UCC crest
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Device details

The lasers studied were GaAs/AlGaAs structures with monolithic semiconductor DBRs and oxide layers on both sides of the active region. The active layer was composed of five 8 nm GaAs quantum wells contained in a $1\lambda$ cavity. The monolithic DBRs are quarter wave thick pairs of Al0.16Ga0.84As/Al0.92Ga0.08As with 25 pairs in the top DBR. The thin (18 nm) Al0.98Ga0.02As oxide confinement layers were embedded in low index quarter-wave layers 3 mirror periods from the active region. The aim of this design was to reduce the overlap between the field and the apertures and thus reduce aperture scattering [62], a factor implicated in the higher threshold gain of smaller devices [60]. A series of lasers with different mesa sizes ranging from 30 $\mu$m to 70 $\mu$m was fabricated by etching square mesas through the active layer with reactive ion etching and oxidising laterally the high Al content layer [55]. The difference in side length between successive mesas was 0.5 $\mu$m, making available lasers with side lengths between <0.5 $\mu$m and 10 $\mu$m in 0.5 $\mu$m steps. On a cryogenic stage the devices lased with heat sink temperatures ranging from 100 K to 400 K with a minimum threshold around 300 K. Measurements of the polarisation properties of small ($\sim 3.0$ $\mu$m aperture sidelength), single mode devices suggests that the sample is strained, as a single polarisation is maintained to within $\pm 3^o$ over the entire temperature range, and across the wafer the same polarisation is found for all devices.


  
Figure: The transverse mode structure of a $10 \times 10$ $\mu$m2 VCSEL, with threshold at 3.6 mA. Each symbol (square, star, triangle...) represents a different transverse mode. The measurement does not include polarisation elements and only modes that lase over a large current range are recorded.
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Next: The experiment Up: Transverse modes of small Previous: Introduction