Comparative Study of Plasma Source-Dependent Charging Polarity in Metal–Oxide–Semiconductor Field Effect Transistors with High-k and SiO2 Gate Dielectrics

The polarities of charging damage in n- and p-channel metal–oxide–semiconductor field effect transistors (MOSFETs) with Hf-based high-k gate stack (HfAlOx/SiO2) were studied for two different plasma sources (Ar- and Cl-based gas mixtures) and found to depend on plasma conditions, in contrast to those with conventional SiO2. It was also found that high-k devices were more susceptible to plasma charging damage than SiO2 devices. For Ar-plasma, which was confirmed to induce a larger charging damage, both n- and p-channel MOSFETs with high-k gate stacks suffer from negative charge trapping, whereas for Cl-plasma confirmed to induce less damage, both n- and p-channel MOSFETs with high-k gate stacks suffer from positive charge trapping. The above-mentioned plasma-source-dependent charging damage was also compared on the basis of the results obtained by the plasma diagnostics. From the results of constant-current stress tests, the unique charging polarity observed for the high-k gate stack was attributed to the characteristic hole and electron trapping phenomena, in accordance with the injected stress current and stress time, implying the necessity of taking the intrinsic charge trapping process into consideration for accurate evaluations of charging damage on high-k gate dielectrics.

[1]  T. Kanashima,et al.  Photoreflectance characterization of the plasma-induced damage in Si substrate , 2000 .

[2]  K. Noguchi,et al.  Modeling oxide thickness dependence of charging damage by plasma processing , 1993, IEEE Electron Device Letters.

[3]  John G. Simmons,et al.  Poole-Frenkel Effect and Schottky Effect in Metal-Insulator-Metal Systems , 1967 .

[4]  S. Samukawa,et al.  Reduction of ultraviolet-radiation damage in SiO2 using pulse-time-modulated plasma and its application to charge coupled 44 device image sensor processes , 2003 .

[5]  Ih-Chin Chen,et al.  Electrical breakdown in thin gate and tunneling oxides , 1985 .

[6]  Koji Eriguchi,et al.  Correlation between two time-dependent dielectric breakdown measurements for the gate oxides damaged by plasma processing , 1998 .

[7]  Masaharu Oshima,et al.  Surface Damage on Si Substrates Caused by Reactive Sputter Etching , 1981 .

[8]  Kin P. Cheung,et al.  Plasma Charging Damage , 2000 .

[9]  G. Bersuker,et al.  Charge trapping and detrapping characteristics in hafnium silicate gate dielectric using an inversion pulse measurement technique , 2005 .

[10]  Koji Eriguchi,et al.  Temperature and stress polarity-dependent dielectric breakdown in ultrathin gate oxides , 1998 .

[11]  Plasma charging damage on MOS devices with gate insulator of high-dielectric constant material , 2001 .

[12]  W. Greene,et al.  Magnetron etching of polysilicon: Electrical damage , 1991 .

[13]  M. V. Malyshev,et al.  Diagnostics of inductively coupled chlorine plasmas: Measurement of electron and total positive ion densities , 2001 .

[14]  Takashi Yunogami,et al.  Radiation damage in SiO2/Si induced by low‐energy electrons via plasmon excitation , 1993 .

[15]  J. McPherson,et al.  Thermochemical description of dielectric breakdown in high dielectric constant materials , 2003 .

[16]  K. Cheung,et al.  Plasma‐charging damage: A physical model , 1994 .

[17]  R. Franklin Electronegative plasmas—why are they so different? , 2002 .

[18]  Koji Eriguchi,et al.  Quantitative Evaluation of Gate Oxide Damage during Plasma Processing Using Antenna-Structure Capacitors , 1994 .

[19]  S. Zafar Statistical mechanics based model for negative bias temperature instability induced degradation , 2005 .

[20]  Koichi Hashimoto,et al.  Charge Damage Caused by Electron Shading Effect , 1994 .

[21]  C. Hu,et al.  Dependence of plasma-induced oxide charging current on Al antenna geometry , 1992, IEEE Electron Device Letters.