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对掺钕光纤激光器输出功率沿光纤的分布以及不同光纤长度下抽运功率和输出功率沿光纤的分布进行了数值模拟.以808nm半导体激光器为抽运源,掺钕双包层保偏光纤为增益介质,对保偏光纤激光器进行了探索性的实验研究.分别就光纤不同弯曲形状和弯曲半径对激光器输出功率指标和偏振特性的影响进行了研究,实验中发现在1060nm和1092nm处有两个峰值.在波长1060nm处得到了7.35W的连续偏振激光输出,斜率效率为58.3%.
关键词:
激光技术
光纤激光器
掺钕保偏光纤
偏振 相似文献
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掺Yb3+双包层大模场面积微结构光纤(micro-structured fibers,MSF)是作为超大功率光纤激光器的理想介质。本文首先采用非化学气相熔炼法制备出掺Yb3+石英基玻璃材料,然后按照设计要求,通过排布拉制法制备了掺Yb3+双包层大模场面积微结构光纤。分别利用钛宝石飞秒激光器(波长调至为975 nm)和波长为980 nm LD激光器作为激励源,对掺Yb3+双包层大模场面积微结构光纤的荧光光谱进行分析,实验结果表明:该光纤在波长为1 050 nm处产生强的荧光,同时该光纤还能有效的抑制合作发光现象(coopera-tive luminescence)的产生。 相似文献
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研究了碱土金属氧化物对Bi离子掺杂RO-Al2O3-SiO2 (R=Ca, Sr, Ba)玻璃近红外超宽带发光性质的影响. 结果表明: 玻璃样品在不同抽运源激发下都可检测到较强的近红外超宽带发光. 在808 nm激光激发下, 随着碱土金属离子半径的增加, Bi离子在1 300 nm附近的近红外发光强度显著增加, 荧光半高宽逐渐增加, 其荧光寿命最长可超过600 μms; 而在690 nm激光激发下, 随着碱土金属离子半径的增加, Bi离子在1 100 nm附近的近红外发光呈减弱趋势, 荧光半高宽逐渐增大, 半高宽最大可超过400 nm. 近红外发光可能源于两种不同形式铋的发光中心. 针对上述结果探讨了该玻璃体系中Bi离子近红外发光的机理. 相似文献
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采用改进化学汽相沉积结合溶液掺杂法制备了Yb/P/Al共掺的石英光纤预制棒,通过光纤芯层的组份和制备工艺的优化,实现了Yb3+的高浓度掺杂和均匀掺杂.预制棒芯层Yb2O3掺杂浓度达到~4wt.%,Yb3+在1 080 nm处荧光寿命为1 780μs.成功拉制出内包层截面形状为八边形的双包层光纤,纤芯直径为7.5 μm,包层吸收系数达到~5 dB/m@976 nm.利用拉制的掺镱双包层光纤开展了全光纤结构的掺镱光纤激光器性能测试实验,实现了5.15W的激光输出,斜率效率达到76%. 相似文献
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波长无啁啾调谐窄线宽掺Yb3+双包层光纤激光器 总被引:1,自引:0,他引:1
用相位掩模法, 在圆形掺Yb3+双包层光纤上制作了Bragg光纤光栅,并用它作为双包层光纤激光器的输出腔镜, 在光栅反射中心波长1055.2 nm位置得到了窄线宽的激光输出, FWHM为0.271 nm, 信噪比约为40 dB.这种结构的双包层光纤激光器, 在双包层增益光纤和后腔镜间没有连接损耗, 减小了双包层光纤激光器体积. 用自行制作的等强度梁对作为输出腔镜的光纤光栅做双向应力调谐, 实现了激光波长无啁啾调谐输出, 调谐范围1051.1~1060.04nm,调谐量达8.9nm, 调谐过程中激光3 dB线宽基本无变化. 相似文献
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在MCVD车床上利用“湿法”掺杂方法研制出纤芯高掺Ge的石英基掺Tm3+光纤预制棒,采用侧面研磨和抛光工艺制成横截面为正六边形的光纤预制棒.经拉丝,内层涂覆低折射率材料后制成包层抽运光纤.测试其吸收谱,并对光纤参数进行优化.通过在光纤两端紫外写入光纤Bragg光栅,制成线形光学谐振腔,在工作波长793nm的激光抽运下,获得工作波长1947.1031nm、功率2.05W的激光输出.由此证明这种光纤具有优异的光学特性.
