光纤光谱仪绝对光谱辐射定标新技术

在700 nm～900 nm波段范围内,用1 000℃黑体标定光纤光谱仪(200 nm～1 100 nm),获得其在该波段范围内的绝对光谱响应函数.通过测量光纤光谱仪对不同色温下卤钨灯的光谱响应,将700 nm～900 nm波段的响应函数推延至400 nm～700 nm波段范围,最终得到400 nm～900 nm波段内的绝对光谱响应函数.光纤光谱仪对不同色温下卤钨灯的5次测量结果表明:在550 nm～900 nm范围内,所获得的绝对光谱响应合成不确定度小于3.53%.     

LCOS液晶波前校正器的色散研究

对液晶波前校正器的色散问题进行了研究,测定了250D离焦、250D像散两种像差镜和650nm、670nm、710nm、840～860nm、835～865nm、830～870nm五种滤光片下的色散.结果表明:可见到近红外波段内20～30nm带宽的光是液晶自适应光学系统的理想光源,可实现系统较大的能量利用率和较小的色散.对于中心波长850nm的近红外光,当光源的带宽低于30nm时,LCOS的色散对系统像差影响较小,可以忽略,系统的光能利用率又较大;一旦光源带宽高于40nm,LCOS的色散会对系统的像差产生明显的影响,使成像分辨率大大降低.     

石油污染水体荧光图谱特征分析

石油类物质对水体吸收系数的影响主要通过黄色物质(CDOM)体现出来,CDOM和石油类物质皆具有荧光基团,如果两者的荧光图谱各自特征明显的话,那么有望利用荧光技术分离出水中石油物质和CDOM各自对水体总吸收系数的贡献,从而提高水体石油类物质含量的遥感反演精度。以大连周边海水和山区水库水为自然水体本底,分别与取自采油污水厂和炼油污水厂的污水进行混合配比,利用试验数据分析了仅含CDOM、含油与CDOM混合、仅含石油三种水样的荧光图谱特征,旨在为利用荧光技术分离出水中石油物质和CDOM各自对水体总吸收系数的贡献提供依据。分析结果表明：(1)自然水体中,海水的CDOM具有三个典型荧光峰,分别位于Ex:225-230 nm/Em:320～330 nm,Ex:280 nm/Em:340 nm和Ex:225-240 nm/Em:430～470 nm,为海水叶绿素碎屑物所致;淡水具有两典型荧光峰,分别位于：Ex：240～260 nm/Em：420～450 nm和Ex：310～350 nm/Em：420～440 nm,为陆源物质所致;(2)用正己烷萃取后的仅含油水样,具有1～3个荧光峰,分别位于Ex: 220～240 nm/Em：320-340 nm,Ex:270～290 nm/Em：310～340 nm和Ex: 220～235 nm/Em：280～310 nm,为各自烃类成分所致;(3)在自然水体中混入油污水后,含油和CDOM的水样荧光图谱呈现出一个非常强的荧光峰,位于Ex：230～250 nm/Em：320～370 nm,为CDOM和石油类物质荧光成分共同作用所致。     

宽光谱棱镜型太阳光谱仪设计

为实现大气层外太阳光谱辐照度(SSI)变化的长期例行监测,设计了一种星载宽光谱太阳光谱仪结构。全系统仅使用单片折反式曲面棱镜实现太阳光谱250～2500 nm的分光,并通过棱镜转动实现谱平面上多探测器的同步扫描探测;同时基于Huygens子波点扩展函数（PSF）仿真了光谱仪的光谱响应函数（SRF）和光谱分辨率。分光棱镜在±2.5°扫描转角内的全谱段子午像差小于8μm;光谱分辨率在紫外谱段(250～400 nm)为0.7～3.5 nm,可见/近红外谱段(400～1000 nm)为3.5～35.0 nm,短波红外谱段(1000～2500 nm)内为28.5～41.2 nm。整个系统结构简单紧凑,性能稳定可靠,分光和像差校正能力满足大气层外太阳光谱辐照度长期监测需求。     

宽波段范围内双光子泵浦钠分子产生的紫外和紫区漫散带受激辐射

本文首次报道了在620.0～670.0nm宽波段范围内以观光子泵浦方式产生钠分子紫外区(350.0～385.0nm)和紫区(405.0～460.0nm)受激漫散带辐射的结果.文中还对所涉及的激发和发射机制进行了讨论.     

