Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs.

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Development of an analytical Development of an analytical mobility model for the mobility model for the simulation of ultra thin SOI simulation of ultra thin SOI MOSFETs. MOSFETs. M.Alessandrini, M.Alessandrini, * * D.Esseni, C.Fiegna D.Esseni, C.Fiegna Department of Engineering - University of Ferrara, Department of Engineering - University of Ferrara, Italy Italy * * DEGM, University of Udine, Italy DEGM, University of Udine, Italy

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Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs. M.Alessandrini, * D.Esseni, C.Fiegna Department of Engineering - University of Ferrara, Italy * DEGM, University of Udine, Italy. - PowerPoint PPT Presentation

Transcript of Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs.

Page 1: Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs.

Development of an analytical mobility Development of an analytical mobility model for the simulation of ultra thin SOI model for the simulation of ultra thin SOI

MOSFETs.MOSFETs.

M.Alessandrini, M.Alessandrini, **D.Esseni, C.FiegnaD.Esseni, C.FiegnaDepartment of Engineering - University of Ferrara, ItalyDepartment of Engineering - University of Ferrara, Italy

**DEGM, University of Udine, ItalyDEGM, University of Udine, Italy

Page 2: Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs.

IntroductionIntroductionThe scaling of the conventional bulk CMOS technology requires high doping concentration to counteract short channel effects (SCE).

ProblemProblem: the increase of doping concentration leads to a significant degradation of the low field mobility (black curves in figure):

SOI devices with SOI devices with almost undoped ultra-almost undoped ultra-thin silicon layer thin silicon layer represent a possible represent a possible solution for mobility solution for mobility degradationdegradation

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Dependence of effective mobility on TsiDependence of effective mobility on TsiRecent works reported a dependence of effective mobility in SOI MOSFETs on the thickness of the silicon layer (TSI ) which is particularly evident at low inversion densities

Conventional mobility models overestimate experimentalmobility and are not able to qualitatively reproduce the dependence of mobility on Tsi

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This workThis work

In this work we developed analytical models for electron mobility limited by two scattering processes that lead to the mobility modulation by TSI in SOI MOSFETs:

● Surface optical phonos scatteringSurface optical phonos scattering

● Coulomb scattering with interface statesCoulomb scattering with interface states

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Scattering with surface optical Scattering with surface optical phononsphonons

The model for mobility limited by surface optical phonons has been developed starting from the general formulation of M. Fischetti and S.Laux (''Monte Carlo study of electron transport in silicon inversion layers'' Phys.Rev. B Vol 48, 1993)* under the following approximations:

● single parabolic umprimed subband,● one constant effective value for the exchanged wave vector with no angular dependence (qe ).

Under these approximations we obtained the following scattering rate:Under these approximations we obtained the following scattering rate:

* This formulation has been used in D. Esseni et al. ''Study of low field electron transport in ultra-thin single and double gate SOI MOSFETs'' IEDM 2002

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Scattering with surface optical Scattering with surface optical phononsphonons

● The wave function is approximated as follow*:

● We empirically relate the parameter b to the effective field Eeff as follows:

*According to F.Stern and W. Howard ''Properties of Semiconductor Sueface Inversion Layer in the Electric Quantum Limit'' Phis.Rev. Vol.163 1997

Fitting parameter

Normalized concentration: n(z)/Ninv

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Determination of the parameter Determination of the parameter ..We determined the value of the parameter We determined the value of the parameter by comparing the calculated g(z) with by comparing the calculated g(z) with the normalized charge density obtained from Schroedinger-Poisson calculations:the normalized charge density obtained from Schroedinger-Poisson calculations:

Bulk MOSFETBulk MOSFET

SOI MOSFET SOI MOSFET (TSI=5.2 nm)(TSI=5.2 nm)

Schroedinger Poisson simulationsg(z) approximation

Schroedinger Poisson simulationsg(z) approximation

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Scattering rate for the case of two Si-SiO2 interfaces:

Scattering with surface optical Scattering with surface optical phononsphonons

Mobility in the relaxation-time approximation:

Page 9: Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs.

Scattering with surface optical Scattering with surface optical phononsphonons

Parameter values used in this model:

The effective exchanged wave vector is obtained by fitting the results of rigorous numerical calculation :D.Esseni et al. ''Study of low field electron transport in ultra-thin single and double gate SOI MOSFETs'' IEDM 2002

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Simulation Results : Simulation Results : fitting of rigorous numerical calculationfitting of rigorous numerical calculation

Numerical model Numerical model

Analytical model applied to electric field obtained Analytical model applied to electric field obtained by Schrodinger/Poisson calculationby Schrodinger/Poisson calculation

Scattering with surface optical Scattering with surface optical phononsphonons

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Scattering with surface optical Scattering with surface optical phononsphonons

Calculation of total effective mobilityCalculation of total effective mobility● We performed a drift diffusion simulation of long MOSFETs using a mobility model for bulk MOSFETs and accounting for quantization by the density gradient model.● We evaluated the mobility limited by SO phonons scattering by post- processing the electric-field distribution with equation:

• We calculated the total electron mobility composing, by the Mathiessen rule, the mobility evaluated at discretization points within the inversion layer with mobility limited by SO phonons scattering. • The effective mobility in the inversion layer is then obtained as an average weigthed by carrier concentration according to:

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Effective mobility in ultra-thin SOI SG MOSFETs including surface optical phonons scattering (symbols) and experimental data for low-doped Bulk MOSFETs (line) (qualitative agreement with Koga et al. IEEE TED June 2002).

Scattering with surface optical Scattering with surface optical phononsphonons

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Simulation Results: effective mobility versus Eeff for bulk structures

Scattering with surface optical Scattering with surface optical phononsphonons

Simulations including the effects of SO phonons

Experimental data

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Coulomb scattering with interface statesCoulomb scattering with interface states

Following the same procedure we described for SO phonons scattering, we obtained the following scattering rate with unscreened interface charge:

Where Mf and Mb are the same used for SO phononsscattering and

Areal density ofinterface states

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Coulomb scattering with interface statesCoulomb scattering with interface states

ScreeningScreening

The screening by inversion carrier is accounted for by a modified :

Where is the Debye length.

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Coulomb scattering with interface statesCoulomb scattering with interface states

Left: experimental mobility versus NinvRight: simulations including SO phonons scattering and interface states scattering.

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Conclusions Conclusions

●In this work, analytical models for the mobility limited by surface optical phonons and by interface states has been developed and applied to the calculation of electron effective mobility in MOSFETs. ●The proposed models can be adopted in conjunction with conventional mobility models developed for bulk devices, and allow to reproduce the main feature of recently-reported mobility data for ultra-thin SOI MOSFETs. ●The model for SO-phonons-limited mobility has been recently implemented in DESSIS using the physical-model software interface.