1986
DOI: 10.1103/physrevb.33.2574
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Charge transfer, polarization, and relaxation effects on the Auger line shapes of Si

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Cited by 79 publications
(21 citation statements)
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“…During this Ga uptake, we also monitored the shape of the Si LVV peak. Ramekar et al and Shivaprasad et al [18,19] have shown that the asymmetry in the Si LVV Auger peak on the surface is due to the 2p electron, which comprises the dangling bond component. We extract this information by measuring the upper and lower excursions in the (dN/dE) spectra which directly corresponds to the p-p electron state contribution (Lpp) and the s-s and s-p state contributions (Lss), respectively.…”
Section: Resultsmentioning
confidence: 97%
“…During this Ga uptake, we also monitored the shape of the Si LVV peak. Ramekar et al and Shivaprasad et al [18,19] have shown that the asymmetry in the Si LVV Auger peak on the surface is due to the 2p electron, which comprises the dangling bond component. We extract this information by measuring the upper and lower excursions in the (dN/dE) spectra which directly corresponds to the p-p electron state contribution (Lpp) and the s-s and s-p state contributions (Lss), respectively.…”
Section: Resultsmentioning
confidence: 97%
“…The deconvolution of the Si (LVV) auger peak in the N(E) mode, enables the extraction of the contribution of the p-electron states to the Auger transition. 23 The density of the dangling bonds (valence bad states), which are predominantly p-in character, can thus be monitored by observing changes in the intensity of the corresponding components. This becomes easily accessible in the Auger spectra acquired in the first derivative mode, since the upper excursion of the peak corresponds directly to the p-p electron state contribution (L pp ), and the lower excursion is due to the s-s and s-p states (L ss ).…”
Section: Adsorptionmentioning
confidence: 99%
“…31 This is due to a quantum interference between the direct Si 2p photoexcitation to the continuum and the KLV Auger emission after excitation of a 1s core hole at the K edge. However, the Si KLV Auger decay is calculated to occur at only 2% for the rate of the KLL Auger decay, 32 making it a very small effect. Also, the width of the Fano interference, taking into account the unfilled bandwidth of the Si conduction band and the lifetimes of the core states, should not extend as far as our point of measurement at 6 eV above the Si K edge.…”
Section: Experimental Test Of Atomic Scattering Factorsmentioning
confidence: 99%