首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   9篇
  免费   3篇
数学   1篇
物理学   11篇
  2018年   2篇
  2017年   1篇
  2016年   1篇
  2013年   2篇
  2006年   1篇
  2005年   3篇
  2004年   1篇
  1997年   1篇
排序方式: 共有12条查询结果,搜索用时 15 毫秒
1.
A frequency stabilizing system for a pulsed injection seeded 1550 nm optical parametric oscillator(OPO) at 20 Hz repetition rate is demonstrated.The optical heterodyne method is used to measure the frequency difference between the seed laser and the OPO output.Using the frequency difference as the error signal,a proportionalintegral controller in combination with a scanner is applied to stably match the OPO cavity length to the seed laser frequency.The root-mean-square(rms) error of the frequency discrimination method is 0.07 MHz according to a ‘frequency shifting-chopping-beat' evaluation.The frequency fluctuation of the frequency-stabilized OPO is0.29 MHz(rms),and the Allan deviation is less than 20 k Hz for averaging time of more than 3 s.  相似文献   
2.
Polarization dependent loss (PDL) has been recognized as a critical issue because various inline optical components may have nonnegligible PDL effect that interacts with polarization mode dispersion (PMD). We investigated the impact of PMD-PDL interaction on degree of polarization (DOP), which is the most commonly used feedback signal in PMD compensation. The simulation results of a 40-Gb/s NRZ code optical transmission system show that the maximum PMD increases from approximately 40 ps to more than 45 ps, while minimum DOP declines from approximately 0.6 to approximately 0.2. The interaction of PMD and PDL also induces residual PMD underestimation of 5-8 ps, which causes degradation of PMD compensation performance.  相似文献   
3.
Polarization mode dispersion (PMD) is becoming major system impairment in high speed and long distance opti- cal fiber transmission systems. Since the PMD-induced pulse spreading is a frequency-dependent statistic pa- rameter and varies randomly over time, it is difficult to be compensated[1-3]. Large length of single mode opti- cal fiber is needed to generate certain amount of PMD in laboratory, and the PMD effect in the fiber varies slightly and slowly over time. Therefore, PMD emula- …  相似文献   
4.
A high-repetition rate master oscillator power amplifier pumped with laser diodes (LDs) is reported. An injection seeding single-frequency electro-optical Q-switched Nd:YAG laser is used as an oscillator, and a conductively cooled Nd:YAG zigzag slab with a bounce-pumped architecture is utilized as a power amplifier. Pulse energies of over 800 mJ at 1 064 nm and 400 mJ at 532 nm, corresponding to average powers of 200 and 100 W, respectively, are achieved with a 12.6-ns pulse width at 250 Hz. Output frequency fluctuations and single-frequency operation are further monitored. Experimental results reveal that the proposed system, which features a single-pass amplified configuration, is a promising design for space-based applications.  相似文献   
5.
A highly efficient laser system output at the H-β Fraunhofer line of 486.1 nm has been demonstrated. A high pulse energy single-frequency hybrid 1064 nm master oscillator power amplifier was frequency-tripled to achieve355 nm laser pulses, which acted as the pump source of the beta barium borate nanosecond pulse optical parametric oscillator. With pump energy of 190 mJ, the laser system generated a maximum output of 62 mJ blue laser pulses at 486.1 nm, corresponding to conversion efficiency of 32.6%. The laser spectrum width was measured to be around 0.1 nm, being in conformity with the spectrum width of the solar Fraunhofer line.  相似文献   
6.
We report the frequency dependence of polarization mode dispersion (PMD) in a PMD compensator based on six cascaded birefringent crystals separated by Faraday rotators. When all crystal axes are aligned, the device can compensate for the first-order PMD. However, if all crystal axes are coupled with arbitrary angles, it can compensate for high-order PMD. The variations of differential group delay and principal state of polarization with optical frequency are analysed. The PMD vector and Stokes components of the device versus wavelength are measured. The theoretical simulations agree well with the experimental results.  相似文献   
7.
随着半导体制造步入1xnm技术节点时代,调焦调平系统的测量精度达到几十纳米。在纳米尺度范围内,集成电路(IC)工艺对调焦调平测量精度的影响很大。提出一种基于光学三角法和叠栅条纹法的调焦调平测量技术,利用空间分光系统将两组位相差为π的叠栅条纹同时成像到两个探测器上,通过归一化差分的方法计算硅片高度,可有效降低调焦调平测量技术对IC工艺的敏感度,尤其是IC工艺导致的光强变化的敏感性。实验结果表明,该系统测量重复性精度为8nm(3σ),线性精度为18nm(3σ)。当测量光强变化达90%时,该测量技术引起的线性精度变化为15nm(3σ);当光强变化为65%时,线性精度变化小于1nm(3σ)。  相似文献   
8.
A Q-switched distributed Bragg reflector fiber laser using a graphene passive saturable absorber is proposed in a cavity consisting of a fiber Bragg grating and Faraday rotator mirror as end mirrors, together with a highly doped erbium-doped fiber as a gain source. The laser has a Q-switched threshold of about 28 mW and a tunable repetition rate of 10.4-18.0 kHz with varying pump power. The shortest pulse width obtained from the system is 3.7 μs, with a maximum pulse energy and peak power of 22.2 nJ and 3.4 mW, respectively.  相似文献   
9.
We report a new first-order polarization-mode-dispersion (PMD) compensator based on birefringent crystals and magneto-optic polarization controllers.The compensator shows the response time of 150μs,insertion loss smaller than 3dB,and maximum differential group delay of 44.6ps.Compared to the first-order PMD compensators reported so far,our PMD compensator exhibits fast response time,low insertion loss,compact size,broad bandwidth,and immunity to environmental vibrations.  相似文献   
10.
幂方根不等式   总被引:1,自引:0,他引:1  
笔者从一类数学现象中得出幂方根不等式,并给出一个证明,又推出条件正数组的对换律,还相应地就一些形式较复杂的命题建立.以及利用对换律使这类命题证明简单化,进行了一些初步研究.下分四个部分予以论述.1一类数学现象易证,2+398>20,近似计算可得;1+...  相似文献   
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号