax to maximum transconductance G_mmax of a reference device in which electric effective channel length L_eff can be assumed to be the mask size. That is, a second relational expression of the following equation (22): L_eff=(G_{mmax L=Lref}/G_{mmax L=Ltar})×L_ref  (22) is stored in a storage unit. To obtain electric effective channel length L_eff, the relational expression of Equation (22) is taken from the storage unit and electric effective channel length L_eff is calculated by substituting the values of G_{mmax L=Lref}, G_{mmax L=Ltar} and L_ref in Equation (22). The second relational expression (22) may be standardized beforehand depending on the type of a semiconductor device so that a storage unit or a recording medium in/on which Equation (22) has been stored is used.

In this case, it was confirmed, using a sample wafer, that transconductance G_mmax of the target device is substantially inversely proportional to electric effective channel length L_eff as expressed by Equation (22).

FIG. 1 is a graph showing a correlation between the inverse of transconductance, i.e., 1/G_mmax, and critical-dimension (CD) SEM gate length L_gsem of a target device in the sample wafer. As shown in FIG. 1, the inverse of transconductance, 1/G_mmax, and gate length L_gsem show a correlation which is strong enough to allow maximum transconductance G_mmax to be used in monitoring a process variation of a physical gate length. That is, electric effective channel length L_eff is easily determined based on Equation (22).

It should be noted that the line of 1/G_mmax−L_gsem does not pass through the origin of the graph. This is because of the following reason. As the gate length of a transistor decreases, the channel resistance decreases but parasitic resistance R_sd is constant. Accordingly, the proportion of parasitic resistance R_sd increases as the gate length decreases. Therefore, to evaluate the absolute value of the gate length, it is necessary to correct the influence of parasitic resistance R_sd as described in an embodiment below.

Now, a characteristic in which the dependence of maximum transconductance G_mmax on threshold voltage V_th is extremely small will be described.

FIG. 2 is a graph showing a result of actual measurement on the dependence of transconductance G_m on gate bias V_g obtained based on the first relational expression (21). Such dependence of transconductance G_m on gate bias V_g is explained using the dependence of effective carrier mobility μ_eff on gate bias V_g.

Specifically, effective carrier mobility μ_eff decreases due to Coulomb scattering in a region where gate bias V_g is low (V_th<V_g<V_th+0.3 (V)) whereas effective carrier mobility μ_eff deteriorates due to phonon scattering in a region where gate bias V_g is high (V_g>V_th+0.3 (V)). Accordingly, transconductance G_m has maximum transconductance G_mmax. Effective carrier mobility μ_eff depends on a substrate concentration. Specifically, effective carrier mobility μ_eff is high at a low substrate concentration and is low at a high substrate concentration. Accordingly, a change in a gate bias causes the presence of a portion where the transconductance is at the maximum. In view of this, the maximum value of this transconductance is determined as maximum transconductance G_mmax.

FIG. 3 is a graph showing a result of a simulation performed to determine how the dependence of transconductance G_m on gate bias V_g changes when the substrate concentration (threshold voltage V_th) is varied within the range of a variation in an actual process. As shown in FIG. 3, threshold voltage V_th varies within the range of ±20 mV because of a process variation of the substrate concentration, and the range of the associated change in maximum transconductance G_mmax is ±1.7%. This range of ±1.7% is only due to a change in effective carrier mobility μ_eff and is very small as compared to the range of a change in saturation value I_dsat of drain current, which is ±6.5%. Therefore, maximum transconductance G_mmax is hardly affected by the influence of a variation of threshold voltage V_th.

In this embodiment, the maximum transconductance G_mmax obtained when gate bias V_d is changed is determined by using the first relational expression (21) showing a relationship among gate bias V_d, carrier mobility μ_eff, electric effective channel length L_eff and transconductance G_m and the second relational expression (22) showing a relationship among maximum-transconductance ratio G_{mmax L=Lref}/G_{mmax L=Ltar} between the target transistor and the reference transistor and electric effective channel lengths L_eff and L_ref. Then, electric effective channel length L_eff is estimated by substituting the value of maximum transconductance G_mmax in the second relational expression (22).

