We measure, in real units, the radiative and total current density in high performance 1.3-μm InAs quantum-dot-laser structures. Despite very low threshold current densities, significant nonradiative recombination (∼80% of the total recombination) occurs at 300 K with an increasing fraction at higher current density and higher temperature. Two nonradiative processes are identified; the first increases approximately linearly with the radiative recombination while the second increases at a faster rate and is associated with the loss of carriers to either excited dot states or the wetting layer
It has been found that Auger recombination is very important in 1.3 μm quantum dot (QD) lasers at ro...
Carrier processes in InAs–GaAs self-assembled quantum dot lasers are investigated via the measuremen...
Unlike InAs/GaAs quantum dot lasers, in 1.55μm InAs/InP devices, non-radiative recombination dominat...
We measure, in real units, the radiative and total current density in high performance 1.3-μm InAs q...
We show that even in quantum dot lasers with very low threshold current density (Jth=740-50 A/cm(2) ...
The temperature dependence of the radiative and nonradiative components of the threshold current den...
We show that even in quantum-dot (QD) lasers with very low threshold current densities (J(th) = 40-5...
The radiative and nonradiative components of the threshold current in 1.3 mu m, p-doped and undoped ...
The drive for low threshold and temperature-stable semiconductor lasers for telecommunication applic...
International audienceThe threshold current and its radiative component in 1.5 µm InAs/InP (311)B qu...
The optical matrix element for excited-states is significantly weaker than the ground-state leading ...
The threshold current and its radiative component in 1.5 mu m InAs/InP (311)B quantum dot lasers are...
Gain saturation increases the radiative component, J(rad), of the threshold current density, J(th), ...
InAs quantum-dot (QD) lasers were investigated in the temperature range 20-300 K and under hydrostat...
We have calculated radiative and Auger recombination rates due to localized recombination in individ...
It has been found that Auger recombination is very important in 1.3 μm quantum dot (QD) lasers at ro...
Carrier processes in InAs–GaAs self-assembled quantum dot lasers are investigated via the measuremen...
Unlike InAs/GaAs quantum dot lasers, in 1.55μm InAs/InP devices, non-radiative recombination dominat...
We measure, in real units, the radiative and total current density in high performance 1.3-μm InAs q...
We show that even in quantum dot lasers with very low threshold current density (Jth=740-50 A/cm(2) ...
The temperature dependence of the radiative and nonradiative components of the threshold current den...
We show that even in quantum-dot (QD) lasers with very low threshold current densities (J(th) = 40-5...
The radiative and nonradiative components of the threshold current in 1.3 mu m, p-doped and undoped ...
The drive for low threshold and temperature-stable semiconductor lasers for telecommunication applic...
International audienceThe threshold current and its radiative component in 1.5 µm InAs/InP (311)B qu...
The optical matrix element for excited-states is significantly weaker than the ground-state leading ...
The threshold current and its radiative component in 1.5 mu m InAs/InP (311)B quantum dot lasers are...
Gain saturation increases the radiative component, J(rad), of the threshold current density, J(th), ...
InAs quantum-dot (QD) lasers were investigated in the temperature range 20-300 K and under hydrostat...
We have calculated radiative and Auger recombination rates due to localized recombination in individ...
It has been found that Auger recombination is very important in 1.3 μm quantum dot (QD) lasers at ro...
Carrier processes in InAs–GaAs self-assembled quantum dot lasers are investigated via the measuremen...
Unlike InAs/GaAs quantum dot lasers, in 1.55μm InAs/InP devices, non-radiative recombination dominat...