Confinement and Threshold Modeling for High Temperature GeSn and GeC/GeCSn Lasers

Models of GeSn and GeCSn quantum well (QW) lasers were compared to predict net gain and threshold for computing applications. GeSn showed weak confinement of electrons in both k-space (directness) and real space, as well as a weak optical confinement factor. Using material parameters from ab-initio calculations, adding 1-2% carbon to Ge or GeSn could provide all three confinements simultaneously, with up to 350 meV of electron confinement by Ge QW barriers and a direct bandgap that is 50-220 meV below the indirect gap. A 2-4x increase in electron effective mass preserves strong confinement even in narrow, 5 nm GeCSn/Ge quantum wells. Simply keeping electrons out of non-lasing, higher energy states doubles the differential gain compared with GeSn lasers and reduces free carrier absorption, while deeper QWs further enhance gain. GeCSn laser thresholds as low as 160 A/cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> are predicted for operation at temperatures of 100 °C, two orders of magnitude lower than comparable GeSn lasers.

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Publication Details

Journal
IEEE Journal of Selected Topics in Quantum Electronics
Published
2024-12-04
DOI
https://doi.org/10.1109/jstqe.2024.3511716
Primary Topic
Photonic and Optical Devices
Type
article
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article

Confinement and Threshold Modeling for High Temperature GeSn and GeC/GeCSn Lasers

Seth R. Bank, Md. Shamim Reza, Augustus W. Arbogast, Qian Meng et al.
2 links
IEEE Journal of Selected Topics in Quantum Electronics
Photonic and Optical Devices
article

Confinement and Threshold Modeling for High Temperature GeSn and GeC/GeCSn Lasers

Seth R. Bank, Md. Shamim Reza, Augustus W. Arbogast, Qian Meng, Tuhin Dey, Mark A. Wistey
article en

Abstract

Models of GeSn and GeCSn quantum well (QW) lasers were compared to predict net gain and threshold for computing applications. GeSn showed weak confinement of electrons in both k-space (directness) and real space, as well as a weak optical confinement factor. Using material parameters from ab-initio calculations, adding 1-2% carbon to Ge or GeSn could provide all three confinements simultaneously, with up to 350 meV of electron confinement by Ge QW barriers and a direct bandgap that is 50-220 meV below the indirect gap. A 2-4x increase in electron effective mass preserves strong confinement even in narrow, 5 nm GeCSn/Ge quantum wells. Simply keeping electrons out of non-lasing, higher energy states doubles the differential gain compared with GeSn lasers and reduces free carrier absorption, while deeper QWs further enhance gain. GeCSn laser thresholds as low as 160 A/cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> are predicted for operation at temperatures of 100 °C, two orders of magnitude lower than comparable GeSn lasers.

IEEE Journal of Selected Topics in Quantum ElectronicsVol. 31(1: SiGeSn Infrared Photon. and)
Texas State University (US), Lam Research (United States) (US), The University of Texas at Austin (US)
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Photonic and Optical Devices
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