1974
DOI: 10.1116/1.1318719
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Tunneling in thin MOS structures

Abstract: Recent results on tunneling in thin MOS structures are described. Thermally grown SiO2 films in the thickness range of 22–40 Å have been shown to be effectively uniform on an atomic scale and exhibit an extremely abrupt oxide-silicon interface. Resonant reflections are observed at this interface for Fowler-Nordheim tunneling and are shown to agree with the exact theory for a trapezoidal barrier. Tunneling at lower fields is consistent with elastic tunneling into the silicon direct conduction band and, at still… Show more

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Cited by 213 publications
(48 citation statements)
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“…An I-V hysteresis loop was found, which is due to the charge accumulation or trapping in the device [100]. At these very low voltages, the current is due to the (inelastic) tunneling into the Si-nc/SiO 2 interface states [102]. The presence of the subbandgap interface states has been reported recently by us [103].…”
Section: Si-nc Based Light Emittersmentioning
confidence: 76%
“…An I-V hysteresis loop was found, which is due to the charge accumulation or trapping in the device [100]. At these very low voltages, the current is due to the (inelastic) tunneling into the Si-nc/SiO 2 interface states [102]. The presence of the subbandgap interface states has been reported recently by us [103].…”
Section: Si-nc Based Light Emittersmentioning
confidence: 76%
“…If the oxide thickness is greater than 50 nm, having some trapped charge inside it, it can be governed by PooleFrenkel conduction model. On the other hand, current conduction for the ultrathin oxide layers less than 5 nm, has been termed as direct tunnelling [8]. Figure 3 shows the current-voltage characteristics across MOSiC structure for different gate oxide thicknesses starting from 23.7 nm to 61.4 nm.…”
Section: Resultsmentioning
confidence: 99%
“…The mechanisms for DC conductivity at low and high electric fields in amorphous as well as crystalline materials have been discussed in the literature. Four main mechanisms have been proposed for the observed behaviour: direct tunnelling (DT), Schottky emission (SE), Fowler-Nordheim (FN) tunnelling and Poole-Frenkel (P-F) conduction, depending upon the magnitude of oxide thickness, defect at the interface and polarity of the applied gate voltage [6][7][8]. P-F conduction mechanism is most often observed in amorphous materials, particularly dielectrics, because of the relatively large number of defect centres present in the energy gap.…”
Section: Introductionmentioning
confidence: 99%
“…The linear portion of this plot for E B between about 2.5 and 4.1 eV is in accord with the Franz twoband model of Refs. [32] and [33], and applies when the conduction band states are free electron-like with predominantly s*-character. The projected values for m eff when E B are attributed to a change in the character of the lowest conduction band states, from s*-extended states in SiO 2 and Si 3 N 4 , to significantly more localized d*-states in the TM and RE dielectrics.…”
Section: Conduction Band Offset Energies and Tunnelingmentioning
confidence: 99%