三亚鹿回头海域珊瑚、石莼和碎石反射率光谱分析

以南海三亚湾鹿回头海域八种常见造礁石珊瑚优势种的反射率光谱为代表,用光谱仪测量它们和此海域常见底质石莼以及碎石的反射率光谱。通过反射率、导数光谱法研究了三亚鹿回头海域造礁石珊瑚、石莼和碎石的光谱差异。石莼于561.4 nm处出现反射率高达48%左右的显著波峰,在500～700 nm波长范围和造礁石珊瑚反射率差异较大;碎石反射率明显高于造礁石珊瑚反射率,整体差异显著。导数分析结果表明造礁石珊瑚、石莼和碎石可区分波段为：造礁石珊瑚与石莼主要为一阶导数在485～487,505～510,515～529,559～578,587～593,598～603和667～670 nm等波段。二阶导数在494.4～505.7,524～534.5,543.6～561.4和567.2～579.7 nm波段。四阶导数在515.8～430,621～627.1,628.8～635.6,639.3～645,661.8～669.8和678.4～682.4 nm等波段。造礁石珊瑚与碎石一阶导数反射光谱,主要为400～413.7,414～418,484.8～486.9,506～509.6,514.5～528.9,576.9～587.6和602.7～653.4 nm波段。二阶导数主要为,451.6～461.6,564.5～570.7和677～685 nm。四阶导数主要为,412.6～425.3,459.8～467,467.7～470.6,535.6～540.8,583.8～591.4,654.4～659.8和670.8～680 nm等波段。     

非接触式可见光-近红外光谱法快速预测天然高分子材料表面粗糙度的研究

利用触针式轮廓法测量了天然高分子材料木材的表面粗糙度,并对可见光-近红外光谱与实测表面粗糙度参数之间的相关性进行研究,探讨了非接触式光谱法快速预测天然高分子材料表面粗糙度的可行性。结果表明：（1）样品三个切面的可见光-近红外光谱（400～2 500 nm）均可预测样品表面粗糙度,实测值与预测值相关系数可达0.92,其中利用样品横切面光谱所建的模型效果最好;（2）在分段光谱400～780 nm,780～1 100 nm,1 100～2 500 nm,780～2 500 nm,400～2 500 nm范围内,所建模型表面粗糙度参数的实测值与预测值相关系数可达0.80以上,显著相关,其中400～2 500 nm区域所建模型效果最好;（3）光谱预处理并不能提高模型预测效果,建议利用可见光-近红外光谱预测天然高分子材料表面粗糙度时采用原始光谱数据。     

LiF晶体中F3^＋—F2混合色心激光器

本文报道了室温下LiF晶体中F_3~+-F_2混合色心激光器.利用一块晶体和单一泵光,输出激光波长范围从510～580nm、640～710nm.总带宽140nm.     

常用合成食品色素荧光光谱研究

分析合成食品色素的分子结构特点,根据荧光与分子结构的关系,理论上推断合成食品色素是荧光物质。应用SP-2558多功能光谱测量系统,测得胭脂红、苋菜红、柠檬黄、日落黄、亮蓝等五种最常用的合成食品色素标准溶液的三维荧光光谱。结果表明,胭脂红在波长330～430 nm的光激发下,产生较强荧光,荧光峰值波长为621 nm,最佳激发波长为376 nm;苋菜红在波长300～440 nm的光激发下,产生较强荧光,荧光峰值波长为643 nm,最佳激发波长为370 nm;柠檬黄在波长280～380 nm的光激发下,产生很强荧光,荧光峰值波长为565 nm,最佳激发波长为315 nm;日落黄在波长310～410 nm的光激发下,产生较强荧光,荧光峰值波长为592 nm,最佳激发波长为348 nm;亮蓝在波长320～390 nm的光激发下,产生较强荧光,荧光峰值波长为456 nm,最佳激发波长为350 nm。进而对这五种合成食品色素的荧光光谱进行了分析讨论。结果可为食品色素检测和食品安全提供帮助。     

