皮秒激光微束仪的研制

本文分析了激光微束仪的设计要点,通光孔径的选取,聚焦系统与观察系统的齐焦,微小光斑获得等。激光微束仪的光源是具有多次谐波功能的皮秒Nd~(+3)YAG激光器,工作频率(10PPS),输出能量为50毫焦耳,平均脉宽为30PS的基波序列脉冲,可选波长为1.06μm、0.53μm、0.355μm、0.266μm,谐波晶体用偏硼酸钡(β-BaB_2O_4),简称BBO。     

强激光作用下生物组织光致破裂效应的研究

基于激光与生物组织作用时产生的光致破裂效应,利用脉冲激光直接聚焦于孕囊内的胚胎内部,激光产生的光致破裂效应对胚胎心脏造成损伤,造成胚胎的快速死亡,初步证明利用激光进行减胎手术有望成为一种新方法。采用输出波长1 064 nm、脉宽8 ns、单脉冲能量60～96 mJ可调的脉冲激光作用于牛肌肉组织样品,并用光学相干层析成像(OCT)系统测量实验样品的损伤直径和损伤深度,建立了不同的激光参数与被作用样品的损伤直径及损伤深度之间的关系。得出结论:样品的损伤深度和损伤直径与激光的脉冲能量成正相关关系,而与激光的脉冲频率成负相关关系。这对于激光应用于减胎手术时参数的优化和精确控制起到一定的指导作用。     

不同激光不同能量对红色毛癣菌的体外抑制评估及部分机制的探讨

目的探讨多种激光在不同的能量下对红色毛癣菌的体外抑制作用以及可能的作用机制。方法将Q开关Nd:YAG 532nm激光、Q开关Nd:YAG 1064nm激光、长脉宽Nd:YAG1064nm激光和强脉冲光分为不同能量组及未照光组,体外照射红色毛癣菌的菌落,观察第0、1、3、7天时菌落直径的变化差异,用酶联免疫吸附测定激光照射后红色毛癣菌产生角蛋白酶的活性。结果与未照光组相比,上述激光在低能量时对红色毛癣菌的菌落直径与角蛋白酶活性无明显影响。2～4J/cm~2能量Q开关Nd:YAG 532nm激光、4～8J/cm~2能量Q开关Nd:YAG 1064nm激光、4J/cm~2长脉宽Nd:YAG 1064nm激光能显著抑制菌落的生长,红色毛癣菌角蛋白酶的活性出现明显下降。结论 2～4J/cm~2能量Q开关Nd:YAG 532nm激光、4～8J/cm~2能量Q开关Nd:YAG 1064nm激光、4J/cm~2长脉宽Nd:YAG 1064nm激光能抑制红色毛癣菌生长及角蛋白酶的活性。     

脉冲1 064 nm激光视网膜损伤动物模型的建立

目的:建立脉冲1 064 nm Nd:YAG激光致视网膜出血性损伤及非出血性损伤动物模型,为治疗药物评价提供技术基础.方法:应用自由振荡脉冲及调Q脉冲1 064 nm激光照射青紫蓝灰兔视网膜,通过在光路中加人透镜获得直径200μm眼底光斑,加入衰减片改变角膜入射激光能量.照射即刻对损伤应用检眼镜进行实时观察,并用眼底相...     

1．06μm激光致皮肤痛觉效应的研究

目的：研究1．06μm激光所致人手背皮肤的痛觉效应。方法：以输出波长为1．06μm的脉冲Nd：YAG激光照射人手背皮肤,记录每次刺激激光的能量以及受试者的反应。采用加权概率单位算法计算诱发痛觉概率为50％时对应的激光剂量ED50,即为痛觉阈值。改变光斑大小和脉冲宽度,测定三种不同刺激条件下的痛觉阈值,并探索温度对激光所致痛觉效应的影响。结果：当皮肤温度约为30℃,分别使用光斑直径1．20mm、脉冲宽度85μs,光斑直径1．20mm、脉冲宽度20ns和光斑直径2．56mm、脉冲宽度20ns的激光刺激时,痛觉阈值分别为394mJ／mm^2、36．4mJ／mm^2和8．92mJ／mm^2。在第一种刺激条件下,当皮肤温度为25℃时,剂量为383mJ／mm^2的激光诱发痛觉的概率为16．7％;当皮肤温度为39℃时,剂量为361mJ／mm^2的激光诱发痛觉的概率为56．7％。结论：1．06“m激光所致痛觉的阈值随脉冲宽度的减小、光斑面积的增大和皮肤表面温度的增加而减小。     

