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High Rollover Power from 8xx nm and 9xx nm Asymmetric Epitaxial Laser Structures with Optical Trap

机译:具有8xx NM和9xx NM不对称外延激光结构的高卷式电力,具有光学陷阱

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The quest for high operating powers from diode lasers has been stimulated in recent years by the increasing demands of industrial users and by programs such as SHEDS. Record powers and power densities of 19 W from 100 μm (190 mW/μm) [1] and 18.5 W from a 90 μm aperture (205 mW/μm) [2] were reported in 2007 for devices operating in the 9xx nm range (915 to 980 nm). Powers higher than 20 W from 100 μm [3] and 21 W from 90 μm [4] have already been reported in 2008 by the same teams. While high efficiency was a major goal of the SHEDS program, the industrial market is more interested in obtaining the highest reliable output power per device, which eventually will lead to reductions in the price per Watt. From the device design perspective, both applications impose similar conditions: low attenuation coefficient, low series resistance and low thermal resistance. A key difference between the applications is related to the device length: a high efficiency can be more easily obtained from short devices, whereas the highest powers can only be obtained from long devices.
机译:近年来,近年来,通过越来越多的工业用户的需求以及棚屋等方案,近年来促进了对二极管激光器的高操作权。的记录功率,并从100微米(190毫瓦/微米)[1]和18.5 W的一个90微米孔径(205毫瓦/微米)[2]的报道,2007年在9XX nm范围内操作的装置(19 W的功率密度915到980 nm)。通过同一团队在2008年报告了高于100μm[3]和21倍的高于20 W的功率从20μm[4]。虽然高效率是Sheds计划的主要目标,但工业市场更有兴趣获得每个设备的最高可靠的输出功率,最终会导致每瓦价格的价格降低。从设备设计的角度来看,这两个应用都施加了类似的条件:低衰减系数,低串联电阻和低热电阻。应用程序之间的关键差异与器件长度有关:从短设备中可以更容易地获得高效率,而最高功率只能从长设备获得。

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