Plasma-assisted atomic layer deposition (ALD) was used to deposit SiO 2 films in the temperature range of T dep = 50-400 • C on Si(100). H 2 Si[N(C 2 H 5 ) 2 ] 2 and an O 2 plasma were used as Si precursor and oxidant, respectively. The ALD growth process and material properties were characterized in detail. Ultrashort precursor doses (∼50 ms) were found to be sufficient to reach self-limiting ALD growth with a growth-per-cycle of ∼1.2 Å (T dep = ∼200 • C) leading to SiO 2 films with O/Si ratio of ∼2.1. Moreover, the plasma ALD process led to a high conformality (95-100%) for trenches with aspect ratios of ∼30. In addition, the electronic (interface) properties of ultrathin ALD SiO 2 films and ALD SiO 2 /Al 2 O 3 stacks were studied by capacitance-voltage and photoconductance decay measurements. The interface quality associated with SiO 2 was improved significantly by using an ultrathin ALD Al 2 O 3 capping layer and annealing. The interface defect densities decreased from ∼1×10 12 eV −1 cm −2 (at mid gap) for single layer SiO 2 to < 10 11 eV −1 cm −2 for the stacks. Correspondingly, ultralow surface recombination velocities < 3 cm/s were obtained for n-type Si. The density and polarity of the fixed charges associated with the stacks were found to be critically dependent on the SiO 2 thickness (1-30 nm).
Differences in Si surface passivation by aluminum oxide ͑Al 2 O 3 ͒ films synthesized using H 2 O and O 3-based thermal atomic layer deposition ͑ALD͒ and plasma ALD have been revealed. A low interface defect density of D it = ϳ 10 11 eV −1 cm −2 was obtained after annealing, independent of the oxidant. This low D it was found to be vital for the passivation performance. Field-effect passivation was less prominent for H 2 O-based ALD Al 2 O 3 before and after annealing, whereas for as-deposited ALD films with an O 2 plasma or O 3 as the oxidants, the field-effect passivation was impaired by a very high D it .
Articles you may be interested inDetailed leakage current analysis of metal-insulator-metal capacitors with ZrO2, ZrO2/SiO2/ZrO2, and ZrO2/Al2O3/ZrO2 as dielectric and TiN electrodes J. Vac. Sci. Technol. B 31, 01A109 (2013); 10.1116/1.4768791 Impact of bottom electrode and Sr x Ti y O z film formation on physical and electrical properties of metalinsulator-metal capacitors Appl. Phys. Lett. 98, 182902 (2011); 10.1063/1.3584022 Influence of precursor chemistry and growth temperature on the electrical properties of SrTiO 3 -based metalinsulator-metal capacitors grown by atomic layer deposition J. Vac. Sci. Technol. B 29, 01AC04 (2011); 10.1116/1.3525280 Impact of crystallization behavior of Sr x Ti y O z films on electrical properties of metal-insulator-metal capacitors with TiN electrodes Appl. Phys. Lett. 97, 162906 (2010); 10.1063/1.3505323 Atomic-layer-deposited Al 2 O 3 -Hf O 2 -Al 2 O 3 dielectrics for metal-insulator-metal capacitor applications Appl. Phys. Lett.In this work, the physical and electrical properties of Sr x Ti 1−x O y ͑STO͒-based metal-insulator-metal capacitors ͑MIMcaps͒ with various compositions are studied in detail. While most recent studies on STO were done on noblelike metal electrodes ͑Ru, Pt͒, this work focuses on a low temperature ͑250°C͒ atomic layer deposition ͑ALD͒ process, using an alternative precursor set and carefully optimized processing conditions, enabling the use of low-cost, manufacturable-friendly TiN electrodes. Physical analyses show that the film crystallization temperature, its texture and morphology strongly depends on the Sr/Ti ratio. Such physical variations have a direct impact on the electric properties of Sr x Ti 1−x O y based capacitors. It is found that Sr-enrichment result in a monotonous decrease in the dielectric constant and leakage current as predicted by ab initio calculations. The intercept of the EOT vs physical thickness plot further indicates that increasing the Sr-content at the film interface with the bottom TiN would result in lower interfacial equivalent-oxide thickness.
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