1998
DOI: 10.1134/1.567626
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Self-organization of germanium nanoislands obtained in silicon by molecular-beam epitaxy

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Cited by 34 publications
(6 citation statements)
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“…Room‐temperature photoluminescence (PL) is observed in such structures at wavelengths 1.3–1.6 µm (0.75–0.95 eV). However, due to the spatial separation of holes and electrons in Ge nanoislands, [ 33 ] their radiative recombination efficiency is not high enough for practical applications. There are several approaches for the increase of this efficiency among which may be mentioned a vertical arrangement of nanoislands in a lattice [ 34 ] and ion bombarding of Ge nanoislands.…”
Section: Introductionmentioning
confidence: 99%
“…Room‐temperature photoluminescence (PL) is observed in such structures at wavelengths 1.3–1.6 µm (0.75–0.95 eV). However, due to the spatial separation of holes and electrons in Ge nanoislands, [ 33 ] their radiative recombination efficiency is not high enough for practical applications. There are several approaches for the increase of this efficiency among which may be mentioned a vertical arrangement of nanoislands in a lattice [ 34 ] and ion bombarding of Ge nanoislands.…”
Section: Introductionmentioning
confidence: 99%
“…In the PL spectra measured using the micro-PL setup, the as-grown sample demonstrated relatively weak signals related to Si band edge transitions in the energy range of 1050 ÷ 1150 meV as well as signals related to the different optical transitions in Ge(Si) nanoislands in the energy range of 750 ÷ 950 meV ( Figure 3 a) [ 44 , 45 , 50 ]. The shape of these signals from the as-grown sample is significantly affected by the interference effects caused by multireflection from the buried oxide layer of the SOI substrate.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 5 shows a PL spectrum measured at 4 K. Apart from the Si-related PL lines (all peaks with an energy above 1050 meV and the TO + O phonon-assisted transition at 1028 meV (sharp peak)) due to the Si substrate and capping layer we can identify two PL peaks from the wetting layer (NP WL , a broad peak with a maximum around 1030 meV, and TO WL , an assisted peak at 980 meV) and two PL peaks at lower energies related to GeSi islands (852 and 805 meV). We associate the low energy PL peaks with non-phonon (NP isl ) and phonon assisted (TO isl ) real-space indirect optical transitions between the heavy holes confined in GeSi islands and the electrons located in Si on the heterojunction of the island [18] (see inset in figure 5).…”
Section: Resultsmentioning
confidence: 99%