972 resultados para Nd : YAG ceramic laser
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Purpose: Current panretinal laser photocoagulative parameters are based on the Diabetic Retinopathy Study, which used exposures of 0.1 - 0.5 second to achieve moderate intensity retinal burns. Unfortunately, many patients find these settings painful. We wanted to investigate whether reducing exposure time and increasing power to give the same endpoint, is more comfortable and effective. Methods: 20 patients having panretinal photocoagulation for the first time underwent random allocation to two forms of laser treatment: half of the retinal area scheduled for treatment was treated with Green Yag laser with conventional parameters {exposure time 0.1 second (treatment A), power density sufficient to produce a visible grey - white burns}. The other half treated with shorter exposure 0.02 second (treatment B). All patient were asked to evaluate severity of pain on a visual analogue scale ranging from 0 - 10 (0 = no pain, 10 = most severe pain). All patients were masked as to the type of treatment. The order of carrying out the treatment on each patient was randomised. Fundus photographs were taken of each hemifundus to confirm treatment. Results: Of the 20 patients, 17 had proliferative diabetic retinopathy, 2 had ischaemic central retinal vein occlusion and one had ocular ischaemic syndrome. The average pain response to treatment A was 5.11 on a visual analogue scale with a mean power of 0.178 Watt; the average pain response to treatment B was 1.40 with a mean power of 0.489 Watt. Short exposure laser burns were significantly less painful (P < 0.001). Conclusion: Shortening exposure time with increased power is more comfortable for patients undergoing panretinal photocoagulation than conventional parameters.
Adhesion of fibroblasts cells on dentine cut surfaces by Er:YAG laser treated or not by Nd:YAG laser
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考虑固体热容激光器对工作介质的要求,对比分析了掺钕的玻璃、YAG和GGG的多种材料性能。并对三者在激光工作周期内的瞬态温度场及热应力进行了数值模拟。结果表明:在给定的边界及工作条件下,当钕玻璃激光器以热容方式工作,时间为5S时,介质最高升温超过400K,最大热致应力为25MPa,接近其断裂极限的50%。在此条件下进行冷却,当水温为283K时,需经过约120S才基本恢复到初始工作状态。而Nd:YAG和Nd:GGG两种介质在相同输入工作条件下,工作时间可达10S,且温度分布相对平坦,温差和热应力较小,经水冷约
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实验研究了高重复率、大功率半导体激光二极管阵列(LDA)侧面环绕抽运的Nd:YAG激光放大器的放大特性、热焦距变化和热致双折射效应引起的退偏特性。偏振光绎千赫兹高功率单通激光放大器,获得约3倍的光脉冲能量放大,脉冲宽度基本保持不变,其输出的P分量与S分量的能量比趋于常数3:1,实验测得的能量放大倍率及放大光束的椭圆偏振度与理论预期吻合很好。
Resumo:
对激光二极管(LD)抽运固体激光器中大功率线阵激光二极管三向对称侧面抽运的漫反射腔结构进行了研究。激光器使用Nd:YAG作为激光晶体,电光器件材料为KD^*P晶体,漫反射体为陶瓷材料。实验表明,抽运光的利用率和均匀性有较大提高。在重复频率为10Hz下,实现了脉冲宽度8ns,最大平均功率为近2W的1064nm红外激光输出,激光器的效率有显著提高。
Resumo:
对高平均功率输出的激光二极管侧面抽运电光调Q倍频 Nd:YAG激光器进行了研究,当采用90个60W的脉冲激光二极管阵列抽运时,在重复频率为10Hz下,实现了最大平均功率为1180mW的1064nm红外激光输出,光-光转换效率为11%。腔外倍频获得600mW的532nm绿光输出,倍频效率达到50%以上。
Resumo:
实验研究了腔内位相锁定来至一LAD侧面抽运的Nd:YAG板条的两束激光,输出镜面出现干涉条纹,获得1.13W的相干光,其组束效率达到64.9%,相干度约60%。实验中发现只需要一根作为滤波的金属丝放在离输出镜合适的位置都就能有效稳定干涉条纹,金属丝引起的损耗低于8%。
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The fluorescence emission spectra of Cr:Nd:YAG crystal are measured and the effective stimulated emission cross-section of the crystal is obtained from -80 to +80 degrees C. A linear temperature dependence between -80 and +80 degrees C is reported for the 1.064-mu m peak stimulated emission cross-section of Cr:Nd:YAG crystal. (C) 2005 Elsevier Ltd. All rights reserved.
Resumo:
Large sized neodymium-doped Y3Al5O12 (Nd:YAG) laser crystals have been grown by temperature gradient technique (TGT) method and compared with Czochralski (Cz) method. The comparison of these two crystal growth methods has been listed. The results showed that the TGT method has many advantages over the Cz method. The concentration distribution of Nd ions in the crystals was determined and the absorption spectra of these crystals have been investigated and compared. The TGT grown highly doped Nd:YAG crystal has a larger absorption FWHM than that of Cz grown Nd:YAG crysral. Highly doped Nd:YAG (similar to 2.8 at. pct) crystals could be obtained by TGT.
Resumo:
用温度梯度法(TGT)生长了大尺寸的Nd:YAG激光晶体,测试了室温下的吸收谱并利用吸收谱研究了Nd离子在YAG晶体中的分布。比较了温度梯度法与提拉法生长晶体的区别。根据热容激光的原理,利用生长的Nd:YAG激光晶体片设计了热容激光器,利用侧面抽运,获得了1200w的激光输出,工作时间为2s,光-光转换效率为30%。