1970
DOI: 10.1109/irps.1970.362425
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A Review of Instability Mechanisms in Passivation Films

Abstract: Over the past ten years a number of single and double-layer insulator structures have been studied for passivation of semiconductor device surfaces. This paper reviews the various charge instability mechanisms associated with these structures. These include ionic drift, polarization, slow electronic trapping, and double-layer effects. The known dependence of these effects on processing and material parameters is discussed and the current state-of-the-art for controlling these instabilities is reviewed.

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Cited by 16 publications
(13 citation statements)
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“…The presence of charged ions in thin oxide films was first reported in the mid and late 1960s when Bell Labs, Fairchild and IBM engaged in the study of thermal silicon dioxide (SiO2) for the production of field-effect transistors (FET) [1]. The work of Snow et al [2][3][4] showed that the ionic conductivity in thin SiO2 films, as also reported by Yamin [5][6][7] and Kerr [8][9][10], was largely due to the presence of sodium and potassium ions. Moreover, they showed that these ions were responsible for the instability problems leading to failure in Metal-Oxide-Semiconductor field effect transistors (MOSFETs), as also thoroughly studied by Hofstein [11][12][13].…”
Section: Introductionmentioning
confidence: 93%
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“…The presence of charged ions in thin oxide films was first reported in the mid and late 1960s when Bell Labs, Fairchild and IBM engaged in the study of thermal silicon dioxide (SiO2) for the production of field-effect transistors (FET) [1]. The work of Snow et al [2][3][4] showed that the ionic conductivity in thin SiO2 films, as also reported by Yamin [5][6][7] and Kerr [8][9][10], was largely due to the presence of sodium and potassium ions. Moreover, they showed that these ions were responsible for the instability problems leading to failure in Metal-Oxide-Semiconductor field effect transistors (MOSFETs), as also thoroughly studied by Hofstein [11][12][13].…”
Section: Introductionmentioning
confidence: 93%
“…However, the initial distribution of energy of the trapped ions at an interface should be known [39]. Approximations to this distribution have been used by assuming a single activation energy [39], a Gaussian distribution of traps as a function energy [8,46], or even a convolution of Dirac functions and the measured current density [47]. Choquet and Balland [48] published an elegant algorithm to calculate the initial ion distribution yet some discrepancies were found in their calculation, thus there still exists uncertainty in determining the initial concentration and energy distribution of trapped ions.…”
Section: Introductionmentioning
confidence: 99%
“…In either case, the hoped-for outcome is the formation of a semiconducting phase having a low concentration of electronic states in its bandgap. Such a phase is desirable because it inhibits the rate of corrosion even when the driving force is large. …”
Section: Introductionmentioning
confidence: 99%
“…The distribution of activation energies has previously been approximated most typically using either single energy values, 48 or Gaussian distributions. 32,[49][50][51] In this work a single activation energy is used for simplicity. Ions are thermally excited over the injection barrier during a high temperature anneal.…”
mentioning
confidence: 99%