氧化应激在长脉宽1064nm Nd: YAG激光治疗甲真菌病中的作用

目的探讨长脉宽1064nm Nd:YAG激光对引起甲真菌病的最常见致病菌-红色毛癣菌(Trichophyton rubrum)的体外抑制/杀灭作用及活性氧簇(ROS)介导的氧化应激反应在其中发挥的作用。方法改变长脉宽1064nm Nd:YAG激光脉冲数(7次脉冲、9次脉冲、11次、13次脉冲),固定其他参数照射红色毛癣菌菌落,绘制生长曲线,确定有抑制作用的最小脉冲数。在此脉冲数条件下干预红色毛癣菌菌落及孢子悬液,比较菌落形态学改变,检测孢子悬液相对活力的改变,同时检测ROS在不同处理后的表达水平变化。结果激光对红色毛癣菌的抑制/杀灭作用随能量的增加而增强,相对活力随时间的增加而下降,呈能量和时间依赖性;激光干预后,菌丝失去正常形态结构,孢子悬液的荧光强度及ROS含量较未照射的高,P=0.0157。结论长脉宽1064nm Nd:YAG激光体外对红色毛癣菌有抑制/杀灭作用,ROS介导的氧化应激反应可能在该激光治疗红色毛癣菌甲真菌病中发挥了一定的作用。     

超脉冲CO_2激光治疗睑缘分裂痣疗效观察

为评估超脉冲CO_2激光治疗睑缘分裂痣的疗效和不良反应。选取使用超脉冲CO_2激光治疗48例1至45岁患者,选择光斑直径(1 mm),能量(60～100 mJ)和脉宽(1 ms)进行治疗,治疗间歇期为3～6个月。经1～4次治疗后,13例治愈,22例显著消退,13例好转。治疗后出现2例感染,2例瘢痕,2例色素减退。结果表明超脉冲CO_2激光治疗睑缘分裂痣疗效显著,不良反应少。     

Q开关Nd:YAG 1064nm和532nm激光对犬心肌切割作用的研究

目的 :研究 10 64nm和 53 2nm波长激光在激光能量为 14 0mJ/pulse(脉冲 )时对犬心肌切割效率。方法 :用Q开关Nd :YAG 10 64和 53 2nm波长脉冲激光分别照射犬离体和在体心肌组织 ,光学显微镜和偏振光学显微镜行组织学分析 ,观察不同条件下激光切割组织的深度和光热对组织的损伤。结果 :离体和在体实验 ,10 64nm波长激光的切割效率高于 53 2nm(p <0 .0 1)。在体和离体实验显示 10 64nm激光能量和重复率相同时 ,所致的切割效率无明显差异 (p >0 .0 5) ,血液对 10 64nm激光的切割效率影响较小。相反 ,在 53 2nm时血液对其影响较大 ,相同的激光能量和重复率 ,离体实验切割效率高于在体 (p <0 .0 1)。 10 64nm激光所致的光热和机械损伤均轻于 53 2nm激光。结论 :在切割效率方面 ,10 64nm激光比 53 2nm更适用于TMLR。 10 64nmQ开关Nd :YAG激光可通过光导纤维传输 ,是TMLR的一个有潜力的激光源     

XeCl 准分子激光辐照生物大分子对其结构影响初步研究-Ⅰ308 nm紫外激光辐照小牛胸腺DNA的电镜观察与分析

XeCl 308 nm紫外激光(单脉冲输出能量33.4 mJ,脉冲频率 2次/秒,辐照时间45秒,光斑6×3 mm,透镜焦距300 mm)辐照330 mm处小牛胸腺DNA(固体).用扫描电子显微镜和透射电子显微镜可以观察到DNA受照射后有断裂、分叉、扭曲、聚集和交联等现象,影响生物大分子的初级结构和高级结构的变化.在我们的实验条件下是以影响DNA构象变化为主.     

Er:YAG激光脉宽对牙硬组织消融特性影响的研究

研究了Er:YAG激光消融离体牙本质过程中激光脉宽对消融阈值、消融深度以及消融后牙硬组织微结构的影响。使用50μs到1 ms脉宽的Er:YAG激光对人牙本质在无喷水冷却下消融实验,通过体式光学显微镜观察样品消融切口进而测量消融坑洞深度,利用扫描电镜(SEM)观察消融后牙本质的形态。实验结果表明,随着激光脉宽的增加,Er:YAG激光对人牙本质的消融阈值、消融深度呈现逐渐增大的趋势,同时还观察到高能量密度消融实验中牙小管封闭以及牙本质熔融现象。该实验结果对了解Er:YAG激光消融牙硬组织的微观过程及牙科治疗应用具有参考价值。     

应用Nd：YAG激光消除晶体后囊膜皱褶

目的：观察应用Ｎｄ：ＹＡＧ激光,消除人工晶体植入术后,影响视力的后囊膜皱褶之效果。方法：国产ＪＹＺ－１Ａ型ＹＡＧ激光眼科治疗机。用单脉冲能量０．３５ｍＪ－１．５ｍＪ,治疗总能量１１．２ｍＪ６４．５ｍＪ击射晶体后囊膜皱褶深处,形成３４ｍｍ孔径管亮区。     

Fluorescence enhancement monitoring of pyrromethene laser dyes by metallic Ag nanoparticles

Fluorescence enhancement monitoring of pyrromethene laser dyes using their complexation with Ag nanoparticles (Ag NPs) was studied. The size of the prepared Ag NPs was determined by transmission electron spectroscopy and UV/Vis absorption spectroscopy. Mie theory was also used to confirm the size of NPs theoretically. The effect of different nanoparticle concentrations on the optical properties of 1 × 10^‐4 M PM dyes shows that 40%of Ag NPs concentration (40%C Ag NPs) in complex is the optimum concentration. Also, the effects of different concentrations of PM dyes in a complex was measured. Emission enhancement factors were calculated for all samples. Fluorescence enhancement efficiencies depended on the input pumping energy of a Nd‐YAG laser (wavelength 532 nm and 8 ns pulse duration) were reported and showed the lowest energy (28 and 32 mJ) in the case of PM567 and PM597, respectively. Copyright © 2014 John Wiley & Sons, Ltd.     

