2016
DOI: 10.1103/physrevb.94.115434
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Excitonic fine structure and binding energies of excitonic complexes in single InAs quantum dashes

Abstract: The fundamental electronic and optical properties of elongated InAs nanostructures embedded in quaternary InGaAlAs barrier are investigated by means of high-resolution optical spectroscopy and many-body atomistic tight-binding theory. These wire-like shaped self-assembled nanostructures are known as quantum dashes and are typically formed during the molecular beam epitaxial growth on InP substrates. In this work we study properties of excitonic complexes confined in quantum dashes emitting in a broad spectral … Show more

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Cited by 22 publications
(29 citation statements)
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“…These dimensions are typical for self-assembled quantum dots and quantum dashes. 21 In our previous work 54 we have studied effects of nanostructure size and composition on quantum dashes spectra, here focus on the role of lateral deformation for pure InAs/InP system. The anisotropy is applied as by elongating the system along [110] axis and shrinking it in the perpendicular [110] axis at the same time, such that the base field (and the overall dot volume) is kept constant.…”
Section: A System and Methodsmentioning
confidence: 99%
“…These dimensions are typical for self-assembled quantum dots and quantum dashes. 21 In our previous work 54 we have studied effects of nanostructure size and composition on quantum dashes spectra, here focus on the role of lateral deformation for pure InAs/InP system. The anisotropy is applied as by elongating the system along [110] axis and shrinking it in the perpendicular [110] axis at the same time, such that the base field (and the overall dot volume) is kept constant.…”
Section: A System and Methodsmentioning
confidence: 99%
“…1(a), we present normalized (to maximum intensities) µPL spectra from a single QDash within the 500 × 250 nm 2 mesa recorded at 5 K and 75 K. The spectral line marked with an arrow is the one identified as originating from the negatively charged exciton (X − ), based on the characteristic linear excitation-power dependence of intensity and no fine-structure splitting as shown in previous studies. 26,29,30 A common redshift of the luminescence peaks with temperature is present due to the thermal shrinkage of the material band-gap. At T = 5 K the considered peak has a Gaussian profile with the linewidth of ∼0.2 meV, which indicates an inhomogeneous impact of the environment.…”
mentioning
confidence: 99%
“…In addition, we cannot neglect the influence of the excess carriers on entire kinetics which has evidently been the case for the excitation power dependence in the cwexcitation as shown elsewhere [18].…”
Section: P Mrowiński Et Almentioning
confidence: 99%
“…Based on that, the bright-dark states splitting is equal to 440 µeV, the binding energies of biexciton and trion are -3.1 meV and -5.6 meV, respectively. Strongly bound state of the charged exciton suggests this is the negatively charged trion [16][17][18], which could be expected for nanostructures deposited on InP substrate being unintentionally n-doped with substantial concentration of the excess electrons. Typically, as for small quantum dots, one would expect that the XX D PL line has significantly lower intensity than X D one due to the spin relaxation from bright to dark exciton which populates the X D states.…”
Section: Introductionmentioning
confidence: 99%