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本文系统制备了980nm半导体崩浦的应用于1.54μm波段微片激光器的高Er^3 /Yb^3 共掺杂的氟铝酸盐玻璃。通过玻璃的吸收光谱,发射光谱和上转换荧光光谱的测试,对其光学性质、浓度淬灭及其淬灭机制进行了分析和讨论。当玻璃中Er^3 离子掺杂浓度低于10mol%的情况下,浓度淬灭现象较弱,Er^3 /Yb^3 共掺杂的氟铝酸盐玻璃在由于Er^3 离子^4 I13/2→4^I 15/2跃迁所引起的1.54μm波段的发射强度比Er^3 单掺杂的氟铝酸盐玻璃中的荧光强度要强。在Er^3 离子掺杂浓度高于10mol%的情况下,由于Er^3 与Yb^3 之间的反能量转移过程,Er^3 /Yb^3 共掺杂的氟铝酸盐玻璃的1.54μm波段的荧光浓度淬灭效应比Er^3 离子单掺杂的情况下明显。在Er^3 离子掺杂浓度小于10mol%的情况下,实验中发现可获得1.54μm波段高发射效率的Er^3 与Yb^3 离子最佳摩尔浓度掺杂比例约为1:1。 相似文献
104.
The conformational transformation of a 30-residue peptide H(Ala-Gly-Ser-Gly-AIa-Gly)5OH, i.e., (AGSGAG)5, extracted from highly crystalline region of Bombyx mori (B. mori) silk fibroin was described by using the high resolution solid state 13^C NMR, and CD spectroscopies. Based on the conformation-dependent 13^C NMR chemical shifts of the Ala, Gly and Ser residues and the line-shape analysis of the conformation sensitive Ala Cβ resonance, the peptide revealed a strong preference for silk Ⅱ structural form, i,e,, an antiparallel fl-sheet structure (φ= - 140±20°and ψ= 135±20°) in solid state. On the contrary, the CD spectra of this peptide in the two non-native hexafluorinated fibre spinning solvents, hexafluoroisopropanol (HFIP) and hexafluoroacetone (HFA), exhibited the existence of an unusual tightly-folded conformation resembling 310-helix (φ=- 60±20° and ψ=-30±20°), as judged from the R ratio of [θ]222/[θ]203 in HFIP solution, whereas a dynamically averaged unordered structure in HFA, Taken together, the information inclined to hypothesis that the primary structure of the highly crystalline regions of B. mori silk fibroin may be easily accessible to the large conformational changes, which in turn may be critical for facilitating the structural transformation from unprocessed silk fibroin (silk I form) to processed silk fiber (silk Ⅱform). 相似文献
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横向激励大气压(transversely excited atmospheric,TEA)CO2激光器的放电稳定性是决定该类型激光器应用效果的关键因素。通过对采用电感充放电电路的紫外预电离激光器的实验研究,得到了激光器放电动态过程的规律,并发现残余振荡是主放电后发生弧光放电的主要原因。实验中采用不同配比的气体,并对电感充放电电路与改进后的硅堆充放电电路进行了比较。实验结果表明:增加充电电感值可以降低主放电结束后储能电容上的残余电压;而采用硅堆放电电路在主放电后仅有相对幅值很低的稳定残压,两种方案都大幅度抑制了弧光放电的形成,有效地提高了激光单脉冲能量。 相似文献
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《化学物理学报(中文版)》2013,(6):I0002-I0002
Chemical kinetics and reaction dynamics, as a crucial branch of physical chemistry, mostly concerns with the "how, why and when" of chemical reactions, which is not only an exciting intellectual frontier but also addresses grand societal needs. These two aspects promote rapidly developing a series of experimental techniques, including ultrafast lasers, high resolution mass spectrometry and optical spectroscopy, and crossed molecular beam etc. Thanks to the rapid development of computer sci- ence, nowadays it is possible to calculate the reaction rates of complex reaction systems by advanced statistical kinetic theories based on accurate potential energy surfaces, 相似文献
109.
Jiancong Du Suhui Deng Shangguo Hou Lingling Qiao Jianfang Chen Qing Huang Chunhai Fan Ya Cheng Yun Zhao 《中国光学快报(英文版)》2014,12(4):41101-38
DNA tetrahedral nanostructures are considered to be uew nanocarriers because they can be precisely controlled and hold excellent penetration ability to the cellular membrane. Although the DNA tetrahedral nanostructure is extensively studied in biology and medicine, its behavior in the cells with nanoscale resolution is not understood clearly. In this letter, we demonstrate superrcsolution fluorescence imaging of the distribution of DNA tetrahedral nanostructures in the cell with a simulated emission depletion (STED) microscope, which is built based on a conventional eonfocal microscope and can t)rovide a resolution of 70 nm. 相似文献
110.
We demonstrate a switchable Q-switched and mode-locked erbium-doped fiber laser (EDFL) operating in the L-band region using the nonlinear polarization rotation effect. The switching operation is achieved by controlling intensity-dependent loss using a polarization controller. In Q-switching mode, the EDFL produces a pulse train with a repetition rate of 21.1 kHz, pulse width of 7.7 #s, and pulse energy of 13.6 nJ. The EDFL also generates a multi-wavelength comb with a very narrow and constant wavelength spacing of 0.045 nm and optical signal-to-noise ratio of at least l0 dB. During mode locking, the EDFL produces stretched pulses with 3-dB bandwidth of 26.2 nm, pulse width of 350 fs, repetition rate of 2.38 MHz, and pulse energy of 48.56 pJ. 相似文献