AVS 63rd International Symposium & Exhibition | |
Electronic Materials and Photonics | Thursday Sessions |
Session EM-ThP |
Session: | EMPD Poster Session |
Presenter: | Lauren Peckler, University of Arizona |
Authors: | L. Peckler, University of Arizona S.L. Heslop, University of Arizona A.J. Muscat, University of Arizona |
Correspondent: | Click to Email |
SiGex is a potential semiconductor for next generation transistors because it could be incorporated into current, silicon-based semiconductor manufacturing processes and it would improve transistor performance due to the high carrier mobility of Ge. Despite these advantages, one major challenge is to reduce the number of Ge defects at the SiGe/dielectric interface because they degrade electrical performance of the transistor. While a relatively stable SiO2 layer can be grown on Si with relatively few defects, the same is not true for Ge. One approach to forming a high quality interface is to remove Ge oxides by passivating the Ge atoms on the surface. SiGe and Ge metal oxide semiconductor capacitors (MOSCaps) were fabricated (10 nm Al2O3) and tested to evaluate the effect of sulfur-based chemical passivation on electrical performance. The (100) faces of three SiGex substrates – x = 0.25, 0.5, 0.75 – and one Ge substrate were cleaned and treated with one of two ammonium sulfide, (NH4)2S, wet chemistries: (NH4)2S/H2O (1:100 v/v) or (NH4)2S/HCl/HF/H2O (1:0.15:0.15:100 v/v). The surfaces of control MOSCaps were cleaned only. The contact area on each device was 12.6 µm2.
Average capacitance in accumulation for SiGex MOSCaps (x = 0.25, 0.5) was 199 ± 5.4 and 205 ± 22 pF, with a DC bias sweep from -2 to +2 V at 1 MHz. The same capacitance was 42 ± 1.3 pF for SiGex (x = 0.75) and 457 ± 12 pF for the Ge MOSCaps. Both (NH4)2S treatments increased the accumulation capacitance by 6% and 34%, on average, for SiGex (x = 0.25, 0.5), 8% for SiGex (x = 0.75), and 8% for Ge MOSCaps. Similarly, VFB shifted -2 V (SiGex (x = 0.25, 0.5)) and -.14 V (SiGex (x = 0.75) and Ge) with respect to the controls. While flatband shifting is at least due to reduction of oxide defects in the Al2O3 layer, the low magnitude of accumulation capacitance (according to oxide thickness calculations) suggests that there are other oxide layers present.
Half of the SiGex MOSCaps (x = 0.25, 0.75) were annealed in forming gas. VFB shifted +3 V for SiGex MOSCaps (x = 0.25) with respect to non-annealed results, which is indicative of a reduction in negatively charged bulk oxide defects . SiGex (x = 0.75), and Ge MOSCaps possibly had less bulk oxide defects because their VFB were within ± 0.5 V before and after annealing. Less bulk oxide defects in these MOSCaps suggest that nucleation and growth of the Al2O3 layer on these surfaces may differ from that of the SiGex (x = 0.25) surface. Among all three SiGex (x = 0.25) MOSCaps, the one treated with (NH4)2S and acid and annealed resulted in the flatband voltage closest to 0 V, as well as the lowest capacitance.