Laser Micro-beam Manipulation System for Cells

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Laser Micro-beam Manipulation System for Cells

This paper introduces a laser micro-beam system for cells manipulation. The laser micro-beam system comprises a laser scissors and a laser tweezers, which are focused by a Nd∶YAG laser and a He-Ne laser through a microscope objective, respectively. Not only the overall design of the laser micro-beam system is discussed, but also the design and choice of the critical components. A laser micro-beam system was constructed and anticipated experiment results were gained. Yeast cells can be successfully manipulated with the laser tweezers. Chromosomes can be successfully incised with the laser scissors.     

稳定耦合效率的沟槽结构半导体激光器

为了稳定半导体激光器激射光束在光纤传输过程的耦合效率,提出一种沟槽结构的半导体激光器,并对该结构激光器的光束、耦合效率及P-I特性进行研究。在普通条形半导体激光器的脊形区刻蚀了周期性的沟槽结构,来改善半导体激光器有源区的增益分布。通过对比普通结构与沟槽结构半导体激光器的光束分析,测试其耦合效率以及P-I特性。结果表明:沟槽结构的半导体激光器能够使光腔内模式更加稳定,输出光束更加集中,并避免了"Kink"效应的发生;与此同时,耦合效率提高至97.7%,并且较普通结构激光器更为稳定。沟槽结构半导体激光器有效地解决了光斑跳动问题,稳定了激光器的耦和效率。     

激光无铅钎焊速度的影响因素(英文)

为了提高激光无铅钎焊的速度,对影响激光无铅钎焊速度的因素(如激光的参数、所用钎料和基体的特性、钎焊的系统结构等)进行了分析研究。研究认为,在激光器、钎料及基体等已定的情况下,相对于那些受到机械惯性制约的移动激光加工头或移动工作台的激光钎焊系统,一种配备了振镜扫描系统和f-theta聚焦透镜的激光钎焊系统具有更高的钎焊速度。另外,对激光钎焊过程中激光束的扫描路径进行了优化,这种优化能在不增加硬件成本的基础上大大缩短总扫描路程,较大程度地提高激光钎焊速度。最后通过实例对激光钎焊的快速性进行了验证。     

Ar+激光和532 nm激光及其线偏振激光辐照光学模型下人正常小肠组织光学特性

采用双积分球系统和光辐射测量技术的基本原理以及运用生物组织的光学模型 ,研究了 4 76 5 ,4 88,4 96 5 ,5 14 5 ,5 32nm激光及其线偏振激光辐照人正常小肠组织的光学特性。结果表明 :组织对激光及线偏振激光的衰减系数和散射系数随着波长的减小而增大 ,而 5 14 5～ 5 32nm波长之间 ,线偏振光与非线偏振光入射则开始有明显差异。吸收系数是随着波长的减小而缓慢地增大 ,而 5 14 5～ 5 32nm波长之间吸收系数的改变则明显变小 ,与是否线偏振光入射无明显差异。平均散射余弦也是随着波长的减小而增大 ,光学穿透深度则是随着波长的增大而增大 ,折射率在这五个波长范围内的值在 (1 38～ 1 4 8)之间。Kubel ka Munk二流模型下组织对同一波长的激光及其线偏振激光的吸收系数、散射系数、总衰减系数、有效衰减系数没有显著性差异 (P >0 0 5 )。组织对不同波长的激光或其线偏振激光的吸收系数、散射系数、总衰减系数、有效衰减系数是有差异的。而在 5 14 5～ 5 32nm波长之间其光学特性参数有较为明显的差异。     

射频板条CO2激光器输出光束的光学变换

射频激励板条CO2激光器输出激光近场光斑近似为一条线,远场光斑为O形图样。在垂直于光束传输方向的平面内,光束在一个方向发散很大,无法用于激光加工。根据激光器不同的激光功率级别及光束尺寸,分别采用了圆柱面镜、滤波光阑、扩束望远镜等不同组合的方法,将200 W激光器输出光束变换成远场光束为Φ6、近似TEM00模的圆形光束,500 W激光器远场光束为Φ10的低阶模的圆形光束。成功用于激光切割。     

10 ps High Power Laser System at 248 nm

1　Ｉｎｔｒｏｄｕｃｔｉｏｎ　　Ｉｎｒｅｃｅｎｔｙｅａｒｓｔｈｅｒｅｈａｓｂｅｅｎａｎｉｎｔｅｎｓｉｖｅｅｆｆｏｒｔｄｉｒｅｃｔｅｄｔｏｗａｒｄｔｈｅｐｒｏｄｕｃｔｉｏｎｏｆｓｈｏｒｔｐｕｌｓｅ,ｈｉｇｈ ｐｏｗｅｒＵＶｌａｓｅｒｓｙｓｔｅｍｓ .ＫｒＦｌａｓｅｒ,ｗｉｔｈｉｔｓ～ 2ｎｍｂａｎｄｗｉｄｔｈ ,ｈｉｇｈｅｌｅｃｔｒｉｃａｌ ｔｏ ｏｐｔｉｃａｌｃｏｎｖｅｒｓｉｏｎｅｆｆｉｃｉｅｎｃｙａｎｄｉｔｓｕｎｂｏｕｎｄ ｇｒｏｕｎｄｓｔａｔｅ ,ｉｓａｎａｔｔｒａｃｔｉｖｅｃａｎｄｉｄａｔｅｆｏｒｔｈｅ…     

