1993
DOI: 10.1109/16.210209
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Correlation of stress-induced leakage current in thin oxides with trap generation inside the oxides

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Cited by 223 publications
(85 citation statements)
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“…Early investigators of SILC in stressed oxides observed a transient component in the leakage current, that was attributed to charging and discharging of oxide traps [210][211][212][213][214] and was exploited to extract information on the oxide quality [215,216]. The detrapping current followed a 1/t dependence down to very short times [217], in agreement with tunneling models [218].…”
Section: Charge Detrappingsupporting
confidence: 52%
“…Early investigators of SILC in stressed oxides observed a transient component in the leakage current, that was attributed to charging and discharging of oxide traps [210][211][212][213][214] and was exploited to extract information on the oxide quality [215,216]. The detrapping current followed a 1/t dependence down to very short times [217], in agreement with tunneling models [218].…”
Section: Charge Detrappingsupporting
confidence: 52%
“…In a different study by Ramprasad,27 simultaneous contributions from multiple transport mechanisms was modeled for metal-insulator-metal capacitor systems, and both J-t and J-V (J is the current density) characteristics were predicted. The phenomenological theory used parameters typical for TaOx capacitors and oxide thickness of several hundred angstroms.…”
Section: -2?mentioning
confidence: 99%
“…18,19 The affected dielectrics were typically highquality thermal oxides with very low trap densities, 20,21 however, the SILC effect has also been observed in PECVD oxides. 22 The physical mechanism of the transient SILC effect has been modeled as the charging and discharging of border traps located within a few nm of metal-dielectric interfaces.…”
mentioning
confidence: 99%
“…21 Given that our devices are not exposed to such high field stresses ( 3 MV/cm) and that repeated measurements on MIM and MEMS devices have shown little change in the power-law exponent with charging bias, polarity, or temperature, we conclude that no new traps are generated in the oxide and that the transient current behavior and changes in pull-in voltage are due to the charging and discharging of existing border traps located close to the bottom metal dielectric interface. The charging and discharging of the border traps have been explained by both elastic 18,19 and inelastic tunneling processes. 21,26 According to the elastic tunneling front model 27 and assuming a uniform spatial distribution of traps, the trapped charge is assumed to be initially adjacent to the metal-dielectric interface and moving into the dielectric at the rate of approximately 0.2-0.4 nm per decade of time.…”
mentioning
confidence: 99%
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