A method for obtaining electric effective channel length L_eff based on the first and second relational expressions (21) and (22) as described in this embodiment (hereinafter referred to as a “G_mmax method”) uses easy algorithms and requires only a short period of time for measurement, as compared to a method for obtaining electric effective channel length L_eff using the S&R method. Accordingly, this method is suitable for estimating an electric effective channel length quickly and for estimating a large amount of data.

Embodiment 2

The method for estimating electric effective channel length L_eff has been described in the first embodiment. However, a technique for converting the estimated length into electric gate length L_gate is needed in application to an actual analysis. Hereinafter, this technique and effects thereof will be described. It should be noted that electric gate length L_gate in this embodiment is a physical gate length of a transistor estimated through measurement of electric characteristics (especially transconductance) of the transistor. CD-SEM gate length L_gsem is a physical gate length of a transistor measured by a CD-SEM.

FIG. 4 is a graph showing a relationship between electric effective channel length L_eff and CD-SEM gate length L_gsem. As CD-SEM gate length L_gsem, data obtained by measuring the gate length of a MOS transistor patterned out of a polysilicon film by dry etching is used. As shown in FIG. 4, electric effective channel length L_eff and CD-SEM gate length L_gsem show a strong correlation. This correlation is also applicable to a different lot as long as a process variation is not significantly large in the same process. A physical gate length measured by another measurement means may be used instead of the CD-SEM gate length.

In this embodiment, the relationship between electric effective channel length L_eff and CD-SEM gate length L_gsem is grasped beforehand by an experiment and a table or an equation of a line showing a correlation between CD-SEM gate length L_gsem and electric effective channel length L_eff is created and is stored in a storage unit. Subsequently, electric effective channel length L_eff is determined by the method of the first embodiment or another method, and then electric gate length L_gate, which is CD-SEM gate length L_gsem estimated from electric effective channel length L_eff, is determined based on the line shown in FIG. 4 or a relational expression indicated by a line. Specifically, substitution of the value of electric effective channel length L_eff in an equation of a line is performed or the value of electric channel length L_eff is assigned to most-approximate data by using a table used to create the line. In other words, electric gate length L_gate is a physical gate length converted from electric effective channel length L_eff.

FIG. 5 is a graph showing a comparison between electric gate length L_gate obtained by a G_mmax method as a combination of the first and second embodiments and electric gate length L_gate obtained by a conventional S&R method. As shown in FIG. 5, electric gate length L_gate obtained by the G_mmax method and electric gate length L_gate obtained by the conventional S&R method substantially coincide with each other. Accordingly, with the G_mmax method, electric gate length L_gate is easily measured with an accuracy almost as high as that obtained by the S&R method.

That is, it is shown that if a correlation between electric effective channel length L_eff and CD-SEM gate length L_gsem measured with a physical method is once grasped, electric gate length L_gate can be obtained from electric effective channel length L_eff in transistors fabricated under the same processing conditions.

FIG. 6 is a graph showing data on V_th roll-off of an n-MIS transistor with CD-SEM gate length L_gsem and electric gate length L_gate plotted on the abscissa. The roll-off herein means a characteristic in which threshold voltage V_th gradually decreases as gate length L_g decreases. FIG. 7 is a graph showing data on V_th roll-off of a p-MIS transistor with CD-SEM gate length L_gsem and electric gate length L_gate plotted on the abscissa. FIGS. 6 and 7 both show data obtained when drain voltage V_d is 1.5V.

As shown in FIGS. 6 and 7, the V_th roll-off characteristic of electric gate length L_gate estimated from electric effective channel length L_eff by the method of this embodiment is almost the same as CD-SEM gate length L_gsem. Accordingly, the method of this embodiment is effectively applicable to actual devices.

Embodiment 3

Now, a technique for estimating the gate length of a transistor used in a standard library cell will be described.

