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Showing papers by "Shashank Gupta published in 2018"


Journal ArticleDOI
TL;DR: In this paper, the authors present a detailed model of light emission in Ge that accurately models inter-valence-band absorption (IVBA) in the presence of strain and other factors such as polarization, doping, and carrier injection.
Abstract: A complementary metal-oxide semiconductor compatible on-chip light source is the holy grail of silicon photonics and has the potential to alleviate the key scaling issues arising due to electrical interconnects. Despite several theoretical predictions, a sustainable, room temperature laser from a group-IV material is yet to be demonstrated. In this work, we show that a particular loss mechanism, inter-valence-band absorption (IVBA), has been inadequately modeled until now and capturing its effect accurately as a function of strain is crucial to understanding light emission processes from uniaxially strained germanium (Ge). We present a detailed model of light emission in Ge that accurately models IVBA in the presence of strain and other factors such as polarization, doping, and carrier injection, thereby revising the road map toward a room temperature Ge laser. Strikingly, a special resonance between gain and loss mechanisms at 4%--5% $\ensuremath{\langle}100\ensuremath{\rangle}$ uniaxial strain is found resulting in a high net gain of more than $400\phantom{\rule{0.28em}{0ex}}{\text{cm}}^{\ensuremath{-}1}$ at room temperature. It is shown that achieving this resonance should be the goal of experimental work rather than pursuing a direct band gap Ge.

23 citations


Proceedings ArticleDOI
13 May 2018
TL;DR: In this article, the first experimental observation of low-threshold lasing in germanium nanowires was made, and the lasing threshold was ∼3.0 kW cm−2, which is more than one order of magnitude lower than the state-of-the-art GF laser.
Abstract: We report the first experimental observation of low-threshold lasing in strained germanium nanowires. The lasing threshold is ∼3.0 kW cm−2 which is more than one order of magnitude lower than the state-of-the-art germanium-tin Fabry-Perot laser.

1 citations