1989
DOI: 10.1103/physrevb.39.5287
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Shallow positron traps in GaAs

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Cited by 143 publications
(62 citation statements)
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“…31 The concentration of impurities is low in our MBE-grown layers whereas Ga As antisites are not expected with the strongly As-rich stoichiometry of LT-GaAs. In a recent theoretical study, Landman et al 55 found a low formation energy for a split As interstitial which could, therefore, be an abundant defect in the strongly As-rich LTGaAs.…”
Section: ϫmentioning
confidence: 69%
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“…31 The concentration of impurities is low in our MBE-grown layers whereas Ga As antisites are not expected with the strongly As-rich stoichiometry of LT-GaAs. In a recent theoretical study, Landman et al 55 found a low formation energy for a split As interstitial which could, therefore, be an abundant defect in the strongly As-rich LTGaAs.…”
Section: ϫmentioning
confidence: 69%
“…The annihilation parameters for such defects are close to the bulk values but they can trap positrons only at low temperatures (TϽ150 K͒ in their shallow potential. 31 The presence of such defects would be detected as a strong decrease of S towards S b with decreasing temperature. This is not found.…”
Section: Revealing Neutral Ga Vacancy Complexes By Temperature-depmentioning
confidence: 99%
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“…The temperature dependence of positron trapping can determine the charge state of vacancy-related defects 8 and can also provide evidence on the presence of acceptor point defects without open volume such as substitutional impurities. 9 The lifetime of the localized positron state is sensitive to the size of the open volume, and the chemical nature of the near neighbor atoms dominates the electron momentum distribution sampled by the positron in the high momentum region. These can be measured using positron annihilation lifetime spectroscopy (PALS) and coincidence Doppler broadening spectroscopy (CDBS), respectively, and the results from both can be compared to DFT calculations.…”
mentioning
confidence: 99%
“…15,16 This temperature dependence provides clear evidence for trapping to defects with a small binding energy for positrons, and the associated positron states exhibit a lifetime similar to the bulk, perfect lattice, lifetime value, s B . 9,15 The fit to the STM for one vacancy defect (s v ¼ 330 ps) with one shallow binding energy trap (s st ¼ s B ¼ 285 ps), 15 both negatively charged, is shown in Fig. 1.…”
mentioning
confidence: 99%