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1.
Compression of chirped free femtosecond pulses in hollow-core photonic bandgap fibers is investigated numerically. The results show that intrapulse stimulated Raman scattering can improve the quality of the compressed pulse. Positive third-order dispersion is the main limitation on the compression of the femtosecond pulse. However, the combined effect of the intrapulse stimulated Raman scattering and the negative third-order dispersion can form still shorter pulses than is possible with intrapulse stimulated Raman scattering alone. We also investigate the influence of width and peak power of input pulse on pulse compression.  相似文献   

2.
基于在正常色散渐减光纤(ND-DDF)或者正常色散光纤放大器,获得线性啁啾抛物线脉冲,提出并分析了利用ND-DDF放大器获得线性啁啾抛物线脉冲的优化方案.数值研究结果表明:与用ND-DDF或者正常色散光纤放大器获得线性啁啾抛物线脉冲的方案相比,利用ND-DDF放大器获得的抛物线脉冲的线性啁啾更为明显;研究还发现,增益影响着线性啁啾的大小和质量.计算表明,利用ND-DDF放大器产生的抛物线脉冲经啁啾补偿后可获得更大的压缩因子和更高的峰值功率.  相似文献   

3.
提出了利用一种高非线性微结构光纤构成非线性光纤环镜(NOLM)进行脉冲压缩和基座抑制的方案.所提出的微结构光纤具有高非线性系数和大反常色散.理论研究了基于这种微结构光纤的NOLM对脉冲的压缩效应,并分析了压缩的机制.数值结果表明,这种NOLM采用较短的光纤长度就能有效地压缩脉冲并明显抑制了基座.对于给定的输入脉冲,存在一个最优的环路长度,可以获得高质量的压缩脉冲.通过适当选择耦合比和环路长度,则可以完全消除脉冲的基座.  相似文献   

4.
Yingchun Ding  Lei Bao  Jiaojiao Li 《Optik》2011,122(24):2172-2175
The pulse compression effect in SBS light storage is numerically investigated. We demonstrate theoretically that the compressed width of retrieved data-pulses is not only related with temporal profile of data-pulse, but also spectrum and temple profile of control-pulse. The data-pulses with steep rising edge can be compressed after they are retrieved. The optimum compression effect takes place when a 2-ns-long exponential data-pulse interacts with a 1.5-ns-long chirped Gaussian control-pulse, where the data-pulse width is compressed to 1.73-ns-long and the readout efficiency is the biggest. A 2-ns-long rectangular data-pulse is also compressed to 1.73-ns-long when it encounters to a 1.5-ns-long rectangular control-pulse, but the readout efficiency isn’t maximum value. The results are significant for increasing storage capacity and variable bits all-optical buffering.  相似文献   

5.
色散渐减光纤的脉冲压缩研究   总被引:7,自引:0,他引:7       下载免费PDF全文
介绍了色散渐减光纤的绝热孤子压缩(ASC)过程,分析结果表明利用线性渐减的色散渐减光 纤(DDF)对飞秒基态孤子进行绝热压缩可以得到高质量的压缩脉冲,但用于压缩的DDF长度很 长,因此又提出DDF的高阶孤子(1<N≤21)脉冲压缩技术,以在较短的DDF长度下获得 较大压缩比和高质量的压缩脉冲. 关键词: 色散渐减光纤 绝热孤子压缩 脉冲压缩 高阶孤子  相似文献   

6.
Based on the space-time duality and the temporal imaging theory, an optical implementation of the Radon-Wigner transform in the time domain is proposed for analyzing the propagation of ultrashort light pulses in guided dispersive media. As an application of this approach, we discuss the temporal selfimaging or Talbot effect originated by a periodic pulse train. The frequency chirp of the pulses is also considered in order to evaluate its effect on both the integer and the fractional selfimages.  相似文献   

7.
We report compression of low-power femtosecond pulses at 1.06 microm in a dispersion-decreasing holey fiber. Near-adiabatic compression of 130 fs pulses down to 60 fs has been observed. Measured spectra and pulse shapes agree well with numerical simulations. Compression factors of ten are possible in optimized fibers.  相似文献   

8.
《Optik》2014,125(16):4505-4507
We present our experimental demonstration of controlling waveform of a signal pulse by using two beams of continuous wave (CW) generated by stimulated Brillouin scattering (SBS) in optical fibers with different frequencies. Waveform of the signal pulse is modulated in an “all-optical” way according to total input power. This method is only suitable for light pulse with nanosecond width. We provide a new method for controlling light with light.  相似文献   

