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David Esseni ESSDERC 2002 1
An Improved Model for Electron Mobility Degradation by Remote Coulomb Scattering in
Ultra-Thin SOI MOSFETs
David Esseni and Antonio Abramo
DIEGM – University of Udine
David Esseni ESSDERC 2002 2
Motivations• Limits to Gate Oxide Scaling in terms of
Reliability and/or Leakage Current• Effect of oxide thickness and Polysilicon
Proximity on Electron Transport• Experimental Reduction of On-Current
for TOX < 1.3nm [Timp-IEDM ’98]• Previous papers on RCS use Simplified
Models Large µrcs Underestimate
David Esseni ESSDERC 2002 3
Purpose of the Work• Numerical Calculation of RCS:
– Wave functions of the 2D Electron Gas– CS Potential induced by a point charge
including Screening in Poly and Substrate– Momentum Relaxation Time (MRT)
• Discuss Importance of Poly Screening and Multi-Subband Transport
• Dependence of µeff on TOX and NPOLY
David Esseni ESSDERC 2002 4
Outline• Numerical Evaluation of µRCS
– The Screened CS Potential– Momentum Relaxation Time (MRT)
• Results for RCS Limited Mobility
• Total µeff in Ultra-Thin Oxide MOSFETs
• Conclusions
David Esseni ESSDERC 2002 5
Determine φ(q,z,z0): z0: Charge Positionq: Spacial Freq. Vectorz: Normal to Interfaceξi: i-th Subband Eigenf.
Non-Local Screening [Stern - 1967]
David Esseni ESSDERC 2002 6
φ(q,z,z0) in Poly/Oxide/Substrate Stack
Boundary Conditions for φ and (dφ/dz)give the unknown constants A1 .. A4
David Esseni ESSDERC 2002 7
Calculation of the CS Potential φ(q,z,z0)
• Poly Screening strongly reduces φ(q,z,z0)• QM Depletion Region [Spinelli-TED ’00]
David Esseni ESSDERC 2002 8
Outline• Numerical Evaluation of µRCS
– The Screened CS Potential
– Momentum Relaxation Time (MRT)
• Results for RCS Limited Mobility
• Total µeff in Ultra-Thin Oxide MOSFETs
• Conclusions
David Esseni ESSDERC 2002 9
Scattering Matrix Elements:
Momentum Relaxation Time:
Inter-Subband Transitions Couple MRTs Calculation !!
David Esseni ESSDERC 2002 10
Momentum Relaxation Time:
Isotropic Bands: τi(E) DOES NOT depend on the angle βi
Set of Non-Linear Algebraic Equations:
David Esseni ESSDERC 2002 11
CS Momentum Relaxation Time
• Inter-Subband Transitions do affect MRTs• Subband Mobility is finally obtained from
the average MRT in the Subband
David Esseni ESSDERC 2002 12
Outline
• Numerical Evaluation of µRCS– The Screened CS Potential
– Momentum Relaxation Time (MRT)
• Results for RCS Limited Mobility
• Total µeff in Ultra-Thin Oxide MOSFETs
• Conclusions
David Esseni ESSDERC 2002 13
RCS Mobility: Effect of Poly Screening
• Large µRCS Underest. w/o Poly Screen.
• CL Poly gives much Larger µRCS
David Esseni ESSDERC 2002 14
RCS Mobility: Multi Subband Transport
• CS Potential decays in the substrate so lowest Subbands have largest Coupling
• µRCS is much Larger than in QL Approx.
David Esseni ESSDERC 2002 15
Outline• Numerical Evaluation of µRCS
– The Screened CS Potential
– Momentum Relaxation Time (MRT)
• Results for RCS Limited Mobility
• Total µeff in Ultra-Thin Oxide MOSFETs
• Conclusions
David Esseni ESSDERC 2002 16
Mobility of Thick Oxide MOSFETs
• Phonons [Jungemann - SSE 1993] and Surface Roughness [Ando - 1982]
• DAC and Roughness adjusted for Nsub=2x1016
David Esseni ESSDERC 2002 17
Mobility of Thin Oxide MOSFETs
• ~20% Reduction for TOX=1.2nm at Ninv~1012
• Larger Reductions with Simplified Models
David Esseni ESSDERC 2002 18
• At Ninv=1013 Mobility is Independent of TOX• ~7% Reduction for TOX=3nm at Ninv~1012
• Simplified Models: µeff Degradation for TOX>5nmcontrary to Data [Liang-TED 1986]
Mobility vs. Oxide Thickness
David Esseni ESSDERC 2002 19
Mobility vs. Polysilicon Doping Concentration
• Increased Density of CS Centers and Poly Screening result in Weak Npoly Dependence
David Esseni ESSDERC 2002 20
Conclusions• Numerical Model for µRCS:
– Polysilicon and Substrate Screening– MRTs Including Inter-Subband Transitions
• Large Underestimates w/o Poly Screening
• QL Approximation NOT Applicable• RCS Effects for TOX<3nm at Low Ninv
• Approach suitable for RCS due to Oxide Charges in High-K Dielectrics
David Esseni ESSDERC 2002 21
Temperature Dependence
• Low Temperatures Confine Electrons in the Lowest Subband and Decrease µRCS
David Esseni ESSDERC 2002 22
Alternative High-K Dielectrics
• For a given Teq High-K Improves µRCS
• For a given TOX High-K Reduces µRCS