2014
DOI: 10.1016/j.matlet.2013.10.077
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Band offsets of La2O3 films on Ge substrates grown by radio frequency magnetron sputtering

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Cited by 13 publications
(11 citation statements)
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“…On the other hand, the sharp breakdown observed on the higher electric field is considered as hard breakdown, E 2 where the increase of instantaneous leakage current density is larger. Figure 7 elucidates the Ge 3d spectra of different oxidation/nitridation durations (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20) minutes. Ge 3d spectra comprise two broad peaks which incorporate Ge 0 and a mixture of various chemical bonding states of distinctive Ge sub-oxides.…”
Section: J-e Characteristicsmentioning
confidence: 99%
“…On the other hand, the sharp breakdown observed on the higher electric field is considered as hard breakdown, E 2 where the increase of instantaneous leakage current density is larger. Figure 7 elucidates the Ge 3d spectra of different oxidation/nitridation durations (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20) minutes. Ge 3d spectra comprise two broad peaks which incorporate Ge 0 and a mixture of various chemical bonding states of distinctive Ge sub-oxides.…”
Section: J-e Characteristicsmentioning
confidence: 99%
“…As we know, the bandgap equals the energy distance between the photoemission peak centroid and the onset of the features due to single particle excitations, and it is usually obtained from the inelastic energy loss features observed on the high binding energy side of the core level photoemission peaks [30]. The onset of O 1s loss spectrum was determined by linearly extrapolating the segment of maximum negative slope to the back ground level [31]. The bandgaps of the as-grown 10 and 20 nm La 2 O 3 films are determined to be 5.55 and 5.45 eV, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…In principle, the photoexcited electrons passing through dielectric films can suffer inelastic losses due to plasmon (collective oscillation) and single particle excitation (band-to-band transition excitation) [23]. It is proved that the band gap equals the energy distance between the photoemission peak centroid and the onset of the features due to single particle excitations, and it is usually obtained from the inelastic energy loss features observed on the high binding energy side of the core level photoemission peaks [24]. Besides, the onset of the O 1 s loss spectrum can be determined by linearly extrapolating the segment of maximum negative slope to the background level [25,26].…”
Section: Resultsmentioning
confidence: 99%