Study of the Interface Roughness Models using 3D Finite Element Schrödinger Equation Corrected Monte Carlo Simulator on Nanoscaled FinFET

By Daniel Nagy1; Muhammad Ali A. Elmessary1; Manuel Aldegunde2; Karol Kalna1

1. College of Engineering, Swansea University, Swansea, Wales, UK 2. School of Engineering, University of Warwick, Coventry, England, UK

Published on

Abstract

IWCE 2015 presentation.  Interface roughness scattering (IRS) is one of the key limiting scattering mechanism for both planar and non-planar CMOS devices. To predict the performance of future scaled devices and new structures the quantum mechanical confinement based IRS models are essential. In this work, the in-house 3D finite element Monte Carlo code with 2D Schrodinger equation based quantum correction serves as a base for implementation of a new multi-subband extended Prange & Nee (EPN) IRS model and for comparison with the previously used 3D Ando model. The transistors selected for the comparison are 10.7 nm gate length SOI Si FinFETs with two cross-sections: rectangular and triangular. The drive current for the rectangular device has been reduced by 25% when using the multi-subband EPN model and even more reduced for the triangular shape, by 44%, at VD = 0.7 V.

Credits

In collaboration with J. Lindberg,  A. Loureiro, College of Engineering, Swansea University, Swansea, Wales, UK, Universidade de Santiago de Compostela, Galicia, Spain

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Cite this work

Researchers should cite this work as follows:

  • Nagy, D, "Multi-subband interface roughness scattering using 2D finite element schodinger equation for monte carlo simulations of multi-gate transistors," in Computational Electronics (IWCE) 2015 International Workshop on, DOI: 10.1109/IWCE.2015.7301977

  • Daniel Nagy, Muhammad Ali A. Elmessary, Manuel Aldegunde, Karol Kalna (2016), "Study of the Interface Roughness Models using 3D Finite Element Schrödinger Equation Corrected Monte Carlo Simulator on Nanoscaled FinFET," https://nanohub.org/resources/23299.

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Time

Location

North Ballroom, PMU, Purdue University, West Lafayette, IN

Tags

Study of the Interface Roughness Models using 3D Finite Element Schrödinger Equation Corrected Monte Carlo Simulator on Nanoscaled FinFET
  • Study of the Interface Roughness Models using 3D Finite Element Schrodinger Equation Corrected Monte Carlo Simulator on Nanoscaled FinFET D. Nagy1, M. A. Elmessary1,3, M. Aldegunde1, J. Lindberg2, A. Loureiro4, and K. Kalna1 1. Study of the Interface Roughne… 0
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  • What I am going to talk about... 2. What I am going to talk about.… 17.217217217217218
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  • Scattering limits CMOS performance 3. Scattering limits CMOS perform… 53.520186853520187
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  • Investigated FinFET devices Perimeter = 35.8 nm Area = 87 nm2 4. Investigated FinFET devices Pe… 135.23523523523525
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  • Which model? Ando1 5. Which model? Ando1 180.01334668001334
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  • Overview of the simulation toolbox 6. Overview of the simulation too… 252.15215215215216
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  • Extract data for EPN 7. Extract data for EPN 332.1654988321655
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  • Step-by-step 8. Step-by-step 366.29963296629967
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  • Change in scattering rate 9. Change in scattering rate 417.81781781781785
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  • Larger limiting effect of EPN mode 10. Larger limiting effect of EPN … 453.18651985318655
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  • Scattering at different energies Γaver(E) = Ractangualr @ VD = 0.05 V 10 0 EPN VG = 0 10 × 10 0 2.0 11. Scattering at different energi… 534.76810143476814
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  • Difference in real space VD = 0.7 V and VG = 0.9 V 12. Difference in real space VD = … 587.38738738738743
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  • Volume inversion VD = 0.7 V and VG = 0.9 V 13. Volume inversion VD = 0.7 V an… 614.11411411411416
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  • The point is... Successful implementation of the multi-subband EPN model EPN IRS is stronger than 3D Ando at large electron kinetic energy (from above 0.06 eV) and above VG = 0.4 V In case of EPN mode the drive current is reduced as: 14. The point is... Successful imp… 640.90757424090759
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  • New Bay Campus! 15. New Bay Campus! 691.22455789122455
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