3.15.6 Fringe Capacitances and Capacitance Model Selectors
The fringing capacitance consists of a bias-independent outer fringing capacitance and a bias-dependent inner fringing capacitance. Only the bias-independent outer fringing capacitance is modeled.
BSIM-CMG offers 3 models for the outer fringe capacitance, selected by CGEOMOD:
For CGEOMOD=0, the fringe and overlap capacitances are proportional to the number of fins and the effective width. The fringe capacitances is given by:
Cgs,fr=NFINtotal⋅Weff,CV0⋅CFSi(3.486)
Cgd,fr=NFINtotal⋅Weff,CV0⋅CFDi(3.487)
Figure 7 illustrates the parasitic resistance and capacitance network used for CGEOMOD=0.

Figure 7: R-C network for CGEOMOD=0, NQSMOD=1, and RGATEMOD=1. If NQSMOD or RGATEMOD is 0, then the corresponding resistances become 0 and the nodes collapse.
In some multi-gate applications the parasitic capacitances are not directly proportional to the width of the device. BSIM-CMG offers CGEOMOD=1 so that the fringe and overlap capacitance values can be directly specified without assuming any width dependencies. The simple expressions for fringe and overlap capacitances in CGEOMOD=1 are:
Cgs,ov=COVSi(3.488)
Cgd,ov=COVDi(3.489)
Cgs,fr=CGSP(3.490)
Cgd,fr=CGDP(3.491)
Note: The switch CGEO1SW can be used to enable the parameters COVS, COVD, CGSP, and CGDP to be in F per fin, per gate-finger, per unit channel width.
The parasitic resistance and capacitance network for CGEOMOD=1 is illustrated in Fig. 8.

Figure 8: R-C network for CGEOMOD=1, NQSMOD=1, and RGATEMOD=1. If NQSMOD or RGATEMOD is 0, then the corresponding resistances become 0 and the nodes collapse.
If CGEOMOD=2, an outer fringe capacitance model for variability modeling which address the complex dependencies on the FinFET geometry will be invoked. RGEOMOD=1 and CGEOMOD=2 share the same set of input parameters and can be used at the same time. Both models are derived based on the FinFET structure (single-fin or multi-fin with merged source/drain).
In CGEOMOD=2 the fringe capacitance is partitioned into a top component, a corner component and a side component (Fig. 9). The top and side components are calculated based on a 2-D fringe capacitance model, which has been derived and calibrated to numerical simulation in [14]. The corner component is calculated based on the formula of parallel plate capacitors.
Cfr,top=Cfringe,2D(Hg,Hrsd,LRSD)×TFIN×NFIN(3.492)
Cfr,side=2×Cfringe,2D(Wg,Trsd,LRSD)×HFIN×NFIN(3.493)
Ccorner=LSPϵsp⋅[Acorner×NFIN+ARSDEND+ASILIEND](3.494)
where
Hg=TGATE+TMASK(3.495)
Trsd=21(FPITCH−TFIN)(3.496)
Wg=Trsd−TOXP(3.497)
Hrsd=HEPI+TSILI(3.498)
ARSDEND and ASILIEND are the additional area of silicon and silicide, respectively, at the two ends of a multi-fin FinFET.
The three components are summed up to give the total fringe capacitance. Several fitting parameters are added to aid fitting. The final expression is:
Cfr,geo=(Ccorner+Cfr,top+CGEOE⋅Cfr,side)×NF×[CGEOA+CGEOB⋅TFIN+CGEOC⋅FPITCH+CGEOD⋅LRSD]
(3.499)

Figure 9: Illustration of top, corner and side components of the outer fringe capacitance.
For the case of TMASK>0 the fringe capacitances are calculated a little differently, since the 2D model is valid only for a thin Tox. Ccorner is set to 0. Cfr,top is proportional to FPITCH and is given by
Cfr,top=[3.467×10−11⋅ln(3.9⋅LSPEPSRSP⋅10−7)+0.942⋅Hrsd⋅LSPϵsp]×[TFIN+(FPITCH−TFIN)⋅CRATIO]⋅NFIN
(3.500)
The RC network has the same topology as CGEOMOD=0.
And finally,
Cds,fr=CDSP
for all CGEOMOD.
References
[14] W.-M. Lin, F. Li, D. D. Lu, A. M. Niknejad, and C. Hu, "A Compact Fringe Capacitance Model for FinFETs," unpublished.