2016
DOI: 10.12693/aphyspola.129.a-66
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Type-I and Type-II Confinement in Quantum Dots: Excitonic Fine Structure

Abstract: We have theoretically studied type-I and type-II confinement in InAs quantum dots with GaAs1−ySby capping layer. The character of the confinement can be adjusted by the Sb content. We have found that upon the transition from type-I to type-II confinement the hole wave functions change the topology from a compact shape to a twosegment shape, resulting in the complex changes in the exciton fine structure splitting with zero values at particular compositions. Additionally, a high exciton radiative recombination p… Show more

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Cited by 4 publications
(4 citation statements)
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“…We further note that considerably smaller FSS for type II corroborates with the results of Refs. [81,82,84] for (In,Ga)As/Ga(As,Sb)/GaAs QDs and, in turn, confirms that to be a rather general property of dots which are type-II in real space. The correlation is obtained in our CI calculations through admixing of excited single-particle states [69].…”
Section: γ-Excitonssupporting
confidence: 65%
See 1 more Smart Citation
“…We further note that considerably smaller FSS for type II corroborates with the results of Refs. [81,82,84] for (In,Ga)As/Ga(As,Sb)/GaAs QDs and, in turn, confirms that to be a rather general property of dots which are type-II in real space. The correlation is obtained in our CI calculations through admixing of excited single-particle states [69].…”
Section: γ-Excitonssupporting
confidence: 65%
“…We now proceed with the fine structure of X 0 . That is caused in (In,Ga)As/GaAs QDs [63,81,82] by the effects of isotropic and anisotropic exchange interaction, which is the case also for the present system. The former causes the energy separation of bright and dark X 0 (∆E bd ) while the latter results in FSS of X 0 .…”
Section: γ-Excitonssupporting
confidence: 62%
“…Namely, those are (i) the exchange Coulomb interaction between ground state electron and hole wavefunction (marked as '2 × 2' in figure 3), (ii) the multipole expansion of exchange interaction [75] (marked as '2 × 2 multipole' in figure 3), and (iii) the effect of Coulomb correlation [71,79] (marked as '12 × 12' in figure 3). Clearly, the dominant contribution to both FSS and BD in CdSe/ZnS QDs comes from the multipole expansion of the exchange interaction, similarly as in references [75,80] for III-V QDs. We further note, that the dominant contribution comes from the dipole-dipole term of that expansion for CdSe QDs.…”
Section: Figurementioning
confidence: 71%
“…We computed the fine structure employing three levels of approximation in CI, i.e., (i) without considering the effect of correlation and with monopole-monopole term of the exchange interaction only, (ii) with correlation and monopole-monopole term of exchange, and (iii) without correlation but with assuming the monopolemonopole, monopole-dipole, and dipole-dipole terms of the exchange interaction what we call multipole expan-sion. [54,64] The results for FSS of X 0 are given in Fig. 3 (a) by full curves along with experimental data from Fig.…”
Section: Theorymentioning
confidence: 99%