All-solid-state narrow-linewidth 455-nm blue laser based on Ti:sapphire crystal

A compact, all-solid-state, narrow-linewidth, pulsed 455-nm blue laser based on Ti：sapphire crystal is developed. Pumped by a 10-Hz, frequency-doubled all-solid-state Nd：YAG laser and injection-seeded by an external cavity laser diode, the narrow-linewidth 910-nm laser with pulse width of 20 ns is obtained from a Ti：sapphire laser. 3.43-mJ blue laser can be obtained from the laser system by frequency-doubling with BBO crystal. This research is very useful to determine the roadmap of developing the practical, high power blue laser. This kind of laser will have potential application for underwater communication.     

An investigation of pulsed laser cutting of titanium alloy sheet

Subsequent welding requirement calls for high-quality laser cut surfaces in the laser cutting of bladed ring parts for aeroengines. This paper presents pulsed laser cutting of titanium alloy sheet and investigates the influences of laser cutting parameters on laser cut quality factors including heat-affected zone (HAZ), surface morphology and corrosion resistance. The thickness of HAZ lasers is studied in detail as a function of laser cutting parameters. For different assist gases the surface morphology and corrosion resistance show great differences. In comparison with air- and nitrogen-assisted laser cutting, argon-assisted laser cutting comes with unaffected surface quality and is suitable for laser cutting with subsequent welding requirement.     

激光光斑形状和尺寸对扫描显示中散斑对比度的影响

计算了圆形、矩形激光光斑对于激光扫描显示系统中散斑对比度的影响.对于圆形光斑,当光斑尺寸大于散射表面相关长度时,得到的散斑对比度随着光斑尺寸变小而下降;当光斑尺寸接近表面相关长度大小时,由于光斑中包含的散射颗粒变少,得到的是非高斯散斑,散斑的对比度反而会变大;随着激光斑进一步变小,由于镜面反射效果散斑的对比度会很快下降.对圆形光斑部分结果给出了实验验证.为了保证光斑中有足够的散射颗粒,只在一个方向压窄光斑,分别计算了平行于扫描方向和垂直于扫描方向压窄光斑得到的散斑对比度.平行于扫描方向压窄光斑,散斑的时间相关性会下降,平均效果变明显,散斑的对比度变小;垂直于扫描方向压窄,散斑对比度变化不大.     

5个不同波长的激光及其线偏振激光辐照人正常膀胱组织光学特性

采用双积分球系统和光辐射测量技术的基本原理以及运用生物组织的光学模型,研究了476.5, 488, 496.5, 514.5和532 nm激光及其线偏振激光辐照人正常膀胱组织的光学特性。结果表明：组织对激光及线偏振激光的总衰减系数和散射系数均随着波长的增大而减小,而且线偏振激光与非线偏振激光入射是有明显的差异。吸收系数是随着波长的增大而缓慢地减小,但有一些起伏,而与是否线偏振光入射无明显差异。平均散射余弦也是随着波长的增大而减小,而且线偏振激光与非线偏振激光入射是有明显的差异。光学穿透深度则是随着波长的增大而增大,而有一些起伏。折射率在这5个波长范围内的值在(1.37～1.44)之间。Kubelka-Munk二流模型下组织对同一波长的激光及其线偏振激光的吸收系数、散射系数、总衰减系数和有效衰减系数没有显著性差异(P＞0.05)。组织对不同波长的激光或其线偏振激光的吸收系数、散射系数、总衰减系数和有效衰减系数则有些是有明显的差异。     

10 ps High Power Laser System at 248 nm

A simple 10 ps KrF laser system consisting of quenched dye laser oscillator pumped by a XeCl laser, a distributed feedback dye laser (DFDL), a three-stage dye amplifier and a two-stage KrF amplifier are described. The output of the laser system is 140 mJ with 10 ps pulse width by using polarization-multiplexing amplification. A focused output laser intensity of about 4×1015 W/cm2 is obtained. The saturation fluence for KrF laser is obtained with this laser.     