关键词:
3+光纤')" href="#">石英基掺Tm3+光纤
光纤Bragg光栅
包层抽运
光纤激光器 相似文献
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Bi-doped SiO 2 –Al 2 O 3 –GeO 2 fiber preforms are prepared by modified chemical vapor deposition (MCVD) and solution doping process. The characteristic spectra of the preforms and fibers are experimentally investigated, and a distinct difference in emission between the two is observed. Under 808-nm excitation, an ultra-broad near-infrared (NIR) emission with full-width at half-maximum (FWHM) of 495 nm is observed in the Bi-doped fiber. This observation, to our knowledge, is the first in this field. The NIR emission consists of two bands, which may be ascribed to the Bi 0 and Bi + species, respectively. This Bi-doped fiber is promising for broadband optical amplification and widely tunable laser. 相似文献
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通过拉曼散射光谱,吸收光谱,荧光发射寿命和808 nm LD激发下的红外荧光光谱的实验测量,系统研究了Nd3+:SrMoO4晶体的自受激拉曼光谱性质.分析指认了拉曼散射光谱中各拉曼峰所对应的晶格振动模式,得出了其SRS活性最强的声子频率约为898 cm-1,对应于(MoO2-4)离子团的完全对称光学伸缩振动Ag模;通过J-O理论对晶体的吸收谱进行了全面的光谱参数计算,得出4F3/2→4I11/2跃迁的积分发射截面达0.57×10-18 cm2,自发辐射概率为141.06 s-1;同时,实验测得该跃迁的荧光发射寿命约为0.2 ms.最后,结合808 nm LD激发下的红外波段荧光光谱,论证了SrMoO4晶体中Nd3+离子1068 nm发射通过拉曼频移获得1180 nm一级斯托克斯激光发射的可能性,为Nd3+:SrMoO4晶体的自受激拉曼激光器研究提供了理论依据.
关键词:
3+离子')" href="#">d3+离子
4 晶体')" href="#">SrMoO4 晶体
自受激拉曼散射 相似文献
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We report the results of our investigation on the optical properties of the bismuth borate glass (75B2O3-25Bi2O3). Unusual near-infrared (NIR) and visible band luminescence was observed when the sample was excited by lasers working at
532 and 808 nm. The NIR fluorescent lifetime of the sample measured at room-temperature was longer than two hundred microseconds.
This indicated that this glass system could be a new candidate for the broadband optical amplification and laser material
covering the wavelength from 1100 to 1300 nm. The influences of preparation conditions and glass compositions on the luminescence
properties of glasses were investigated. It was found that the heat-treatment under air and hydrogen atmosphere can both weaken
the infrared luminescence of the materials. Furthermore, with the addition of oxidation agent CeO2, the sample did not show any NIR luminescence upon the excitation of the lasers working at 532 or 808 nm. All the results
indicated that the infrared luminescence center should be Bi+ ions. 相似文献
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Superbroadband 1310 nm emission from bismuth and tantalum codoped germanium oxide glasses 总被引:4,自引:0,他引:4
Near-infrared broadband emission from bismuth-tantalum-codoped germanium oxide glasses was observed at room temperature when the glasses were pumped by an 808 nm laser diode. The emission band covered the O, E, S, C, and L bands (1260-1625 nm), with a maximum peak at approximately 1310 nm, a FWHM broader than 400 nm, and a lifetime longer than 200 micros. The observed broadband luminescence was attributed to bismuth clusters in the glasses. Bismuth-tantalum-codoped germanium oxide glass might be promising as amplification media for broadly tunable lasers and wideband amplifiers in optical communications. 相似文献
