Lasers based on self-assembled quantum dots (QDs) emitting at 1.3 µm are commercially available, but producing longer wavelength devices has proven challenging. In both cases strain-engineered InAs/InxGa1-xAs/GaAs metamorphic structures are exploited, with the InGaAs layers above and below the QDs called upper and lower confining layers (CLs).The emission wavelength may be controlled by changing two independent parameters of the relaxed InxGa1-xAs lower CL [1]. (1) Changing x the amount of In in the CLs,. This changes results in modifications of the band discontinuities between the QDs and CLs and also affects the QD-CL mismatch f, that determines the QD strain. (2) Changing the lower CL thickness, d, only affects f [1]. By this method it should be possible to optimize the confinement of exciton whilst also extending the wavelength to 1.55 µm: emission as long as 1.59 µm in similar metamorphic nanostructures has been reported [2]. Measuring the emission wavelength is straightforward, but how about the confinement? Here we do this by studying exciton properties (Bohr radius, aB and reduced mass, µ) using low temperature magneto-photoluminescence [3].
Confinement of Excitons in Strain-engineered InAs/InGaAs/GaAs Metamorphic Quantum Dots
Luca Seravalli;Giovanna Trevisi;Paola Frigeri
2013
Abstract
Lasers based on self-assembled quantum dots (QDs) emitting at 1.3 µm are commercially available, but producing longer wavelength devices has proven challenging. In both cases strain-engineered InAs/InxGa1-xAs/GaAs metamorphic structures are exploited, with the InGaAs layers above and below the QDs called upper and lower confining layers (CLs).The emission wavelength may be controlled by changing two independent parameters of the relaxed InxGa1-xAs lower CL [1]. (1) Changing x the amount of In in the CLs,. This changes results in modifications of the band discontinuities between the QDs and CLs and also affects the QD-CL mismatch f, that determines the QD strain. (2) Changing the lower CL thickness, d, only affects f [1]. By this method it should be possible to optimize the confinement of exciton whilst also extending the wavelength to 1.55 µm: emission as long as 1.59 µm in similar metamorphic nanostructures has been reported [2]. Measuring the emission wavelength is straightforward, but how about the confinement? Here we do this by studying exciton properties (Bohr radius, aB and reduced mass, µ) using low temperature magneto-photoluminescence [3].I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.