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second harmonic light
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  倍频光
     In order to study the feasibility of submicron lithography using second harmonic light of a copper vapor laser(CVL), a 1∶1 catadioptric projection lens, and an illumination system which consists of a rotating diffuser and a ligth pipe, are designed and constructed. A resolution of 0.6 μm line/space patterns is produced in AZ1350 resist.
     为了研究波长为255.3nm的铜蒸气激光倍频光在亚微米光刻中的可行性,设计了带宽为1nm的11折反射式投影光刻物镜和一个带散射板的光管式均匀照明系统,获得了0.6μm的光刻分辨率。
短句来源
     The result shows that the second harmonic light of CVL can be used as an illumination source in submicron lithography.
     此结果表明,铜激光倍频光可作为亚微米光刻的照明光源
短句来源
  “second harmonic light”译为未确定词的双语例句
     Submicron Projection Lithography with Second Harmonic Light of Copper Vapor Laser
     铜激光倍频光亚微米投影光刻系统的设计和实验研究
短句来源
     SECOND HARMONIC LIGHT EMISSION FROM PLASMAS PRODUCED WITH SMOOTHED 1. 05μm LASER
     束匀滑激光照射下等离子体二次谐波特性研究
短句来源
     THE STUDIES ON THE PROPERTIES OF THE SPECTRAL PEAKS FOR THE SECOND HARMONIC LIGHT THROUGH THE FERROELECTRIC DOMAINS CONSTRUCTED FOLLOWING THE FIBONACCI-CLASS QUASILATTICE SEQUENCE
     按斐波那契类准周期序列排列的铁电畴超晶格二次谐波谱峰性质研究
短句来源
     SECOND HARMONIC LIGHT EMISSION FROM PLASMAS PRODUCED WITH 1.053μm LASER
     1053μm激光打靶产生的二次谐波
短句来源
     Bloembergen et al. First we determined the second harmonic light intensity of single domain LiNbO3 crystals in the regime eω ·eωe→e2ω. Then by using angle-scanning and temperature-scanning, we obtained the maximum second harmonic output from crystals with periodic domains corresponding to quasi-phase-matching.
     首先运用Maker条纹法在实验上直接测定了单畴LiNbO_3晶体在e~ω·e~ω→e~(2ω)非位相匹配下的倍频光强,并采用角度扫描和温度扫描方法,以获得满足准位相匹配条件时的不同片数的聚片多畴晶体的最大倍频强度,从而验证了聚片多畴晶体倍频相对光强与片畴数N成平方关系。
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  相似匹配句对
     Second .
     二、破自造论。
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     Second,
     二是对于?
短句来源
     On the Nondiffvacting Second Harmonic Beam
     非衍射的二次谐波
短句来源
     THE DIFFRACTION AND WALKOFF IN THE SECOND HARMONIC GENERATION
     二次谐波转换中的衍射和离散效应
短句来源
     Harmonic and Administration
     谐波及其治理
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  second harmonic light
Second harmonic light generation in a nonlinear medium with random nonuniformities
      
In addition, we found that the absorption edge of BNPM was 430 nm with a 0.9-mm-thick crystal, and we observed the second harmonic light with BNPM single crystal at the wavelength of 1064 nm and in the range from 906 nm to 990 nm.
      
The intensity of second harmonic light (532?nm) increased with angle of incidence and indicated the polar order in the plane of the film.
      
The angular dependence of the observed second harmonic light in films of well-defined symmetry is consistent with second harmonic generation originating in the bulk.
      
Second harmonic light scattering in paraelectric perovskites
      
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We studied the second harmonic generation of light in LiNbO3 crystals with periodic laminar ferroelectric domains, in order to make a detailed experimental verification of the theory of quasi-phase-matching proposed by N. Bloembergen et al. First we determined the second harmonic light intensity of single domain LiNbO3 crystals in the regime eω ·eωe→e2ω. Then by using angle-scanning and temperature-scanning, we obtained the maximum second harmonic output from crystals with periodic domains...

We studied the second harmonic generation of light in LiNbO3 crystals with periodic laminar ferroelectric domains, in order to make a detailed experimental verification of the theory of quasi-phase-matching proposed by N. Bloembergen et al. First we determined the second harmonic light intensity of single domain LiNbO3 crystals in the regime eω ·eωe→e2ω. Then by using angle-scanning and temperature-scanning, we obtained the maximum second harmonic output from crystals with periodic domains corresponding to quasi-phase-matching. We have verified experimentally the relation that the second harmonic output is proportional to N2(N is the number of domains in the crystal) with N up to 200. We have compared the second harmonic output of crystals with periodic laminar domains in the quasi-phase-matching regime with that of single domain crystals of the same length and optical quality under phase-matched condition oω· 0ω→e2ω. An order of magnitude enhancement of second harmonic light output has been found. Finally, the structure sensitivity of the second harmonic generation of LiNbO3 crystal with periodic laminar ferroelectric domains has also been studied experimentally.

通过对聚片多畴LiNbO_3晶体倍频效应的研究,从实验上对Bloembergen等人所提出的准位相匹配理论进行了细致的检验。首先运用Maker条纹法在实验上直接测定了单畴LiNbO_3晶体在e~ω·e~ω→e~(2ω)非位相匹配下的倍频光强,并采用角度扫描和温度扫描方法,以获得满足准位相匹配条件时的不同片数的聚片多畴晶体的最大倍频强度,从而验证了聚片多畴晶体倍频相对光强与片畴数N成平方关系。在N<200时,取得令人满意的结果。把聚片多畴晶体的倍频光强与同质量同长度单畴晶体在o~ω·o~ω→e~(2ω)位相匹配下的倍频光强进行比较,其倍频强度提高一个数量级之多。最后,还从实验上讨论了倍频增强效应的结构敏感性。

The properties of Nd:YVO4 solid-state laser pumped with a Ti:sapphire laserhave been investigated. The output power of 190 mW and the pump threshold of 13 mWhave been obtained where the optical slope efficiency was 51%. The output power of 10mW for the second-harmonic light was observed using an intracavity KTP crystal,and thetotal optical efficiency was 2.3%.The dependence of the output power on the pumpwavelength ranging from 740nm to 830 um is given.

研究了用钛蓝宝石激光泵浦的Nd:YVO4固体激光器的特性。得到基频连续激光输出功率为190mW,泵浦阈值为13mW,光学斜效率为51%。用KTP晶体腔内倍频,得到二倍频激光输出功率为10mW,总的光学转换效率为2.3%。给出了泵浦光波长(740~830um)与激光输出功率之间的关系。

In order to study the feasibility of submicron lithography using second harmonic light of a copper vapor laser(CVL), a 1∶1 catadioptric projection lens, and an illumination system which consists of a rotating diffuser and a ligth pipe, are designed and constructed. A resolution of 0.6 μm line/space patterns is produced in AZ1350 resist. The result shows that the second harmonic light of CVL can be used as an illumination source in submicron lithography.

为了研究波长为255.3nm的铜蒸气激光倍频光在亚微米光刻中的可行性,设计了带宽为1nm的11折反射式投影光刻物镜和一个带散射板的光管式均匀照明系统,获得了0.6μm的光刻分辨率。此结果表明,铜激光倍频光可作为亚微米光刻的照明光源

 
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