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1.
应用激发态吸收增强瞬态热折射理论结合激发态折射理论研究了新型锌卟啉化合物Zn-porphyrin 中激发态吸收增强瞬态热折射与激发态折射间的相互竞争. 样品在不同脉宽激光激发下呈现自聚焦-自散焦间的转化. 当入射激光脉宽为4 ns时,激发态折射占主要地位,样品呈现自聚焦性质;当入射激光脉宽为8ns时,激发态吸收增强瞬态热折射占主要地位,激发态折射占次要地位,样品呈现自散焦性质.
关键词:
金属卟啉化合物
激发态折射
瞬态热折射 相似文献
2.
Cr4+:YAG crystal was used as a saturable absorber in an active-passive mode-locked Nd:YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of ~0.8 ns to 2.4 ns for a single pulse was obtained by using Cr4+:YAG crystals with the different initial transmissions, and there was a shortest pulse width. The mode-locking dynamic process of Cr4+:YAG crystal was discussed to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
3.
Cr4+∶YAG crystal was used as a saturable absorber in an active-passive mode-locked Nd∶YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of ~0.8 ns to 2.4 ns for a single pulse was obtained by using Cr4+∶YAG crystals with the different initial transmissions, and there was a shortest pulse width. The mode-locking dynamic process of Cr4+∶YAG crystal was discussed to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
4.
萘酞菁铅化合物的光限幅特性研究 总被引:6,自引:0,他引:6
应用调Q倍频ns/ps Nd:YAG脉冲激光,在波长为532nm,脉冲宽度为8ns,重复频率为1Hz的条件下,研究了溶于二甲基亚砜(DMSO)中的萘酞菁铅溶液的反饱和吸收和光限幅特性。实验表明,萘酞菁铅具有良好的光限幅特性,它的有效激发态吸收截面与基态吸收截面的比值约为15.21,大于萘酞菁铜。研究结果表明,萘酞菁铅的光限幅特性优于C60,激发态吸收是其主要的光限幅机理。实验结果证实了重原子效应可以通过增强系际跃迁而使三重态的反饱和吸收增强,从而提高光限幅的能力。 相似文献
5.
We report a novel method of determining the lifetimes of the high-lying excited singlet states of dye molecules in solution. The method is based on simulating the Z-scan technique with ground-state and excited-state absorptions of an incident laser pulse having Gaussian temporal and spatial distributions. This leads to the important finding that the use of laser pulses as long as tens of picoseconds can resolve subpicosecond lifetime. 相似文献
6.
7.
We present a theoretical study of temporal compression of a short-wavelength laser pulse predicted in a real, Doppler-broadened, atomic system. The compression is the result of the coherent control peculiarities of electromagnetically induced transparency-propagation dynamics. Numerical results are reported and discussed, showing a temporal compression of 2 orders of magnitude (from 10 ns to 100 ps) of a 106.7-nm laser pulse in argon atoms at room temperature. 相似文献
8.
Concentration dependent nonlinear refraction in chloroaluminum phthalocyanine/ethanol solution 下载免费PDF全文
Nonlinear refractive properties of chloroaluminum phthalocyanine
(CAP) in ethanol solution are studied using the Z-scan
technique with picosecond (ps) and nanosecond (ns) laser pulses at a
wavelength of 532 nm. A transition from self-focusing to
self-defocusing in CAP solution excited by 10 ns pulses is observed
during the decrease of its concentration. This transition is due to
co-existing excited-state refraction and transient thermal lensing
effects. The experimental results are described very well using
the rate-equation model and the theory of transient thermal
refraction in liquids. The refractive cross sections of the
excited-state are also obtained. 相似文献
9.
J. Zhang K. Sugioka T. Takahashi K. Toyoda K. Midorikawa 《Applied Physics A: Materials Science & Processing》2000,71(1):23-26
A new technique of dual-beam laser ablation of fused silica by multiwavelength excitation process using a 248-nm KrF excimer laser (ablation beam) coupled with a 157-nm F2 laser (excitation beam) in dry nitrogen atmosphere is reported. The dual-beam laser ablation greatly reduced debris deposition and, thus, significantly improved the ablation quality compared with single-beam ablation of the KrF laser. High-quality ablation can be achieved at the delay times of KrF excimer laser irradiation shorter than 10 ns due to a large excited-state absorption. The ablation rate can reach up to 80 nm/pulse at the fluence of 4.0 J/cm2 for the 248-nm laser and 60 mJ/cm2 for the F2 laser. The ablation threshold and effective absorption coefficient of KrF excimer laser are estimated to be 1.4 J/cm2 and 1.2᎒5 cm-1, respectively. 相似文献
10.
11.
Cr4+ : YAG crystal was used as a saturable absorber in an active–passive mode-locked Nd : YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of a single pulse was obtained from 0.8 to 2.4 ns by changing the Cr4+ : YAG crystal with different initial transmission, when there was the shortest pulse width. The mode-locking dynamic process of Cr4+ : YAG crystal was analyzed by the rate equations to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
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13.
