Abstract:Solar-pumped solid-state lasers are promising for renewable extreme-temperature material processing. Here, we report a significant improvement in solar laser collection efficiency by pumping the most widely used Nd:YAG single-crystal rod through a heliostat-parabolic mirror system. A conical-shaped fused silica light guide with 3D-CPC output end is used to both transmit and compress the concentrated solar radiation from the focal zone of a 2 m diameter parabolic mirror to a 5 mm diameter Nd:YAG rod within a co… Show more
“…In addition, SPLs could play a critical role in a more sustainable magnesium energy cycle, reconverting magnesium oxide to magnesium 2,9,10 . Although many improvements in the optical gain medium and solar collector design have been reported since the first demonstration of an SPL 11 , most SPLs still rely on lens or mirror concentrator systems with concentration factors on the order of thousands to obtain sufficient gain in the irradiated active medium [12][13][14][15][16][17][18] . Such concentration optics limit the practicality of SPLs because they are expensive and require very precise tracking of the sun to keep the focal point on the active medium to within 0.01°1 9 , which is challenging at high winds.…”
A solar-pumped laser (SPL) that converts sunlight directly into a coherent and intense laser beam generally requires a large concentrating lens and precise solar tracking, thereby limiting its potential utility. Here, we demonstrate a fully-planar SPL without a lens or solar tracking. A Nd 3+-doped silica fiber is coiled into a cylindrical chamber filled with a sensitizer solution, which acts as a luminescent solar collector. The body of the chamber is highly reflective while the top window is a dichroic mirror that transmits incoming sunlight and traps the fluorescence emitted by the sensitizer. The laser-oscillation threshold was reached at a natural sunlight illumination of 60% on the top window. Calculations indicated that a solar-to-laser power-conversion efficiency could eventually reach 8%. Such an SPL has potential applications in long-term renewable-energy storage or decentralised power supplies for electric vehicles and Internet-of-Things devices.
“…In addition, SPLs could play a critical role in a more sustainable magnesium energy cycle, reconverting magnesium oxide to magnesium 2,9,10 . Although many improvements in the optical gain medium and solar collector design have been reported since the first demonstration of an SPL 11 , most SPLs still rely on lens or mirror concentrator systems with concentration factors on the order of thousands to obtain sufficient gain in the irradiated active medium [12][13][14][15][16][17][18] . Such concentration optics limit the practicality of SPLs because they are expensive and require very precise tracking of the sun to keep the focal point on the active medium to within 0.01°1 9 , which is challenging at high winds.…”
A solar-pumped laser (SPL) that converts sunlight directly into a coherent and intense laser beam generally requires a large concentrating lens and precise solar tracking, thereby limiting its potential utility. Here, we demonstrate a fully-planar SPL without a lens or solar tracking. A Nd 3+-doped silica fiber is coiled into a cylindrical chamber filled with a sensitizer solution, which acts as a luminescent solar collector. The body of the chamber is highly reflective while the top window is a dichroic mirror that transmits incoming sunlight and traps the fluorescence emitted by the sensitizer. The laser-oscillation threshold was reached at a natural sunlight illumination of 60% on the top window. Calculations indicated that a solar-to-laser power-conversion efficiency could eventually reach 8%. Such an SPL has potential applications in long-term renewable-energy storage or decentralised power supplies for electric vehicles and Internet-of-Things devices.
“…For clearly exhibiting the thermal loads effects on Nd:YAG solar-lasers performance, research details will be given afterward. Some literatures [1][2][3]6,7,9,[21][22][23][24][25][26][27][28][29] were made for the solar-laser efficiency improvement, whereas others included laser beam quality enhancements. 11,[26][27][28][30][31][32][33][34][35] Research details will be given for both multimode and monomode (fundamental-mode) solar-laser operations, respectively.…”
Section: Summary Of Research Details For Exhibitingmentioning
“…Despite the small overlap between the Nd:YAG absorption spectrum and the solar spectrum, Nd:YAG has been demonstrated as the best material under solar pumping because of its superior characteristic on thermal conductivity, high quantum efficiency and mechanical strength compared to other host materials [2][3][4][5][6][7][8][9][10][11]. For 1.1 at% Nd 3+ -doped YAG single-crystal medium, 22 absorption peaks are defined in ZEMAX TM numerical data.…”
Section: Numerical Analysis Of the Nd:yag Solar Laser Performancementioning
confidence: 99%
“…Parabolic mirrors have been exploited to achieve tight focusing of incoming solar radiation [2][3][4][5]. 13.9 W/m 2 collection efficiency has been achieved at the PROMES-CNRS (Odeillo, France) in 2012, by pumping a Nd:YAG single-crystal rod through a heliostat -parabolic mirror system [6]. This value is, to the best of our knowledge, the highest solar laser collection efficiency achieved with parabolic mirrors.…”
To obtain a good compromise between collection efficiency and brightness figure of merit of solar-pumped lasers, a new side-pumping scheme is proposed. Firstly the solar radiations are collected and concentrated by six 700 mm diameter Fresnel lenses. The concentrated solar radiations are subsequently reflected by six plane folding mirrors with 95% reflectivity, into a common focal spot. This allows the concentration of 1740 W solar power with about 6.4 W/mm 2 peak solar flux. A secondary concentrator is composed of six aspheric fused silica lenses, positioned around a 40 mm radius fused silica sphere, compressing all the concentrated solar radiation from the six Fresnel lenses into an 8 mm diameter by 9 mm length Nd:YAG single-crystal rod. By positioning the spherical concentrator slightly above the aspherical lenses, a more uniform absorption profile is achieved. Mechanical support with a water cooling system ensures an efficient cooling to the laser medium. Optimal laser parameters are found through ZEMAX TM and LASCAD TM numerical analysis software. Only 16% of the solar power is absorbed by Nd:YAG medium. Solar laser power of 42.6 W is numerically calculated, reaching a collection efficiency of 18.5 W/m 2 . For a 400 mm plane-concave resonance cavity with -5m radius of curvature, M 2 x = M 2 y = 22 beam quality factors are numerically predicted. A near uniform pump absorption profile can be achieved by increasing the number of Fresnel lens and folding mirrors.
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