Abstract:Here comes a report on the optical properties of InP based InAs columnar quantum dashes, which are proposed as an alternative for columnar quantum dots in semiconductor optical amplifiers construction since they offer convenient spectral tuning over 1.55μm together with a very broad and high gain. Electronic structure details are investigated by photoreflectance and photoluminescence and analyzed by comparison with effective mass calculations. Columnar quantum dash emission from the cleaved edge is examined by… Show more
“…The PL emission is TE dominated in this low energy part of the spectrum that originates from the "true" ͑i.e., three dimensionally confined͒ CQDash states. 13 This is due to the fact, that for this orientation the polarization is determined by the elongated extension of the CQDashes, 13 which is much larger than the vertical dimensions ͑about 300 nm length compared to ϳ10 nm height͒.…”
mentioning
confidence: 99%
“…Due to the reduced CQDash gain in this geometry the lasing wavelength is significantly blueshifted to 1550 nm ͑see Fig. 2͒, which thus constitutes lasing of the quantum well such as immersion layer 13 with the polarization of the laser emission being also TE in this case.…”
mentioning
confidence: 99%
“…This spectral part is almost unpolarized as it is dominated by transitions of the more quantum well-like states of the slightly tensile strained immersion layer. 13 So the reason why lasing does not start in TM polarization on the CQDash states is because the gain of the immersion layer is slightly higher than the gain of the CQDashes for this orientation. Nevertheless, the polarization of the CQDash emission itself was changed from TE to TM dominated by changing the geometrical orientation of the dashes.…”
“…The PL emission is TE dominated in this low energy part of the spectrum that originates from the "true" ͑i.e., three dimensionally confined͒ CQDash states. 13 This is due to the fact, that for this orientation the polarization is determined by the elongated extension of the CQDashes, 13 which is much larger than the vertical dimensions ͑about 300 nm length compared to ϳ10 nm height͒.…”
mentioning
confidence: 99%
“…Due to the reduced CQDash gain in this geometry the lasing wavelength is significantly blueshifted to 1550 nm ͑see Fig. 2͒, which thus constitutes lasing of the quantum well such as immersion layer 13 with the polarization of the laser emission being also TE in this case.…”
mentioning
confidence: 99%
“…This spectral part is almost unpolarized as it is dominated by transitions of the more quantum well-like states of the slightly tensile strained immersion layer. 13 So the reason why lasing does not start in TM polarization on the CQDash states is because the gain of the immersion layer is slightly higher than the gain of the CQDashes for this orientation. Nevertheless, the polarization of the CQDash emission itself was changed from TE to TM dominated by changing the geometrical orientation of the dashes.…”
“…The active region consists of four sheets of 5 monolayer InAs dashes, each embedded within a 7.6 nm thick compressively strained In 0.64 Ga 0.16 Al 0.2 As quantum well [8] with a thickness of 50 nm of tensile strained In 0.50 Ga 0.32 Al 0.18 As barrier. The Q-dash structures have an average height of 3.2 nm, average width of 18 nm, and length varied from 20 to hundreds of nm.…”
Section: Optical Properties Of Q-dash Materialsmentioning
confidence: 99%
“…Among the variety of such materials the quantum dashes (strongly elongated quantum dots) are of growing interest now due to perspectives in optoelectronic applications, especially in telecommunication lasers operating at 1.55 mm and longer wavelengths [7][8][9]. Size distribution of quantum dash (Q-dash) structures results in a broad gain profile and wide tunable emission (from 1.5 to 2 mm) [7].…”
The self assembly of quantum dots by heteroepitaxy of lattice‐mismatched semiconductors is based on elastic energy relaxation, which spontaneously occurs at the growth front when the largest atoms in the crystal cluster together. Because a larger covalent radius is related to weaker bonds, and this is in turn fundamentally related to smaller bandgaps, the formation of quantum dots leads to a confinement potential for electrons and/or holes. This effect has applications ranging from ultralow threshold diode lasers to highly efficient solar cells and usually requires the stacking of multiple quantum dots. The number of layers is limited by the stress accumulated during growth due to the larger covalent radius of the atoms that constitute the quantum dots. This accumulated stress can be relieved by introducing in the epitaxial layers compensating atomic species with a smaller covalent radius, enabling a reduction of spacer layer thickness. In the limit of sub‐nanometer spacer thickness, the quantum dots, which have a tendency to line up vertically, fuse into a quantum post. The current efforts to optimize the properties of strain balanced quantum dot stacks and quantum posts are reviewed.
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