1973
DOI: 10.1149/1.2403638
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Charge in SiO[sub 2]-Al[sub 2]O[sub 3] Double Layers on Silicon

Abstract: The negative charge in AI-A1203-SiO2-Si double layers was found to be located at the insulator-insulator interface. This charge is independent of the thickness of the A1203 and inversely dependent on the SiO2 thickness. Evidence for a constant voltage drop across the SiO2 during A1203 deposition was found for polycrystalline A1.~O3, N2-deposited and O2-deposited amorphous A1208. It is suggested that the traps at the interface Al~O3-SiO~ are due to oxygen vacancms.Double layer insulators are becoming more and m… Show more

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Cited by 41 publications
(23 citation statements)
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References 9 publications
(15 reference statements)
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“…[13] presence of AI vacancies in the AI203 film. [14] It was shown that these vacancies are predominantly present at the c-Si/A1203 interface, [15] in excellent agreement with the position of the fixed negative charge density deduced from thickness dependent capacitance voltage measurements by for example Abouaf et al [16] A negative Qf is especially beneficial for the passivation of p-type c-Si as the minority carriers, the electrons, are effectively shielded from the c-Si surface. This is clearly apparent from the fact that the negative charge-dielectric AI203 provides a state-of-the-art level of surface passivation even on highly B-doped p-type c Si surfaces as shown in Fig.…”
Section: Introductionsupporting
confidence: 75%
“…[13] presence of AI vacancies in the AI203 film. [14] It was shown that these vacancies are predominantly present at the c-Si/A1203 interface, [15] in excellent agreement with the position of the fixed negative charge density deduced from thickness dependent capacitance voltage measurements by for example Abouaf et al [16] A negative Qf is especially beneficial for the passivation of p-type c-Si as the minority carriers, the electrons, are effectively shielded from the c-Si surface. This is clearly apparent from the fact that the negative charge-dielectric AI203 provides a state-of-the-art level of surface passivation even on highly B-doped p-type c Si surfaces as shown in Fig.…”
Section: Introductionsupporting
confidence: 75%
“…The latter can also be directly appreciated from the stack with a 30 nm interlayer. Therefore, in addition to the relation given in (3), an alternative, more complex model can be introduced which accounts for a positive charge contribution Q pos at the Si/SiO 2 interface and a negative charge contribution Q neg at the SiO 2 /Al 2 O 3 interface: 49,51 …”
Section: Capacitance-voltage Measurementsmentioning
confidence: 99%
“…Values reported in the literature by Saito et al 41 for the effective charge density in Si/SiO 2 /Al 2 O 3 stacks with dry thermal oxide interlayers in the thickness range 0.7-2 nm are between À2 Â 10 13 and À5 Â 10 12 cm À2 , respectively. Aboaf et al 42 obtained values of $3 Â 10 11 cm À2 for plasma oxidized interlayers in Si/SiO 2 /Al 2 O 3 stacks with a SiO 2 thickness in the range of 23-100 nm. Compared to our data these values from the literature agree very well for both SiO 2 thickness ranges, especially, considering the fact that the interlayers have been prepared using different deposition methods.…”
Section: B Determination Of the Absolute Charge Density In The Stacksmentioning
confidence: 99%