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Bufetov IA Firstov SV Khopin VF Medvedkov OI Guryanov AN Dianov EM 《Optics letters》2008,33(19):2227-2229
Bismuth-doped fiber lasers operating in the range 1300-1470 nm have been demonstrated for the first time, to our knowledge. It has been shown that Bi-doped alumina-free phosphogermanosilicate fibers reveal optical gain in a wavelength range of 1240-1485 nm with pumping at 1205, 1230, or 808 nm. 相似文献
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Fufei Pang Xianglong Zeng Zhenyi Chen Tingyun Wang 《Optical and Quantum Electronics》2007,39(12-13):975-981
We fabricated a novel special silica optical fiber doped with nano-semiconductor material InP in double cladding layers by using conventional modified chemical vapor deposition (MCVD) process. During the deposition process, InP powder was placed at the entrance of silica substrate tube and vaporized by high temperature. With the help of nitrogen gas flow, the vaporized InP was carried into silica substrate tube and deposited on the inner surface in the form of nano-particle. The physical structure and amplification characteristics of the special fiber were investigated. From the refractive index distribution of the preform, we can observe obvious increase in inner cladding index, which attributes to InP dopant. By using 532 nm LD as pump, a broadband amplified spontaneous emission (ASE) was demonstrated in the wavelength range from 1,080 to 1,350 nm. The proposed nano- semiconductor doped fiber with optical amplification is expected to a wide application in optical fiber communications. 相似文献
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以970 nm和808 nm半导体激光器作为抽运源,从光纤长度和抽运功率两个方面,探讨了Nd~(3+)/Yb~(3+)摩尔浓度比约为4:1的共掺磷酸盐玻璃光纤的发光与激光特性.在970 nm抽运下,光纤光谱以Yb~(3+)离子的发光为主,但Yb~(3+)→Nd~(3+)能量传递会对光纤光谱(激光和受激放大自发辐射)产生调制作用,调制作用随970 nm抽运功率或光纤长度的增加而显著,甚至出现显著的双波长激光现象.尽管玻璃样品中Nd~(3+)→Yb~(3+)的能量传递效率ηNd→Yb高达64%,但在808 nm抽运下,激光峰始终在1053 nm附近产生,且与808 nm抽运功率大小和光纤长度无关.为解释这一现象,推导了考虑Nd~(3+)离子受激辐射的能量传递模型.从理论模型来看,Nd~(3+)→Yb~(3+)能量传递作用随Nd~(3+)离子受激辐射信号光强度的增加而迅速减弱,这与该光纤实际测试的荧光光谱随808 nm抽运功率的变化规律相符合.因此,当采用Nd~(3+)离子来敏化Yb~(3+)离子时,需要考虑Nd~(3+)离子的受激辐射对Nd~(3+)→Yb~(3+)能量传递的抑制作用. 相似文献
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包层泵浦的L波段Er3+/Yb3+共掺光纤激光器 总被引:5,自引:4,他引:1
报道了一种工作波长在L波段的包层泵浦Er3+/Yb3+共掺光纤环形激光器. 环形腔内的激光工作介质为一段9 m长的Er3+/Yb3+共掺高掺杂光纤. 利用6个976 nm LD同时抽运前段Er3+/Yb3+共掺双包层光纤产生的放大自发辐射谱作二次抽运源, 使腔内增义谱由C波段移到L波段, 实现了L波段光纤激光器的稳定输出; 采用包层泵浦技术, 在抽运功率为3594.5 mW时, 测得泵浦入纤功率为2731.8 mW, 实现了输出连续功率最大518.4 mW,斜率效率达到19% 的激光输出; 所形成激光的工作波长为1613.94 nm, 激光光谱的3 dB带宽为1.5 nm, 边模抑制比接近于50 dB. 相似文献
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同带抽运是目前实现高功率光纤激光器的有效手段.本文基于同带抽运方式,以国产25/250μm掺镱双包层光纤为增益光纤,构建了全光纤化的主控振荡器功率放大器.实验中采用的国产光纤是中国电子科技集团公司第四十六研究所采用化学气相沉积结合气相-液相复合掺杂工艺制备的,其Yb~(3+)离子的分布更均匀,吸收截面更大,吸收系数更高.实验中,在种子光功率为67.8 W、抽运总功率为3511 W的条件下,实现了3079 W的激光输出,斜效率为85.9%,光束质量M~2约为2.14,3dB带宽为1.4nm,这是目前基于国产光纤同带抽运方式实现的最高功率.理论和实验结果表明国产光纤制备技术不断成熟,已经具备承受高功率输出的能力.继续提高抽运功率,优化增益光纤长度,改良散热方式,国产光纤有望实现更高功率的激光输出. 相似文献