分段表面放电光抽运XeF(C-A)激光器

阐述了分段表面放电光抽运XeF(C -A)激光器的设计和实验技术。分段表面放电辐射源在 140nm～ 170nm辐射区域亮度温度Tb≈ 15× 10 3K ,用该辐射源作抽运源离解XeF2 获得了XeF(C -A)蓝绿 (4 70nm～ 495nm)激光输出 ,激光脉宽为 340ns、光谱宽度为 15nm。     

窄线宽1064 nm光纤激光泵浦高效率中红外3.8μm MgO:PPLN光参量振荡器

采用放大1064 nm掺镱光纤激光器作为泵浦源,实现了中红外3.8μm MgO:PPLN光参量振荡(OPO)激光输出。在泵浦源中,采用分布式反馈激光器(DFB)作为种子源来实现光纤激光窄线宽的调制,实现线宽2.5 nm到0.1 nm的压缩,最大平均输出功率可达40 W。进一步对不同泵浦线宽条件下中红外3.8μm MgO:PPLN OPO激光进行研究,最终在泵浦功率为18.1 W、线宽为0.1 nm、重频为1 MHz、脉宽为2 ns时,获得了最高平均输出功率为2.06 W的3822.5 nm激光输出,光-光转换效率为11.38%,光束质量为M2=2.34,提高了窄线宽泵浦对中红外MgO:PPLN OPO激光输出效率。     

1.57μm被动调Q光学参量振荡器

在半导体泵浦被动调QNd∶GdVO4/Cr4+∶YAG激光腔内,利用KTP晶体实现了高重复频率的内腔OPO的稳定运转。OPO其信号光转换效率为7%,斜效率为10.3%。当泵浦功率7.3W时,可获得平均功率为0.48W,重频15kHz,脉宽6ns,峰值功率达13KW的1570nm激光输出。     

High repetition rate mid-infrared generation with singly resonant optical parametric oscillator using multi-grating periodically poled MgO:LiNbO3

A high repetition rate mid-infrared singly resonant optical parametric oscillator (OPO) using MgO-doped multi-grating periodically poled LiNbO₃ (MgO:PPLN) is demonstrated. A 1064 nm Q-switched Nd:YVO₄ laser at 10 kHz repetition rate and pulse width of 17.8 ns was used to pump the OPO. The period of the quasi-phase matched (QPM) grating in the multi-grating MgO:PPLN chip varied from 25.5 to 31.5 μm in steps of 0.5 μm. This corresponds to the generation of a signal beam from 1.37 to 1.64 μm and an idler beam from 3.0 to 4.8 μm, respectively. A maximum signal power of 250 mW and idler power of 140 mW has been obtained with an input pump beam of power 1.92 W, for a grating period of 30.5 μm. A maximum optic-optic conversion efficiency of 20% and 7.4% in the idler has been observed. It has been observed that the output power increases as the period of the grating increases.     

高功率腔内双共振2μm光参量振荡器特性研究

报道了一种稳定的高功率双共振2?μm 光参量振荡器（OPO）. 该OPO使用调Q的线偏振全固态Nd∶YAG激光器作为抽运源,利用双棒串接补偿热致双折射和双Q开关正交放置技术提高了抽运源的输出功率和光束质量,通过腔内抽运单块KTP晶体实现了稳定的高功率2?μm 激光输出. 在调Q频率为5?kHz时,得到了295 W的2?μm 激光输出. 研究了OPO输出功率同KTP晶体温度和声光Q调制频率的关系,并测量了在29W时2?μm激光的功率稳定性. 在1 h内该OPO的功率起伏小于1.4%. 关键词： 光参量振荡器 2?μm激光器 KTP晶体 双共振     

Low-pump-threshold tunable optical parametric oscillator using periodically poled MgO:LiNbO3

We fabricated and characterized periodically poled MgO:LiNbO₃ device with five gratings in 0.5 μm increments from 29 μm to 31 μm for optical parametric oscillator (OPO). The OPO operation threshold is 30 μJ using this device with a 50 mm effective length. At 560 mW input pump power, we have achieved 300 mW of the total output power, and the conversion efficiency is 54%. Multi-periods and temperatures tuning of the OPO yields a signal wavelength range from 1.45 to 1.72 μm and an idler wavelength range from 2.8 to 4.05 μm in the mid infrared.     