9.
为了实现对飞秒激光器产生的超短脉冲的进一步压缩,对近年来出现的一种新型负曲率空芯光纤展开了研究,并基于该光纤对800 nm飞秒激光进行了压缩实验。首先介绍了一种圆形玻璃管包层结构的负曲率空芯光纤,通过有限元方法对光纤的损耗特性进行计算,并与实验测试结果进行对比。然后利用广义非线性薛定谔方程对脉冲在光纤中的传输进行了模拟仿真。最后利用该光纤进行了超短脉冲压缩实验,将脉冲宽度为160 fs的钛宝石飞秒激光耦合进一段充高压氩气的圆形玻璃管包层结构的负曲率空芯光纤,通过光纤内反常色散和自相位调制的共同作用,得到84 fs的输出,实现脉冲的压缩,实验结果与仿真计算一致。这种新型的负曲率空芯光纤损伤阈值高、色散、非线性系数小且灵活可调,非常适用于超快领域研究。  相似文献   

10.
Behar V  Adam D 《Ultrasonics》2004,42(10):1101-1109
A linear array imaging system with coded excitation is considered, where the proposed excitation/compression scheme maximizes the signal-to-noise ratio (SNR) and minimizes sidelobes at the output of the compression filter. A pulse with linear frequency modulation (LFM) is used for coded excitation. The excitation/compression scheme is based on the fast digital mismatched filtering. The parameter optimization of the excitation/compression scheme includes (i) choice of an optimal filtering function for the mismatched filtering; (ii) choice of an optimal window function for tapering of the chirp amplitude; (iii) optimization of a chirp-to-transducer bandwidth ratio; (iv) choice of an appropriate n-bit quantizer. The simulation results show that the excitation/compression scheme can be implemented as a Dolph–Chebyshev filter including amplitude tapering of the chirp with a Lanczos window. An example of such an optimized system is given where the chirp bandwidth is chosen to be 2.5 times the transducer bandwidth and equals 6 MHz: The sidelobes are suppressed to −80 dB, for a central frequency of 4 MHz, and to −94 dB, for a central frequency of 8 MHz. The corresponding improvement of the SNR is 18 and 21 dB, respectively, when compared to a conventional short pulse imaging system. Simulation of B-mode images demonstrates the advantage of coded excitation systems of detecting regions with low contrast.  相似文献   

11.
By using the Radon-Wigner transform (RWT), we analyze the temporal selfimaging or Talbot effect for producing well-conformed pulse trains with variable repetition rates and duty-cycles. The relationships linking the selfimaging conditions with the fractional orders of the RWT are first obtained for unchirped pulse trains. Then, we extend the analysis to chirped pulse sequences by deriving the conditions to be fulfilled by an equivalent unchirped pulse train producing the same selfimage irradiances. This result becomes relevant for observing well-defined high order fractional selfimaging, which are of interest due to their repetition rate multiplication. Besides, the effect of the finite extension of the pulse train on the selfimage quality is analyzed and a condition is found for relating the required minimum pulse number with the chirp parameter of the pulses.  相似文献   

12.
The temporal Radon-Wigner transform (RWT), which is the squared modulus of the fractional Fourier transform (FRT) for a varying fractional order p, is here employed as a tool for pulse compression applications. To synthesize the compressed pulse, a selected FRT irradiance is optically produced employing a photonic device that combines phase modulation and dispersive transmission. For analysis purposes, the complete numerical generation of the RWT with 0 < p < 1 is proposed to select the value of p required for pulse compression. To this end, the amplitude and phase of the signal to be processed should be known. In order to obtain this information we use a method based on the recording of two different FRT irradiances of the pulse. The amplitude and phase errors of the recovered signal, which are inherent to the recording process, are discussed in connection with the RWT production. Numerical simulations were performed to illustrate the implementation of the proposed method. The technique is applied to compress signals commonly found in fiber optic transmission systems, such as chirped gaussian pulses, pulses distorted by second and third-order dispersion and nonlinear self-modulated pulses.  相似文献   

13.
In this paper, gold-coated gratings for pulse compression have been prepared and their laser damage experiments have been performed. Varied laser damage morphologies have been observed: when a 60 fs-pulsed laser with energy density slightly higher than the damage threshold was used, damage morphology with a characteristic of discrete distribution of small pits was appeared. These damage pits are linearly distributed at the junction of ridges and grooves. If the laser energy density is much higher than the damage threshold, the gold films was overall ablated and the grating structure disappeared. Besides, if the gold film has poor adhesion, it was peeled off. When a 450 ps-pulsed laser with energy density slightly higher than the damage threshold was used, part of grating ridges will be ablated and an obvious line exists between the ablated area and the unchanged area. In theory, the laser induced temperature field and stress field in gold-coated gratings were calculated based on the electromagnetic field using the finite element method. It is demonstrated that the temperature and thermal stress distribution characteristics are affected by the laser heating rate and the heat diffusion time (the calculated diffusion time ranges from 6 fs to 450 ps), which determines the laser damage characteristics. The possible damage drivers have electron hydrodynamic pressure, thermal ablation and thermal stress.  相似文献   

