2015
DOI: 10.1109/jqe.2015.2410288
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Graphene Q-Switched Cr:ZnSe Laser

Abstract: For the first time, to the best of our knowledge, a stable Q-switched Cr:ZnSe laser was realized with the graphene saturable absorber grown on SiC substrate. Under an absorbed pump power of 1.8 W, a maximum average output power of 256 mW was obtained with an optical-to-optical conversion efficiency of 14% and a slope efficiency of 19.6%, corresponding to the highest single pulse energy of 1.66 µJ. The shortest pulse width and highest pulse repetition rate were 157 ns and 169 kHz, respectively. Using a nanoscan… Show more

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Cited by 24 publications
(24 citation statements)
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“…[54] The N-methoxy amide directing group was crucial for the Rh(III)-catalyzed C(sp 2 )–H activation. The authors used iodosylbenzene to oxidize hydroquinones to generate quinones in situ .…”
Section: Rhodium Catalysismentioning
confidence: 99%
“…[54] The N-methoxy amide directing group was crucial for the Rh(III)-catalyzed C(sp 2 )–H activation. The authors used iodosylbenzene to oxidize hydroquinones to generate quinones in situ .…”
Section: Rhodium Catalysismentioning
confidence: 99%
“…19 Eventually, we wish to derive an equation expressing R spon in terms of J. Let us analyze the carrier recombination process inside the quantum well by means of the traditional ABC model for simplicity 14 (although the traditional ABC model somewhat fails to explain the "efficiency droop" phenomenon of InGaN-based MQW LEDs), namely J/qd = An + Bn 2 + Cn 3 , where A and C represent Shockley-Read-Hall (SRH) and Auger coefficients; q the elementary charge; d the thickness of the MQW. Solving this ABC model directly for deriving a formula expressing n in terms of J, however, is quite complicated, prompting us to seek another approach instead.…”
Section: Theorymentioning
confidence: 99%
“…A vertically uniform carrier distribution among the QWs is a challenge in all GaN-based light-emitters 83,84 due to the large difference between the activation energy of donor and acceptor impurities 85 , the strong imbalance between electron and hole mobilities 86 , the large band offsets and, possibly even more critical, the spontaneous and piezoelectric polarization effects at heterointerfaces 87,88 . In order to maximize the radiative recombination in the QWs, one should minimize current crowding 89,90 as well as carrier leakage beyond the active region, which can involve both electrons [91][92][93] and holes 94 and could be enhanced by Auger 95,96 and excited subband recombination 97 . Electrons can be prevented from leaking into the p-GaN layers by inserting an energy barrier in the conduction band between QWs and p-layers, a socalled electron-blocking layer (EBL).…”
Section: Carrier Transport and Optical Gainmentioning
confidence: 99%