As described in reference 3, suppose a is a finger length (the distance from the interface between an STI and an active region to a gate end), a_min is a minimum design rule of the finger length, a₀ is an equivalent finger length converted from stress caused by a nitride film, a silicide film and others, and U_0(a) is carrier mobility when the finger length is a. U_0(a) is the sum of a component inversely proportional to finger length a and a constant component independent of finger length a (stress independent of a nitride film, a silicide film and others), and thus the following equation (23) is established U_0(a)/U_0(amin)=(1/a+1/a₀)/(1/a_min+1/a₀)  (23)

If Equation (24) is determined as follows: V_mu0(W,L)=−a/(a₀+a_min)  (24) Equation (23) is altered as the following equation (25): U_0(a)=U_0(amin)[1+V_mu0(W,L)(a−a_min)/a]  (25)

Equation (25) is applicable to a case where finger lengths are asymmetric or an active region is not rectangular (i.e., a rectangle having a cut-away portion) in a plan view.

FIGS. 8 and 9 are plan views schematically showing layouts of MIS transistors in each of which finger lengths are asymmetric and an active region is not rectangular in the plan view, respectively. In FIGS. 8 and 9, OD1 and OD2 respectively denote layout patterns of active regions, GA1 and GA2 respectively denote layout patterns of gates, L and W denote the gate length and the gate width, respectively, in each transistor, aS and aD denote finger lengths of source and drain, respectively, W1 and W2 denote gate widths in a case where the active region is a rectangle having cut-away portions in the plan view, and a1 and a2 denote a larger finger length and a smaller finger length, respectively, in the case where the active region is a rectangle having cut-away portions in the plan view.

In the case of FIG. 9, it is sufficient to conduct estimation by the following equations (26) and (27): U_0(aeq)=[U_0(a1)+U_0(a2)W₂]/W  (26) 1/a_eq=W₁/(W·a₁)+W₂/(W·a₂)  (27)

In this embodiment, U_0(a) in Equation (23) is used as effective carrier mobility μ_eff in Equation (21), so that carrier mobility μ_eff for calculating maximum transconductance G_mmax is corrected based on layout information. Specifically, relationships expressed by Equations (21) and (23) are stored in a storage unit and layout information stored in the storage unit and the relational expressions of Equations (21) and (23) stored in the storage unit are taken out, thereby calculating electric effective channel length L_eff using the corrected carrier mobility. Accordingly, even in such a case where the active region is a rectangle having cut-away portions in a plan view, for example, an error in the carrier mobility resulting from a layout (i.e., the dependence of the mobility on the layout) is corrected, so that electric effective channel length L_eff is estimated more accurately in the first embodiment and the accuracy in estimating electric gate length L_gate is enhanced in the second embodiment.

Embodiment 4

In a fourth embodiment of the present invention, a technique for estimating transconductance G_m in consideration of source resistance R_s and drain resistance R_d will be described.

FIG. 10 is an equivalent circuit diagram showing a MIS transistor in consideration of parasitic resistance R_d of drain and parasitic resistance R_s of source. In FIG. 10, R_s and R_d are parasitic resistances of source and drain, respectively, VG and VD are a gate voltage and a drain voltage, respectively, applied from the outside, V_g and V_d are a gate voltage and a drain voltage inside the transistor, and I_d is drain current.

