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Total Dose Response of HfO 2 /Dy 2 O 3 on Ge and Hf 0.6 Si 0.2 ON 0.2 on Si MOS Capacitors

Total Dose Response of HfO 2 /Dy 2 O 3 on Ge and Hf 0.6 Si 0.2 ON 0.2 on Si MOS Capacitors. D. K. Chen, R. D. Schrimpf, D. M. Fleetwood, K. F. Galloway, A. Canals Department of Electrical Engineering and Computer Science, S. T. Pantelides, Department of Physics

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Total Dose Response of HfO 2 /Dy 2 O 3 on Ge and Hf 0.6 Si 0.2 ON 0.2 on Si MOS Capacitors

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  1. Total Dose Response of HfO2/Dy2O3 on Ge and Hf0.6Si0.2ON0.2 on Si MOS Capacitors D. K. Chen, R. D. Schrimpf, D. M. Fleetwood, K. F. Galloway, A. Canals Department of Electrical Engineering and Computer Science, S. T. Pantelides, Department of Physics Vanderbilt University, Nashville, TN G. Lucovsky, S. Lee Dept of Physics and Material Science, North Carolina State University Bongim Jun Dept of Electrical Engineering, Georgia Institute of Technology A. Dimoulas, A. Sotiropoulos, and Y. Panayiotatos Institute of Materials Science, NCSR DEMOKRITOS Athens, Greece 2006 MURI Review

  2. Motivation • Limitations of ultrathin SiO2 gate dielectric microelectronic devices: high gate leakage current, reduced current drive, and reliability concerns • Leakage current unmanageable for tox less than ~ 1.2 nm • Germanium MOS devices • Higher electron and hole mobility leads to higher drive current • Unstable native oxide • Dysprosium oxide on Ge • HfO2 (K~25) and HfxSiyONz (K~15) 1.2 nm 1.9 nm M.L. Green, JAP 2001 (90) 5 2006 MURI Review

  3. Outline • HfO2/Dy2O3 • No measurable change in C-V characteristics after TID • Large hysteresis and leakage current • Hf0.6Si0.2ON0.2 • Significant electron trapping after TID • Conclusions and future plans 2006 MURI Review

  4. HfO2/Dy2O3 on Ge Eg ~ 5.7 eV (HfO2) 2006 MURI Review

  5. C-V Characteristics EOT= 1.9 nm EOT= 1.1 nm • Hysteresis ~ 800 mV for 10 nm HfO2, ~ 150 mV for 5 nm HfO2. • No measurable change in C-V characteristics after total dose irradiation to 30 Mrad(SiO2) for 10 nm HfO2 and 10 Mrad(SiO2) for 5 nm HfO2 • Equal electron and hole trapping in HfO2 and/or large leakage currents neutralize radiation-induced oxide traps 2006 MURI Review

  6. Gate Current Densities EOT= 1.1 nm EOT= 1.9 nm • Leakage current density @ 1 MV/cm: 30 nA/cm2 (EOT=1.9nm) and 35 nA/cm2 (EOT=1.1nm) • Large leakage current reflects the interface quality of dysprosium oxide/germanium 2006 MURI Review

  7. Outline • HfO2/Dy2O3 • No measurable change in C-V characteristics after TID • Large hysteresis and leakage current • Hf0.6Si0.2ON0.2 • Significant electron trapping after TID • Conclusions • Future plan 2006 MURI Review

  8. 2.4 eV 7.2 eV 3.7 eV HfxSiyONz Si Hf0.6Si0.2ON0.2 on Si 2006 MURI Review

  9. C-V Characteristics • Hysteresis ~ 15 mV • Jg ~ 2 nA/cm2 @ VG = 0.4 V 2006 MURI Review

  10. Charge trapping in Hf0.6Si0.2ON0.2 on Si G. Pant, APL 2006 (88) 032901 • Correlation between crystallization and ∆VTH • Trap density increases with crystallization • Crystallization increases with increasing thickness • Dit ~ 2 x 1011 cm-2 eV-1 pre-irradiation • ∆NOT = 6.27 x 1012 cm2 after 500 krad • Predominantly electron traps 2006 MURI Review

  11. Plan for future experiments • Obtain new HfO2/Dy2O3 films of various thicknesses – check hysteresis, leakage, rad response • Determine the structure and composition of the Hf0.6Si0.2ON0.2 films – irradiate under negative and zero bias to obtain additional trapping information • Perform Bias Temperature Instability (BTI) tests to further investigate properties of Hf0.6Si0.2ON0.2 films 2006 MURI Review

  12. Conclusions • HfO2/Dy2O3 on Ge • Gate leakage current and/or equal electron hole charge trapping cause neutralization of radiation-induced oxide trap charges • High border trap densities reflect the physical nature of interface of HfO2/Dy2O3 and Ge • Future work will concentrate on films with low leakage and hysteresis • Hf0.6Si0.2ON0.2 on Si • Low hysteresis • Significant electron trapping due to film composition 2006 MURI Review

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