5.3 Linear Region

Step 1: Extract work function, interface charge and mobility model parameters for long gate length.

Extracted Parameters Device and Experimental Data Extraction Methodology
PHIG PHIG , CIT CIT A long device Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V Observe subthreshold region offset and slope.
U00 U0_0 , UA0 UA_0 , UD0 UD_0 , EU EU , ETAMOB ETAMOB A long device Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V Observe strong inversion region Id,lin I_{d,lin} and Gm,lin G_{m,lin} .

Note: Larger length is better, as it will minimize the short channel effect and emphasize carrier mobility, work function and interface charge related parameters.


Step 2: Refine Vth V_{th} roll-off, DIBL and SS degradation parameters.

Extracted Parameters Device and Experimental Data Extraction Methodology
DVT0 DVT0 , DVT1 DVT1 , CDSC CDSC , DVT2 DVT2 Both short and medium devices Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V Observe subthreshold region of all devices in the same plot. Optimize DVT0 DVT0 , DVT1 DVT1 , CDSC CDSC , DVT2 DVT2 .

Note: We do not need very accurate fitting because mobility, series resistance parameters are not determined yet.


Step 3: Extract low field mobility U0[L] U0[L] for long and medium gate lengths.

Extracted Parameters Device and Experimental Data Extraction Methodology
UP UP , LPA LPA Long and medium devices Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V . U0[L]=U00×(1UP×LeffLPA) U_0[L] = U0_0 \times (1 - UP \times L_{eff}^{-LPA} ) Observe strong inversion region Id,lin I_{d,lin} and Gm,lin G_{m,lin} , extract U0[L] U0[L] to get UP UP , LPA LPA . For each Li L_i , find Yi Y_i corresponding to Li L_i , fit (Li L_i , Yi Y_i ) by Eq(1) to extract UP UP , LPA LPA ). Refer to Fig. 16 for instance.

So far, we have good fit with data in subthreshold regions from long to short channel devices, and strong inversion for long channel devices. We need good fit for strong inversion in medium and short channel devices.

In linear region, current is to the first order, governed by low field mobility. So we start by tuning low field mobility values.

In short channel devices series resistance, coulombic scattering and enhanced mobility degradation effects are pronounced. To avoid the inuence of these effects, long and medium channel length devices are selected to especially extract low field mobility parameters.

Figure 16

Figure 16: Fit low field electron mobility with Lg L_g


Step 4: Extract mobility model and series resistance parameters for short gate lengths.

Extracted Parameters Device and Experimental Data Extraction Methodology
PARAM0 PARAM_0 , APARAM APARAM , BPARAM BPARAM , LINT LINT , LL LL , LLN LLN Short and medium devices Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V 1. Observe strong inversion region Id,lin I_{d,lin} and Gm,lin G_{m,lin} . Similar to Step 3, find values of UA[L] UA[L] , UD[L] UD[L] , RDSW[L] RDSW[L] and ΔL[L] \Delta L[L] that gives good fit to experimental data, varying them simultaneously. UA0 UA0 , UD0 UD0 are provided from Step 1 and RDSW0 RDSW0 , LINT LINT are provided from parameter initialization. 2. Variation of each parameter with respect to L L should be kept minimal with smooth continuous trend. 3. From the length dependence of UA[L] UA[L] , UD[L] UD[L] , RDSW[L] RDSW[L] and ΔL[L] \Delta L[L] , find AUA AUA , BUA BUA , AUD AUD , BUD BUD , ARDSW ARDSW , BRDSW BRDSW , LL LL , LLN LLN .

Note: Step 3 parameters are extracted from long and medium channel lengths, whereas, Step 4 involves short and medium channel lengths. As in Step 4 'exponential' corrections are particularly pronounced for small L L (short channel). Its Taylor expansion when Leff L_{eff} is medium can give appropriate modifications when power functions alone don't fit very well for medium lengths. Thus, the extracted parameters remain valid for all channel lengths to bring forth the intended length dependence in effect.


Step 5: Refine geometry scaling parameters for mobility degradation parameters.

Extracted Parameters Device and Experimental Data Extraction Methodology
AUA AUA , AUD AUD , ARDSW ARDSW , LL LL Short and medium devices Id I_d vs. Vg V_g @ Vd0.05V V_d \sim 0.05V Observe strong inversion region of all devices in the same plot. Optimize AUA AUA , AUD AUD , ARDSW ARDSW , LL LL .

Step 6: Refine all Group 1 scaling parameters.

Further optimize the parameters by repeating Step 5 and 2. If not getting good fitting, tune LLN LLN , BUA BUA , BUD BUD , BRDSW BRDSW . If still not good, tune other parameters in Group 1 as appropriate. Iteration ends in Step 5 and then proceeds to Step 7. A sample fitting result up till this step is shown in Fig. 17.

Figure 17

Figure 17: Id I_d vs Vg V_g and Gm G_m vs. Vg V_g @ Vd0.05V V_d \sim 0.05V


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