In this case, externally-applied drain voltage VD and externally-applied gate voltage VG are respectively given by the following equations (28) and (29): VD=V_d+(R_s+R_d)I_d  (28) VG=V_g+R_s·I_d  (29) As described above, drain current I_d is given by the following equations (30) and (31): I_d=β(V_g−V_th)V_d  (30) β=W·μ_eff·C_ox/L_eff  (31) Transconductance G_m actually measured is given by the following equation (32) G_m=δI_d/δVG  (32) (where δ means a partial differentiation.) Pure transconductance G_m′ inside the transistor is given by the following equation (33): $\begin{array}{cc}\begin{array}{c}{G}_m^{\prime }=\frac{\delta I_d}{\delta V_g}\\ =\beta ·V_d\end{array}& \left(33\right)\end{array}$ Accordingly, in consideration of Equations (28) and (29), the following equations (34) and (35) are established δI_d/δVG=−(R_s+R_d)*G_m  (34) δV_g/δVG=1−R_s·G_m  (35) Accordingly, if transconductance G_m is calculated based on the above definitions, $\begin{array}{cc}\begin{array}{c}{G}_m=\frac{\delta I_d}{\delta V_g}\\ =\beta [\left(V_g-V_{\mathrm{th}}\right)\left(\frac{\delta \mathrm{VD}}{\delta V_g}\right)+V_d\left[\left(\frac{\delta V_g}{\delta V_g}\right)\right]\\ =\beta \left[-\left(R_s+R_d\right)G_m\left(V_g-V_{\mathrm{th}}\right)+\left(1-R_s·G_m\right)V_d\right]\\ =\beta ·V_d-\beta ·R_s·G_m·V_d-\left(R_s+R_d\right)·G_m·\beta ·\left(V_g-V_{\mathrm{th}}\right)\\ =\beta ·V_d-\beta ·R_s·G_m·V_d-\left(R_s+R_d\right)·G_m·\left(\frac{I_d}{V_d}\right)\end{array}& \left(3\right)\end{array}$ If Equation (36) is rearranged with respect to G_m, the following equation (37) is established $\begin{array}{cc}\begin{array}{c}{G}_m=\beta ·\frac{V_d}{\left[1+R_s·\beta ·V_d+\left(R_s+R_d\right)\left(\frac{I_d}{V_d}\right)\right]}\\ =\frac{G_m^{\prime }}{\left[1+R_s·G_m^{\prime }+\left(R_s+R_d\right)\left(\frac{I_d}{V_d}\right)\right]}\end{array}& \left(37\right)\end{array}$ Accordingly, pure G_m′ inside the transistor is given by the following equation (38): G_m′=G_m[1+(R_s+R_d)(I_d/V_d)]/[1−R_s·G_m]  (38)

In this embodiment, maximum transconductance G_mmax is calculated more accurately with an error caused by parasitic resistances corrected, by the following equations (39): G_mmax′=G_mmax[1+(R_s+R_d)(I_d/V_d)]/[1−R_s·G_mmax]  (39) where R_s is a parasitic resistance of source of the transistor and R_d is a parasitic resistance of drain of the transistor. Accordingly, electric effective channel length L_eff is estimated more accurately in the first embodiment and the accuracy in estimating electric gate length L_gate is enhanced in the second embodiment.

Embodiment 5

In a fifth embodiment of the present invention, a technique for estimating source/drain resistance R_s/R_d in a case where an active region has a symmetrical shape.

FIGS. 11A and 11B are plan views schematically showing two examples of transistors with layouts A and B in which gates are of the same shape and active regions are of different shapes and in each of which the shape of source and drain is symmetric with respect to the gate in the plan view.

Internal maximum tranconductances G_m′_A and G_m′_B in layouts A and B are given by the following equations (40) and (41): G_m′_—A=β_—A·V_d=W·μ_eff—A·C_ox/L_eff  (40) G_m′_—B=β_—B·V_d=W·μ_eff—B·C_ox/L_eff  (41) where I_d—A and I_d—B are actually-measured values of drain current in layouts A and B, respectively, G_m—A and G_m—B are actually-measured values of maximum transconductance G_mmax in layouts A and B, respectively, and μ_eff—A and μ_eff—B are carrier mobilities in layouts A and B, respectively. Suppose drain parasitic resistance R_d is equal to source parasitic resistance R_s in layouts A and B. Then, since the layout shape of the active region is symmetric, substitution of R_d=R_s is conducted as $\begin{array}{cc}\frac{G_{\mathrm{m\_}}^{\prime }A}{G_{\mathrm{m\_}}^{\prime }B}=\frac{{\mu }_{\mathrm{eff\_}}A}{{\mu }_{\mathrm{eff\_}}B}=\frac{\left[G_{\mathrm{m\_}}A\left\{\frac{1+2R_s\left(\frac{I_{\mathrm{d\_}}A}{V_d}\right)}{\left\{1-R_s·G_{\mathrm{m\_}}A\right\}}\right\}\right]}{\left[\frac{G_{\mathrm{m\_}}B\left\{1+2R_s\left(\frac{I_{\mathrm{d\_}}B}{V_d}\right)\right\}}{\left\{1-R_s·G_{\mathrm{m\_}}B\right\}}\right]}& \left(42\right)\end{array}$ From Equation (42), source/drain parasitic resistance R_s/R_d is estimated from the ratio between internal maximum tranconductances G_m′_A and G_m′_B in layouts A and B.

