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GaAs/AlGaAs Quantum Dot Intermediate-band Solar Cell grown by Droplet Epitaxy

Authors :
Scaccabarozzi, A
Adorno, S
Bietti, S
Acciarri, M
Sanguinetti, S
SCACCABAROZZI, ANDREA
BIETTI, SERGIO
ACCIARRI, MAURIZIO FILIPPO
SANGUINETTI, STEFANO
Scaccabarozzi, A
Adorno, S
Bietti, S
Acciarri, M
Sanguinetti, S
SCACCABAROZZI, ANDREA
BIETTI, SERGIO
ACCIARRI, MAURIZIO FILIPPO
SANGUINETTI, STEFANO
Publication Year :
2013

Abstract

Quantum dot intermediate band (IB) solar cells have been proposed in order to increase the efficiency of traditional solar cells and immediately attracted a lot of attention and research since the time they were first proposed [1]. The IB introduces an extension of the absorption coefficient of the semiconductor to lower energies, allowing a more thorough collection of the solar spectrum, via a two-step absorption of low-energy photons. Quantum dot (QD) structures are good candidates for IB solar cells, because their confined energy levels can overlap and form a miniband in dense arrays and the position of these levels and bands can be tuned varying the size and spacing of the QDs. The IB working mechanisms have been demonstrated for InAs QDs in GaAs [2], and a lot of research is devoted to reduce the problems due to strain, and defect nucleation increasing carrier escape [3]. Droplet epitaxy (DE) [4] is a molecular beam epitaxy technique that allows for the growth of quantum dots of materials lattice matched to the barrier and the removal of the wetting layer. DE makes possible to indipendently control density, size and shape of the nanostructures. Densities as high as some 1011 cm-2 per layer have been reported [5] and potentially a large number of layers can be stacked because the system is strain-free, leading to a much higher density of states in the IB than the more conventional Stranski-Krastanov techniques. Since it is a strain-free technique, there are virtually no defects in DE-grown materials, and this is fundamental to have high performance devices. Moreover, DE nanostructures can be grown without the presence of a wetting layer [6], that would introduce unwanted quantum-well-like states in the system. By tuning the size of the QDs it is obviously possible to change the position of the IB, and by tuning their aspect ratio the high energy states of the QDs can also be tuned in order to have a small electron-phonon coupling with the barrier. The lack of de

Details

Database :
OAIster
Notes :
STAMPA, English
Publication Type :
Electronic Resource
Accession number :
edsoai.on1311390541
Document Type :
Electronic Resource