2021
DOI: 10.1109/led.2021.3066624
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Observation of Hydrogen-Related Defect in Subgap Density of States and Its Effects Under Positive Bias Stress in Amorphous InGaZnO TFT

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Cited by 22 publications
(14 citation statements)
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“…First, based on previous work, the subgap DOS of a-ZBTO was incorporated into the simulation framework . The DOS model used is formulated as follows: , g ( E ) = g TD ( E ) + g DD ( E ) + g DA ( E ) + g TA ( E ) = N TD × exp ( E E V k T TD ) + N DD × exp ( ( E C E DD E k T DD ) 2 ) + N DA 0.25em × exp ( ( E C E DA E k T DA ) 2 ) +…”
Section: Resultsmentioning
confidence: 99%
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“…First, based on previous work, the subgap DOS of a-ZBTO was incorporated into the simulation framework . The DOS model used is formulated as follows: , g ( E ) = g TD ( E ) + g DD ( E ) + g DA ( E ) + g TA ( E ) = N TD × exp ( E E V k T TD ) + N DD × exp ( ( E C E DD E k T DD ) 2 ) + N DA 0.25em × exp ( ( E C E DA E k T DA ) 2 ) +…”
Section: Resultsmentioning
confidence: 99%
“…First, based on previous work, the subgap DOS of a-ZBTO was incorporated into the simulation framework . The DOS model used is formulated as follows: , where the total DOS g ( E ) consists of g TD (donor-like tail states), g DD (donor-like deep states), g DA (acceptor-like deep states), and g TA (acceptor-like tail states); N TD and N TA are the intercept densities at E V and E C , respectively; kT TD and kT TA are the characteristic energies of the exponential tail states near E V and E C , respectively; kT DD and kT DA are the characteristic energies of the Gaussian deep states near E V and E C , respectively; E DD and E DA are the center energies of the Gaussian DOS peak near E V and E C , respectively; and N DD and N DA are the densities at the central energies E DD and E DA , respectively, of the Gaussian distribution.…”
Section: Resultsmentioning
confidence: 99%
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“…Given that V o H acts as the major electron donor, the IGZO channel usually becomes heavily n-doped after atomic-layerdeposition (ALD)-based ferroelectric top-gated (TG) dielectric deposition since the ALD deposition chamber is typically hydrogen abundant [27], [28]. Although different postdeposition annealing (PDA) treatments for defects passivation or channel carrier concentration modulation for IGZO-based devices have been widely studied [29], [30], [31], the high sensitivity and complexity of the channel interface/bulk defects formation as a function of different process ambients (e.g., H 2 , N 2 , or O 2 ) render the PDA effects unreliable.…”
Section: Introductionmentioning
confidence: 99%
“…Density functional theory-based calculations have indicated a possible shallow donor state near (< 0.6 eV) from the conduction band minimum 22 and enhanced state density in hydrogen-rich devices has been reported to be observed in the range 0.2 − 0.6 eV from the conduction band minimum. 12,32 However, hydrogen incorporation in a-IGZO has also been repeatedly correlated with an increased response from states in the near valence band region of the subgap, 9,11,17,23,28,33 which at least one author 33 has suggested could be linked to OH −interaction.…”
Section: Introductionmentioning
confidence: 99%