Specifically, suppose in two transistors with layouts in which gates are of the same shape and active regions are of different shapes and in each of which the shape of source and drain is symmetric with respect to the gate in the plan view, parasitic resistances R_s and R_d are equal to each other. Then, with a technique for estimating parasitic resistance R_s from the ratio between internal values of maximum transconductances G_mmax, parasitic resistances R_s and R_d are determined quickly. An error caused by the fact that the line of 1/G_mmax−L_gsem in FIG. 1 does not pass through the origin can be disregarded. Consequently, electric effective channel length L_eff is estimated more accurately in the first embodiment and the accuracy in estimating electric gate length L_gate is enhanced in the second embodiment.

Now, a method for estimating source/drain parasitic resistances R_s and R_d in a case where the shape of an active region is asymmetric will be described.

FIGS. 12A and 12B are plan views schematically showing examples of transistors with layouts C and D in which gates are of the same shape and active regions are of different shapes and in each of which the active region is asymmetric with respect to the gate. As shown in FIGS. 12A and 12B, the shape of each active region is asymmetric with respect to the gate.

Internal maximum tranconductances G_m′_C and G_m′_D are given by the following equations (43) and (44): $\begin{array}{cc}\frac{G_m^{\prime }\mathrm{\_C}\mathrm{\_for}}{G_m^{\prime }\mathrm{\_D}\mathrm{\_for}}=\frac{\left[G_m\mathrm{\_C}\mathrm{\_for}\frac{\left\{1+\left(R_s+R_d\right)\left(\frac{I_d\mathrm{\_C}\mathrm{\_for}}{V_d}\right)\right\}}{\left\{1-R_s·G_m\mathrm{\_C}\mathrm{\_for}\right\}}\right]}{\left[\frac{G_m\mathrm{\_D}\mathrm{\_for}\left\{1+\left(R_s+R_d\right)\left(\frac{I_d\mathrm{\_D}\mathrm{\_for}}{V_d}\right)\right\}}{\left\{1-R_s·G_m\mathrm{\_D}\mathrm{\_for}\right\}}\right]}& \left(43\right)\\ \frac{G_m^{\prime }\mathrm{\_C}\mathrm{\_rev}}{G_m^{\prime }\mathrm{\_D}\mathrm{\_rev}}=\frac{\left[G_m\mathrm{\_C}\mathrm{\_rev}\frac{\left\{1+\left(R_d+R_s\right)\left(\frac{I_d\mathrm{\_C}\mathrm{\_rev}}{V_d}\right)\right\}}{\left\{1-R_d·G_m\mathrm{\_C}\mathrm{\_rev}\right\}}\right]}{\left[\frac{G_m\mathrm{\_D}\mathrm{\_rev}\left\{1+\left(R_d+R_s\right)\left(\frac{I_d\mathrm{\_D}\mathrm{\_rev}}{V_d}\right)\right\}}{\left\{1-R_d·G_m\mathrm{\_D}\mathrm{\_rev}\right\}}\right]}& \left(44\right)\end{array}$ where I_d—C_for and I_d—D_for are actually-measured values of forward drain current in layouts C and D, respectively, I_d—C_rev and I_d—D_rev are actually-measured values of backward drain current in layouts C and D, respectively, between which source and drain are replaced with each other, G_m—C_for and G_m—D_for are actually-measured values of G_mmax with respect to forward drain current in the layouts C and D, respectively, G_m—C_rev and G_m—D_rev are actually-measured values of G_mmax with respect to backward drain current in the layouts C and D, respectively, and R_s and R_d are parasitic resistances of source and drain, respectively, in layouts C and D. Accordingly, parasitic resistances R_s and R_d are estimated from the ratio between internal values of two types of G_mmax obtained in the layouts between which direction of source and drain is switched, as expressed by Equations (43) and (44).