半导体泵浦铷蒸气激光器出光实验

针对中心波长780 nm的商用连续波半导体激光器,使用斩波器将连续激光变为脉冲输出形式,用2400 line/mm的平面全息光栅搭建Littrow外腔将线宽压窄至0.2 nm以下。采用透镜组对线宽压窄后的半导体激光进行光束整形,半导体激光经线宽压窄和光束整形后,经透镜聚焦进长约8 mm的铷蒸气泡进行半导体泵浦碱金属激光实验。首次出光得到17.5 mW的基模线偏振铷激光;在最新的改进实验中,半导体泵浦铷激光输出功率已达到2.8 W。     

单CCD彩色相机激光干扰模型及外场干扰实验

开展了多波段激光(750~970 nm)对彩色CCD成像系统的外场干扰实验,测得了不同辐照条件下对外场1.3 km处彩色CCD成像系统的干扰效果;建立了彩色CCD相机的激光干扰模型,对实验结果进行了理论验证与分析。理论与实验结果表明:强激光对彩色CCD成像系统的干扰效果明显,CCD靶面出现了明显的光饱和和串扰现象,光饱和区域的形成是由激光束进入光学系统后发生衍射效应造成的;到靶激光功率密度越强,CCD靶面光饱和面积越大,激光干扰效果越好;单波段750 nm激光作用下,到靶功率密度为4.2 kW/cm²,CCD靶面的光饱和面积为0.88 mm×0.97 mm;多波段激光(750~970 nm)作用下,到靶功率密度为20.7 kW/cm²,CCD靶面发生全靶面饱和现象;仿真结果与实验结果基本一致,证明了理论模型的正确性。对远场干扰能力计算结果表明:随着干扰距离的增加,到靶功率密度减小,激光干扰效果变差。     

An excimer laser pumped atomic iodine laser emitting pulses in the range of 2–12 ns

An iodine photodissociation laser is pumped with a laser pulse from a XeCl or a KrF laser. Single smooth laser pulses with a duration variable from 2.6 to 12 ns are emitted by the iodine laser. A pulse power of 0.5 MW is obtained with diffraction limited beam divergence.     

Effects of Pulse Durations on High-order Harmonic Generation

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A comparative study on diode-pumped single-frequency Tm:YAG and Tm:GdVO<Subscript>4</Subscript> lasers

In this paper, we present experimental results concerning on the laser characteristics of Tm:YAG laser and Tm: GdVO₄ laser. At room temperature, the maximum output power of Tm:YAG laser and Tm:GdVO₄ laser is 210 and 145 mW, respectively. High efficiency can be achieved for both lasers at room temperature. Nevertheless, compared with Tm:GdVO₄ laser, Tm:YAG laser can operate on single frequency with high power easily. As much as 60 mW of 2013.9 nm single-longitudinal-mode (SLM) laser was achieved for Tm:YAG laser. For Tm:GdVO₄ laser 51 mW of 1919.7 nm SLM laser was achieved. The SLM Tm:YAG laser is better for using as a seed laser for coherent wind measurements and differential absorption LIDAR systems.     

种子注入的短脉冲激光器特性研究

 从LD泵浦固体激光器优化设计原则出发，设计了一种微型二极管泵浦激光器，并对种子激光器的结构和参数进行了优化。该激光器运转稳定，输出光束质量高，光束发散角小，光-光转化效率为17-4%，斜率效率可达24%，输出功率可达80mW。将此种子激光注入到调Q激光器中，改善了调Q激光器的输出特性，使得激光脉冲的建立时间缩短了40ns，输出的横模场分布得到了明显改善。     

连续和重复频率激光对旋转壳体加热效率的数值模拟

 基于有效利用激光能量的目的，采用有限元分析方法分析并比较了重复频率和连续激光对旋转壳体的加热效率。数值计算结果表明：重复频率激光要比连续激光的加热效率高，而且加热效率与重复频率、占空比等有关；在平均功率密度相同的前提下，在频率相同条件下，占空比减小，温度上升加快，即加热效率随占空比的减小而增大；在相同占空比条件下，重复频率越小温度周期变化越明显，振荡峰值越大，当占空比较小时随着辐照时间的增加重复频率对加热效率影响减小。     

An intermittent frequency offset lock of a transverse Zeeman laser to an iodine stabilized He-Ne laser

A single-mode frequency stabilized laser with modulation-free and moderate power is desired as a light source for an ultra-high resolution interferometer system and/or a rapid laser calibration system. For this purpose, we developed a new stabilized laser system that utilizes intermittent control of a 2 mW transverse Zeeman stabilized He-Ne laser (Zeeman laser) with an iodine stabilized He-Ne laser (I2 stabilized laser). Because of the intermittent control, working time of the I2 stabilized laser is reduced. The Zeeman laser has two operational modes: independent and slave mode. In the independent mode, the Zeeman laser is stabilized through control of Zeeman beat frequency. Temperature dependent drift of the oscillation frequency during the independent mode is periodically corrected by the slave operation utilizing frequency offset locking to the I2 stabilized laser. Frequency instability of the Zeeman laser in independent and slave modes is 7.7X10-11 and 2.0X10-11, respectively, at the sampling time of 100 s.