2021
DOI: 10.1103/physrevb.104.l161303
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Scanning ultrafast electron microscopy reveals photovoltage dynamics at a deeply buried pSi/SiO2 interface

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Cited by 12 publications
(10 citation statements)
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“…In our recent work ( 33 ), we have shown that the material response is well reproduced by modeling the one-dimensional (1D) diffusion of charge carriers near a surface treated as a saturable adsorption boundary condition (details provided in section S10). As such, we can consider surface traps forming a density of photoexcited charge carriers ρ cc ( t , z ) where z is in the vertical direction, to prepare an initial condition ofnormalρccfalse(0,Zfalse)=fhνeαzwhere f , ν, and α are the fluence, frequency of light, and attenuation coefficient, respectively, albeit the exponential term is not applied in these analyses.…”
Section: Resultsmentioning
confidence: 99%
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“…In our recent work ( 33 ), we have shown that the material response is well reproduced by modeling the one-dimensional (1D) diffusion of charge carriers near a surface treated as a saturable adsorption boundary condition (details provided in section S10). As such, we can consider surface traps forming a density of photoexcited charge carriers ρ cc ( t , z ) where z is in the vertical direction, to prepare an initial condition ofnormalρccfalse(0,Zfalse)=fhνeαzwhere f , ν, and α are the fluence, frequency of light, and attenuation coefficient, respectively, albeit the exponential term is not applied in these analyses.…”
Section: Resultsmentioning
confidence: 99%
“…The differences in carrier mobilities and concentrations could thus offset each other and may account for the similarity in timescales of dynamics observed in these studies. Other material properties will also affect these dynamics, most notably surface structure (17,33,(48)(49)(50)(51), which will have effects on other processes such as Fermi-level pinning. Such differences likely account for the observed differences in the contrast mechanisms and the dynamics between various SUEM studies on GaAs (39,40).…”
Section: Discussionmentioning
confidence: 99%
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“…Indeed, taking the peak distance of 81 µm from the edge of the beam radius (30 µm) as the diffusion length and 43 ps as the time, the expected diffusion coefficient for this rapid expansion would be on the order of 6 × 10 5 cm 2 /s. Furthermore, the signal outside of the laser spot is not generated by the pump laser pulse itself, as the fluence 81 µm away in the major axis is 5 × 10 -3 µJ/cm 2 , far below the values required to see any signal at all 36 . The peak distance by itself is three times the size of the laser spot size, suggesting that the charge carriers rapidly spread through ballistic transport of hot carriers or ultrafast diffusion 31,39 .…”
Section: Introductionmentioning
confidence: 93%
“…Despite the 38% increase in counts, the minority carrier concentration only increases by 10 18 cm -3 . There is some discussion on the charge carriers inducing a band-bending effect at the oxide-semiconductor interface which increases the SE emission, but further experiments are required to fully understand the large change in counts 36 .…”
Section: Introductionmentioning
confidence: 99%