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Highlights • The epitaxial S-K InAs/InP(0 0 1) growth is impacted by As/P exchange process. • Two transitions have been observed in S-K InAs/InP(0 0 1) growth (three regimes). • Three regimes are: 2D layer, large 3D islands, and quantum dots growth. • The truncated pyramidal large 3D islands transform into spherical cap quantum dots. • All experimental transitions are explained through thermodynamic modeling. Abstract Quantum Dots (QDs) are considered as an efficient building block of many optoelectronic applications, such as semiconductor laser, photodetector, whereby their physical dimension is the key parameter to be controlled. In this work, we have studied experimentally the growth of InAs QDs on InP(0 0 1) substrate by MOVPE and established a theoretical model explaining the observed epitaxial behaviour. In variance with the classical Stranski-Krastanov growth, we show that during the growth there is an intermediate stage whereby although first large 3D islands are formed, an increased density of small QDs is formed concurrent with the shrinkage of the large 3D islands. As a result, the growth can be divided into three regimes: 2D layer growth, large 3D islands growth and QDs growth. To explain this evolution, a thermodynamic model has been developed accounting for the process driven by surface energy, elastic relaxation energy and inter-island interaction energy. It will be shown that the balance between the surface energy and the elastic relaxation energy provides the transition from 2D layer to large 3D islands (around at 3 ML of InAs growth). This model also supports the energetically favourable truncated pyramidal shape for large 3D islands and the spherical cap shape for QDs. We show in this paper that a balance between surface energy, elastic relaxation energy and inter-island elastic interaction explains the volume shrinkage of the early large 3D islands towards the formation of small QDs in high density. [ABSTRACT FROM AUTHOR]

Silicon does not emit light efficiently, therefore the integration of other light-emitting materials is highly demanded for silicon photonic integrated circuits. A number of integration approaches have been extensively explored in the past decade. Here, the most recent progress in this field is reviewed, covering the integration approaches of III-V-to-silicon bonding, transfer printing, epitaxial growth and the use of colloidal quantum dots. The basic approaches to create waveguide-coupled on-chip light sources for different application scenarios are discussed, both for silicon and silicon nitride based waveguides. A selection of recent representative device demonstrations is presented, including high speed DFB lasers, ultra-dense comb lasers, short (850nm) and long (2.3μm) wavelength lasers, wide-band LEDs, monolithic O-band lasers and micro-disk lasers operating in the visible. The challenges and opportunities of these approaches are discussed. [ABSTRACT FROM AUTHOR]

• Encapsulation of S-K grown InAs QDs on InP(0 0 1) substrate by InP material. • Preservation of InAs QDs after the InP capping. • InAs QDs dimension shrinkage after InP capping by P/As exchange process. • P incorporation in InAs QDs during InP capping process. • 1550 nm emission with significant increase of carrier lifetime from InP capped InAs QDs. The three-dimensional carrier confinement in Quantum Dots (QDs) is the key to achieve superior properties (electronic and optical) compared to the Quantum Well (QWL) for optoelectronic applications, such as semiconductor lasers, photodiodes. After the growth of QDs, the encapsulation is the next crucial step to confine carriers in QDs and achieve the targeted wavelength emission. In this work, we have studied the InP capping of Stranski-Krastanov (S-K) grown InAs QDs on InP(0 0 1) substrate by MOVPE. During the encapsulation, the P/As exchange is a vital process which either transforms the QDs into a 2D layer or reduces QDs' dimensions. This study shows that a control of Phosphorous concentration on the surface during InP capping facilitates to obtain the expected QDs dimension for 1550 nm wavelength. The emitted photoluminescence peak shifts following the preserved average QDs' dimensions. By combining simulation with optical response we have proved the Phosphorous incorporation into the InAs structure (QDs or 2D layer) during the encapsulation step. As expected, the carrier lifetime reveals the superior quality of the preserved QDs in InP barrier compared to the 2D layer. Finally, the reduction of the non-radiative recombination sources, e.g. dangling bonds, by passivation treatment demonstrates a further increment in carrier lifetime. [ABSTRACT FROM AUTHOR]