采用无模激光器发射波长为330 nm的激光激发多色激光导星,需要考虑脉冲激光重频率、激光带宽、激光初始光斑直径以及大气透过率对回波光子数的影响.通过数值模拟,计算了高斯光束的脉冲激光和连续激光激发多色激光导星在实际大气中后向辐射330 nm和2207 nm波长的回波光子数.数值计算结果表明,在垂直发射和接收的情况下,当到达大气中间层的激光能量为1 W时,连续激光能够获得更多的回波光子数,并且回波光子数几乎无起伏.对于脉冲激光,提高脉冲激光重频率达到50 kHz以上时,多色激光导星330 nm的回波光子数随脉冲重频率的增加趋于有限值;当大气能见度小于5 km且大气相干长度为12.8 cm时,大约需要34 W以上的激光发射能量,才能获得满足使用自然星全倾斜探测的330 nm回波光子数.对于连续激光,相同情况下,大约需要20 W以上的激光发射能量. 相似文献
14.
A novel technique for two-dimensional measurements of soot volume fraction and particle size has been developed. It is based
on a combined measurement of extinction and laser-induced incandescence using Nd:YAG laser wavelengths of 532 nm and 1064 nm.
A low-energy laser pulse at 532 nm was used for extinction measurements and was followed by a more intense pulse at 1064 nm,
delayed by 15 ns, for LII measurements. The 532-nm beam was split into a signal beam passing the flame and a reference beam,
both of which were directed to a dye cell. The resulting fluorescence signals, from which the extinction was deduced, together
with the LII signal, were registered on a single CCD detector. Thus the two-dimensional LII image could be converted to a
soot volume fraction map through a calibration procedure during the same laser shot. The soot particle sizes were evaluated
from the ratio of the temporal LII signals at two gate time positions. The uncertainty in the particle sizing arose mainly
from the low signal for small particles at long gate times and the uncertainty in the flame temperature. The technique was
applied to a well-characterized premixed flat flame, the soot properties of which had been previously thoroughly investigated.
Received: 21 June 2000 / Revised version: 11 September 2000 / Published online: 7 February 2001 相似文献
15.
利用准分子激光等离子体技术,在紫外预电离XeCl准分子激光器上获得了最短1.58 ns的短脉冲激光输出。实验中分析了聚焦到薄膜表面的光束能量密度对所产生的等离子体密度的影响,并对不同等离子体密度及维持时间情况下脉冲压缩效果进行了讨论,给出了激光器谐振腔在稳定腔及非稳腔两种工作方式下的实验结果。激光器在稳定腔工作时,脉宽可压缩至2.87 ns;采用非稳腔结构时,在脉冲能量不变情况下减小聚焦光斑面积,提高入射到薄膜表面的能量密度,得到了最短1.58 ns的短脉冲激光输出。该技术适用于任何其它准分子器件。 相似文献
16.
The dynamic range of a picosecond visible streak camera has been improved by the combination of a plasma shutter and multishot averaging performed with a photoconductive switch sweep circuit. We use this technique to measure the contrast of a 100-fs laser pulse over 2 ns with a dynamic range of 7 orders of magnitude. 相似文献
17.
利用可饱和吸收半导体GaAs作为被动调Q元件和FP输出耦合镜,实现了半导体激光器(LD)抽运Nd:YVO4激光调Q运转,获得脉宽度为47ns,重复频率为1183kHz,平均功率为430mW,光束质量为M2=113的TEM00激光基横模输出,调Q抽运阈值为1700mW.并数值求解了含有GaAs被动调Q兼输出耦合的速率方程,分析了GaAs被动调Q机理以及脉宽宽度、重复频率、平均功率随抽运速率、腔长的变化关系,理论与实验结果相一致.为多功能综合型微型调Q固体激光器提供了简单有效的方法.
关键词:
被动调Q
输出耦合
GaAs 相似文献
18.
A.K. Sharma R.K. Patidar M. Raghuramaiah P.A. Naik P.D. Gupta 《Optics Communications》2011,284(19):4596-4600
A simple technique is presented to generate temporally flat-top shaped laser pulses using electro-optic modulator (Pockels cell). It involves splitting of input laser pulse into two halves of equal intensity and then stacking together with appropriate optical delay to get a temporally flat-top laser pulse. It also allows generation of other pulse shapes by varying the relative intensity, delay, and phase between two halves of the input laser pulse. Temporally flat-top laser pulses of duration ~ 9 ns have been generated using ~ 7 ns duration incident laser pulses from a flash lamp pumped Q-switched Nd:glass laser oscillator. The rise and fall-time of the shaped pulse is limited by speed of electro-optic switch (Pockels cell), which is ~ 2 ns in the present case. 相似文献
19.
We demonstrated a 1.91 μm pumped, injection-seeded Q-switched Ho:YAG laser operating at room temperature. By inserting two Fabry-Perot etalons into the laser cavity, single-frequency Tm, Ho:YAG seed lasing was achieved at a wavelength of 2090.9 nm, with a typical output power of 60 mW. Single-frequency, nearly transform-limited Q-switched operation of the Ho:YAG laser was achieved by injection seeding. The output energy of the single-frequency Q-switched pulse is 7.6 mJ, with a pulse width of 132 ns and a repetition rate of 100 Hz. We measured the pulse spectrum, half-width of which was 3.5 MHz, by a heterodyne technique. 相似文献