In this paper, state-of-the-art research on two-state passive mode-locking of InAs/(In)GaAs quantum dot lasers is reviewed with a focus on the influence of extended absorber biasing conditions on the two quantized emission-states of a strongly inhomogeneously broadened quantum dot laser. We start with the recently demonstrated state-selectivity of ground-state, joint ground- and excited-state and then sole excited-state emission by a resistor Self-Electro-Optical Effect configuration. This regime is then extended towards the reverse-bias regime giving access to both excited-state and joint ground- and excited-state emission and to higher laser output power. Finally, we find an excellent accordance of the emission-states at the boundary of the two regimes. The occurrence and evolution of the emission-states in dependence on the biasing conditions are explained qualitatively.
Extended ground-state and excited-state emission-state control in a mode-locked two-section quantum dot laser / Breuer, S.; Rossetti, Mattia; Drzewietzki, L.; Bardella, Paolo; Montrosset, Ivo; Hopkinson, M.; Wolfgang Elsasser, W.. - STAMPA. - (2011). (Intervento presentato al convegno Transparent Optical Networks (ICTON), 2011 13th International Conference on tenutosi a Stockholm nel 26-30 June 2011) [10.1109/ICTON.2011.5970825].
Extended ground-state and excited-state emission-state control in a mode-locked two-section quantum dot laser
ROSSETTI, MATTIA;BARDELLA, PAOLO;MONTROSSET, Ivo;
2011
Abstract
In this paper, state-of-the-art research on two-state passive mode-locking of InAs/(In)GaAs quantum dot lasers is reviewed with a focus on the influence of extended absorber biasing conditions on the two quantized emission-states of a strongly inhomogeneously broadened quantum dot laser. We start with the recently demonstrated state-selectivity of ground-state, joint ground- and excited-state and then sole excited-state emission by a resistor Self-Electro-Optical Effect configuration. This regime is then extended towards the reverse-bias regime giving access to both excited-state and joint ground- and excited-state emission and to higher laser output power. Finally, we find an excellent accordance of the emission-states at the boundary of the two regimes. The occurrence and evolution of the emission-states in dependence on the biasing conditions are explained qualitatively.Pubblicazioni consigliate
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https://hdl.handle.net/11583/2498823
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