A Study of the Effect of Terahertz Electromagnetic Radiation on Microbial Cell Viability

Biophysics - Abstract—The effect of pulsed terahertz radiation at a wavelength of 66 μm, a pulse duration of 100 ns, and a pulse energy of 200 mJ on a suspension of microbial cells was...     

Laser crosslinking of E. coli RNA polymerase and T7 DNA.

The first photochemical crosslinking of a protein to a nucleic acid using laser excitation is reported. A single, 120 mJ, 20 ns pulse at 248 nm crosslinks about 10% of bound E. coli RNA polymerase to T7 DNA under the conditions studied. The crosslinking yield depends on mercaptoethanol concentration, and is a linear function of laser intensity. The protein subunits crosslinked to DNA are beta, beta' and sigma.     

Photothermal sensitisation: evidence for the lack of oxygen effect on the photosensitising activity.

Irradiation of amelanotic melanoma B78H1 cells in the presence of liposome-delivered Ni(II)-octabutoxy-naphthalocyanine with a Q-switched Ti:sapphire laser operated in a pulsed mode (850 nm, 30 ns pulses, 10 Hz, 120 mJ pulse -1) promotes a photothermal sensitization process leading to extensive cell inactivation. The photoprocess occurs with identical efficiency in N2-saturated and air-equilibrated media, indicating that this photosensitization modality does not require the presence of oxygen.     

XeCl准分子激光辐照对溶菌酶结构的影响

利用荧光光谱、SDS-PAGE和NMR方法,考察308 nm XeCl准分子激光辐照对溶菌酶结构与活性的影响。使用能量密度为0.3 mJ/mm2的激光辐照溶菌酶,脉冲数分别为25、50、100、200、600、1200、1800、3600和7200。结果表明,用低强度激光辐照(低于200个脉冲)时,溶菌酶的活性出现增高趋势。随着激光辐照脉冲数的进一步增大,溶菌酶的活性又开始逐步降低。激光辐照处理后,溶菌酶的荧光强度发生了与生物活性相对应的先增高再降低现象,说明溶菌酶的高级结构发生了显著变化。SDS-PAGE结果显示,经激光辐照后,溶菌酶出现了分子间的聚合。分析溶菌酶的1H-NMR谱发现,辐照后,溶菌酶色氨酸(Trp)111、Trp63和Trp62的化学位移发生了变化,此结果进一步说明,激光辐照使溶菌酶的高级结构发生了变化。该实验可为激光辐照诱导蛋白质去折叠的研究提供参考。     

The energetics of the jump of the locust Schistocerca gregaria.

The anatomy of the metathoracic leg is redescribed with particular reference to storage of energy in cuticular elements and the way in which the stored energy is used in jumping. The jump of adult male locusts requires an energy of 9 mJ and that of the female requires 11 mJ. The semilunar processes of each metafemur store 4 mJ at a stress of 15 N, and the extensor tibiae apodeme stores a further 3 mJ at the same stress. The total stored energy in both metathoracic legs is 14 mJ. The extensor tibiae muscle produces a maximum isometric force of over 15 N at 30 degrees C and, when loaded with the extensor apodeme and semilunar processes, attains this force in 0.3 sec with a strain of 0.8 mm. The peak power output is 36 mW or 0.45 W.g-1. The peak isometric force is attained when the tibia is fully flexed and the force falls as the tibia extends. The extensor tibiae muscle A band is 5.5 mum long and the peak force is over 0.75 N.m-2. The peak velocity of shortening is 7 mm.sec-1 or about 1.75 lengths/sec at 30 degrees C. The tensile strength of the extensor apodeme is 0.6 kN.mm-2 and Young's modulus is 19 kN.mm-2. The safety factor does not exceed 1.2 and the safety factor of the semilunar processes and tibial cuticle is little higher. The jump impulse lasts 25-30 msec. A velocity of 3.2 m.sec-1 is reached after a peak acceleration of 180 m.sec-2. The peak power output is 0.75 W at close to maximum velocity. Energy losses in rotating the femur and tibia are small and it is shown that the leg is able to extend at 7 times the normal rate with losses of about 20%. Most of the stored energy is converted to kinetic energy as the animal jumps. A model is based on the relaxation of a spring that has the properties of the elastic elements of the locust leg into a lever with the same kinematics as the locust leg produces a force-distance curve similar to that measured for locust jumps. The major part of the jump energy is stored before the jump.