2018
DOI: 10.1016/j.mssp.2017.11.024
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Temperature-dependent Fowler-Nordheim electron barrier height in SiO2/4H-SiC MOS capacitors

Abstract: This paper reports on the physical and temperature dependent electrical characterizations of the oxide/semiconductor interface in MOS capacitors with a SiO2 layer deposited on 4H-SiC using dichlorosilane and nitrogen-based vapor precursors. The capacitors, subjected to a standard post deposition annealing process in N2O, exhibited an interface state density Dit ≈ 9.0×10 11 cm -2 eV -1 below the conduction band edge. At room temperature, a barrier height (conduction band offset) of 2.8 eV was observed, along wi… Show more

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Cited by 31 publications
(13 citation statements)
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“…The higher valence band offset and the lateral confinement of the TD produces the creation of a quantum well. Considering the ideal conduction contribution -i.e., the ideal Fowler-Nordheim (FN) tunnelling [24] and the quantum confinement that inhibits the FN tunnelling from the bottom of the quantum well [25] -the oxide electric field produces a minor increase of the hole current through the insulator layer. Besides the calculated increase of the electric field due to the TD band gap narrowing, also the surface morphology plays a role [26].…”
Section: Resultsmentioning
confidence: 99%
“…The higher valence band offset and the lateral confinement of the TD produces the creation of a quantum well. Considering the ideal conduction contribution -i.e., the ideal Fowler-Nordheim (FN) tunnelling [24] and the quantum confinement that inhibits the FN tunnelling from the bottom of the quantum well [25] -the oxide electric field produces a minor increase of the hole current through the insulator layer. Besides the calculated increase of the electric field due to the TD band gap narrowing, also the surface morphology plays a role [26].…”
Section: Resultsmentioning
confidence: 99%
“…with where ϕ t is the electron emission barrier height from the trap states, ε AlN is the relative dielectric permittivity of the gate insulator at high frequency ( ε AlN 4.77 [ 49 ]), ε 0 is the permittivity of free space, and C is a constant. The validity of the PF emission fitting was verified by checking the temperature dependence of the linear coefficient m ( T ) obtained from the lineal fit of the PF plots ln( J / E ) as a function of E 1/2 [ 50 ], which is shown in Fig. 10 .…”
Section: Resultsmentioning
confidence: 99%
“…Figure 7 shows the comparison between the conductivity profile on the as deposited (black line) and N2O annealed (blue line) samples, determined using the SSRM. Fabrication details can be found in Reference [55]. As can be seen, the number of free carriers in the nitridated sample is increased by more than one order of magnitude in a region about 10 nm wide from the SiO2/4H-SiC interface [47,51].…”
Section: Effects Of Counter Doping and Interface Stressmentioning
confidence: 98%