2011•Unpublished venueRequires access

A coupled quantum dot laser amplifier using raman transitions between spin singlet and triplet states

J. M. Elzerman, K. M. Weiss, J. Miguel Sanchez, Ataç İmamoğlu

Open publisher page 3 citations

Abstract

We report the observation of Raman amplification in a three-level lambda scheme realized in a single coupled quantum dot (CQD) molecule. When both QDs contain a single electron, the lowest energy levels correspond to spin singlet (S) or triplet (T) states, which share a common optically excited state (X). Electron tunneling between the two dots gives rise to an exchange splitting between the S and T states, which allows us to selectively address them optically. We take advantage of fast (-10 ns) relaxation from T to S to generate population inversion and laser amplification on the T-to-X transition by pumping the S transition.

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What this paper is about

We report the observation of Raman amplification in a three-level lambda scheme realized in a single coupled quantum dot (CQD) molecule. When both QDs contain a single electron, the lowest energy levels correspond to spin singlet (S) or triplet (T) states, which share a common optically excited state (X). Electron tunneling between the two dots gives rise to an exchange splitting between the S and T states, which allows us to selectively address them optically. We take advantage of fast (-10 ns) relaxation from T to S to generate population inversion and laser amplification on the T-to-X transition by pumping the S transition.

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OpenAlex reports 3 citations for this work. Citation counts describe recorded attention and do not establish research quality.

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Available abstract

We report the observation of Raman amplification in a three-level lambda scheme realized in a single coupled quantum dot (CQD) molecule. When both QDs contain a single electron, the lowest energy levels correspond to spin singlet (S) or triplet (T) states, which share a common optically excited state (X). Electron tunneling between the two dots gives rise to an exchange splitting between the S and T states, which allows us to selectively address them optically. We take advantage of fast (-10 ns) relaxation from T to S to generate population inversion and laser amplification on the T-to-X transition by pumping the S transition.

Key concepts: Excited state, Singlet state, Quantum dot, Population inversion, Quantum tunnelling, Physics, Laser, Population

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