The characteristics of TDDB （time-dependent dielectric breakdown） and SILC （stress-induced leakage current） for an ultra-thin SiO2/HfO2 gate dielectric stack are studied. The EOT （equivalent-oxide-thickness） of ...The characteristics of TDDB （time-dependent dielectric breakdown） and SILC （stress-induced leakage current） for an ultra-thin SiO2/HfO2 gate dielectric stack are studied. The EOT （equivalent-oxide-thickness） of the gate stack （Si/SiO2/HfOz/TiN/TiA1/TiN/W） is 0.91 am. The field acceleration factor extracted in TDDB experi- ments is 1.59 s.cm/MV, and the maximum voltage is 1.06 V when the devices operate at 125 ℃ for ten years. A detailed study on the defect generation mechanism induced by SILC is presented to deeply understand the break- down behavior. The trap energy levels can be calculated by the SILC peaks： one S1LC peak is most likely to be caused by the neutral oxygen vacancy in the HfO2 bulk layer at 0.51 eV below the Si conduction band minimum; another SILC peak is induced by the interface traps, which are aligned with the silicon conduction band edge. Fur- thermore, the great difference between the two SILC peaks demonstrates that the degeneration of the high-k layer dominates the breakdown behavior of the extremely thin gate dielectric.展开更多
Positive bias temperature instability（PBTI） characteristics and degradation mechanisms of NMOSFET with high-k/metal gate last process have been systematically investigated. The time evolution of threshold voltage sh...Positive bias temperature instability（PBTI） characteristics and degradation mechanisms of NMOSFET with high-k/metal gate last process have been systematically investigated. The time evolution of threshold voltage shift during PBTI stress still follows a power law. However, the exponent n decreases from 0.26 to 0.16 linearly as the gate stress voltage increases from 0.6 to 1.2 V. There is no interface state generation during stress because of the negligible sub-threshold swing change. Moreover, the activation energy is 0.1 e V, which implies that electrons directly tunnel into high-k bulk and are trapped by pre-existing traps resulting into PBTI degradation. During recovery the threshold voltage shift is linear in lgt, and a mathematical model is proposed to express threshold voltage shift.展开更多
基金Project supported by the Important National Science & Technology Specific Projects(No.2009ZX02035)the National Natural Science of China(No.61306129)the National Found for Fostering Talents of Basic Science(No.J0730318)
文摘The characteristics of TDDB （time-dependent dielectric breakdown） and SILC （stress-induced leakage current） for an ultra-thin SiO2/HfO2 gate dielectric stack are studied. The EOT （equivalent-oxide-thickness） of the gate stack （Si/SiO2/HfOz/TiN/TiA1/TiN/W） is 0.91 am. The field acceleration factor extracted in TDDB experi- ments is 1.59 s.cm/MV, and the maximum voltage is 1.06 V when the devices operate at 125 ℃ for ten years. A detailed study on the defect generation mechanism induced by SILC is presented to deeply understand the break- down behavior. The trap energy levels can be calculated by the SILC peaks： one S1LC peak is most likely to be caused by the neutral oxygen vacancy in the HfO2 bulk layer at 0.51 eV below the Si conduction band minimum; another SILC peak is induced by the interface traps, which are aligned with the silicon conduction band edge. Fur- thermore, the great difference between the two SILC peaks demonstrates that the degeneration of the high-k layer dominates the breakdown behavior of the extremely thin gate dielectric.
基金Project supported by the Important National Science&Technology Specific Projects(No.2009ZX02035)the National Natural Science Foundation of China(Nos.61176091,61306129)
文摘Positive bias temperature instability（PBTI） characteristics and degradation mechanisms of NMOSFET with high-k/metal gate last process have been systematically investigated. The time evolution of threshold voltage shift during PBTI stress still follows a power law. However, the exponent n decreases from 0.26 to 0.16 linearly as the gate stress voltage increases from 0.6 to 1.2 V. There is no interface state generation during stress because of the negligible sub-threshold swing change. Moreover, the activation energy is 0.1 e V, which implies that electrons directly tunnel into high-k bulk and are trapped by pre-existing traps resulting into PBTI degradation. During recovery the threshold voltage shift is linear in lgt, and a mathematical model is proposed to express threshold voltage shift.