Specifically, with a technique for estimating parasitic resistances R_s and R_d from the ratio between actually-measured internal values of two types of G_mmax in layouts between which the direction of source and drain is switched, parasitic resistances R_s and R_d are obtained quickly. An error caused by the fact that the line of 1/G_mmax−L_gsem in FIG. 1 does not pass through the origin can be disregarded. Consequently, electric effective channel length L_eff is estimated more accurately in the first embodiment and the accuracy in estimating electric gate length L_gate is enhanced in the second embodiment.

The present invention is applicable to evaluation of characteristics of a MIS transistor in LSI incorporated in various electric devices.

Claims

1. A method for evaluating a semiconductor device using storage means for storing a first relational expression and a second relational expression, the first relational expression representing a relationship among a gate bias, carrier mobility, an electric effective channel length and transconductance of a transistor, the second relational expression representing a relationship among a maximum-transconductance ratio between a target transistor and a reference transistor and electric effective channel lengths of the respective transistors, the method comprising the steps of: (a) taking the first relational expression from the storage means and determining, as the maximum transconductance, the maximum value of transconductance obtained when a gate bias of the target transistor is changed; and (b) taking the second relational expression from the storage means and substituting the value of the maximum transconductance of the target transistor determined in the step (a) in the second relational expression, thereby estimating the electric effective channel length of the target transistor.

2. The method of claim 1, further comprising the step of obtaining the second relational expression using actually-measured data and storing the second relational expression in the storage means, before the step (a) is performed.

3. The method of claim 1, wherein the storage means stores a correlation between an electric effective channel length of a transistor and a physical gate length of the transistor, and the method further comprises the step (c) of taking the correlation from the storage means and substituting the electric effective channel length calculated in the step (b) in the correlation, thereby estimating a physical gate length of the target transistor.

4. The method of claim 1, wherein the storage means stores layout information, the method further comprises the step (d) of taking layout information on the target transistor from the storage means and calculating the carrier mobility of the target transistor based on a layout, and in the step (a), the carrier mobility calculated in the step (d) is used as the carrier mobility in the first relational expression.

5. The method of claim 1, wherein in the step (a), maximum transconductance in which an error caused by a parasitic resistance in the target transistor is corrected is given by the following equation (A):

6. The method of claim 5, wherein in the step (a), the parasitic resistances Rs and Rd are estimated from a Gm′ ratio between two target transistors based on the assumption that the target transistors have gates of the same shape and active regions of different shapes and the shape of the source and the drain in the active region of each of the transistors is symmetric with respect to the gate in a plan view.

7. The method of claim 5, wherein in the step (a), the parasitic resistances Rs and Rd are estimated from two types of Gm′ ratios with respect to forward drain current and backward drain current in two target transistors which have gates of the same shape and active regions of different shapes and in each of which the shape of the source and the drain in the active region is asymmetric with respect to the gate in a plan view.

8. A method for evaluating a semiconductor device using storage means for storing a correlation between an electric effective channel length of a transistor and a physical gate length of the transistor, the method comprising the steps of: (a) calculating an electric effective channel length of a target transistor: and (b) taking the correlation from the storage means and substituting the electric effective channel length calculated in the step (a) in the correlation, thereby calculating a physical gate length of the target transistor as an electric gate length.