Performance evaluation of ZnGeP2 optical parametric oscillator pumped by a Q-switched Tm,Ho:GdVO4 laser

A doubly resonant ZnGeP2 （ZGP） optical parametric oscillator （OPO） pumped by a novel Tm,Ho：GdVO4 laser was demonstrated. Cryogenic Tin（5 at.-%）, Ho（0.5 at.-%）：GdVO4 laser with high pulse repetition frequency （PRF） of 10 kHz at 2.05 μm was employed as pumping source of ZGP OPO. The 15-mm-long ZGP crystal, 55° cut for I-type phase-matching with low absorption coefficient less than 0.05 cm^-1 at 2 μm, was placed in a piano-piano cavity with resonator length of 30 mm. The ZGP OPO generated a total combined output power of 1.2 W at 3.75 and 4.52 μm under pumping power of 5.3 W, corresponding to slope efficiency of 40% from incident 2μm laser power to midinfrared （Mid-IR） output. A widely tunable range from 3.0 to 6.5 μm was achieved by changing the crystal angle only 3.5°.     

Efficient 1.8 μm KTiOPO4 optical parametric oscillator pumped within an Nd:YAG/SrWO4 Raman laser

A 1.8?μm optical parametric oscillator (OPO) based on a noncritically phase-matched KTiOPO4 crystal is demonstrated. OPO and stimulated Raman scattering techniques are successfully combined in an acousto-optically Q-switched Nd:YAG/SrWO4 Raman laser. The device efficiently realizes three steps of conversion: from a laser diode wavelength of 808?nm to the fundamental wavelength of 1064?nm; next, to the Stokes wavelength of 1180?nm; and finally to the OPO signal wavelength of 1810?nm. With an incident diode power of 7.2?W and a pulse repetition rate of 15?kHz, an average signal power of 485?mW is obtained with a diode-to-signal conversion efficiency of 6.75%. The beam quality factors (M2) of the signal wave in both horizontal and vertical directions are measured to be 1.7±0.2. The numerical output power results of the system, the thermal lensing, and the stability parameter of the cavity are also discussed.     

Mid-IR frequency comb source spanning 4.4-5.4 μm based on subharmonic GaAs optical parametric oscillator

Broadband mid-IR output suitable for producing 1000-nm-wide frequency combs centered at 4.9?μm was achieved in a degenerate subharmonic optical parametric oscillator (OPO) based on 500-μm-long Brewster-angled orientation-patterned GaAs crystal. The OPO was synchronously pumped at 182 MHz repetition rate by 100 fs pulses from a Cr2?:ZnSe laser with the central wavelength of 2.45?μm and the average power of 100 mW.     

Widely tunable, high-repetition-rate, dual signal-wave optical parametric oscillator by using two periodically poled crystals

This paper reports on a high-repetition-rate dual signal-wave (DSW) optical parametric oscillator (OPO) operating at the 1.5 μm band with tunable wavelength intervals from 2.5 nm to 69.1 nm. Two periodically poled crystals, a periodically poled lithium niobate (PPLN) with multiple gratings and a single grating MgO-doped PPLN (PPMgOLN), are cascaded in the same OPO cavity to generate dual signal-waves by using quasi-phase-matched (QPM) technique. The pump source was a Q-switched diode-pumped Nd:YVO₄ laser operating at 50 kHz. At an incident pump power of 3 W, an average output power of 169.6 mW at 1489.2 nm and 1558.3 nm has been achieved.     

A ring ZnGeP2 optical parametric oscillator pumped by a Ho:LuAG laser

We have demonstrated that we believe to be the first ring ZnGeP₂ (ZGP) optical parametric oscillator (OPO) pumped by a pulsed Ho:LuAG laser. The maximum output power of the ring ZGP OPO laser was 5.51 W at 13.1 W incident Ho pump power, corresponding to a slope efficiency of 59.0 %. The ZGP OPO laser produced 14 ns mid-infrared pulses in the 3.72–4.01 and 4.37–4.75 μm spectral regions simultaneously. In addition, the continuous wave Ho:LuAG laser generated 26.5 W of linearly output at 2,094.4 nm at the absorbed Tm pump power of 49.9 W.