14.
王强  毛捷  廉国选 《应用声学》2020,39(4):558-562
该文研究了不同编码带宽下超声换能器对编码信号脉冲压缩后信噪比与轴向分辨率的影响关系。将脉冲压缩后的时域峰值转化为频域积分的形式,得到考虑换能器影响的脉冲压缩信噪比公式。以线性调频信号为例,仿真与实验结果表明,编码激励相对于方波激励的信噪比增益随编码带宽的减小而增大,因为受换能器带宽限制,编码激励的轴向分辨率随编码带宽的增大先减小后趋于稳定。该研究为编码激励方法更有效地应用于超声检测的背景中提供了参考。  相似文献   

15.
X波段脉冲压缩装置的数值模拟及优化设计   总被引:1,自引:1,他引:0  
 利用有限元方法,通过调节X波段脉冲压缩装置的腔体长度、输入膜片宽度、输出耦合口位置等参量,研究了这些参量对谐振频率和品质因数的影响关系。研究表明:通过微调腔体长度并优化结构参数,可以将该装置的工作频率限制在规定的范围内;输入膜片缝隙由宽变窄的过程中,驻波比由大变小,达到临界耦合后,驻波比又由小变大,且谐振频率略有升高;品质因数与H-T分支的T形输出口的微波泄露密切相关,而该输出口泄露的大小随短路面到H-T分支中线的距离周期性变化。模拟得到的膜片距输出口中线长度为1 133.75 mm,分支中线到短路面的长度为95.25 mm,输入膜片宽9 mm,本征频率为9.387 2 GHz,输入耦合系数为1.15,品质因数为8 000。根据数值模拟结果,优化设计了一套脉冲压缩装置,实测得到的工作频率为9.388 4 GHz,输入耦合系数为1.03,品质因数为5 500。由于该装置输出口微波泄露较大,因此实测的品质因数比模拟的要小一些,这一点可以通过改进终端滑动短路面的调节方式来改善。  相似文献   

16.
光纤损耗对皮秒脉冲孤子效应压缩的影响   总被引:16,自引:2,他引:14  
曹文华  廖常俊 《光学学报》1993,13(11):003-1007
在计及常规光纤损耗的前提下,通过数值求解求解修正的非线性薛定谔方程,全面地计算和分析了损耗对皮秒脉冲在单模光纤中孤子效应压缩过程的影响。结果表明,与不计及损耗时相比,损耗一方面导致脉冲压缩比,压缩后的脉冲峰值功率和脉冲压缩质量的下降,另一方面还导致所选用的最佳光纤度的增加。进一步研究表明,损耗对脉冲压缩的影响程度还与输入脉冲的峰值功率和脉宽有关。  相似文献   

17.
Nowadays, many ultrasonic sensory systems are being developed to operate outdoors, where they are finding a variety of applications, such as local positioning, vehicle navigation or obstacle detection. To assure the reliable operation of these systems under any meteorological condition, it is necessary to achieve a thorough comprehension of the effects that the different atmospheric phenomena can have on the propagation of these acoustic waves. This paper deals with one of these phenomena, atmospheric refraction, and its influence on the performance of an ultrasonic system whose signals are detected by matched filtering.  相似文献   

18.
为了增加靶上的功率密度和耦合效率,基于饱和增益开关原理,发展了一种适用于放大自发辐射平滑光束的脉宽压缩方法。利用该方法,在赛格德大学的一台放电泵浦KrF准分子激光器上进行了实验,将该激光器输出的脉宽为14.5 ns的放大自发辐射光束压缩到了7.5 ns,并且保持了光束原有的均匀性。  相似文献   

19.
Song J  Chang JH  Song TK  Yoo Y 《Ultrasonics》2011,51(4):516-521
Coded tissue harmonic imaging with pulse inversion (CTHI-PI) based on a linear chirp signal can improve the signal-to-noise ratio with minimizing the peak range sidelobe level (PRSL), which is the main advantage over CTHI with bandpass filtering (CTHI-BF). However, the CTHI-PI technique could suffer from motion artifacts due to decreasing frame rate caused by two firings of opposite phase signals for each scanline. In this paper, a new CTHI method based on a nonlinear chirp signal (CTHI-NC) is presented, which can improve the separation of fundamental and harmonic components without sacrificing frame rate. The nonlinear chirp signal is designed to minimize the PRSL value by optimizing its frequency sweep rate and time duration. The performance of the CTHI-NC method was evaluated by measuring the PRSL and mainlobe width after compression. From the in vitro experiments, the CTHI-NC provided the PRSL of −40.6 dB and the mainlobe width of 2.1 μs for the transmit quadratic nonlinear chirp signal with the center frequency of 2.1 MHz, the fractional bandwidth at −6 dB of 0.6 and the time duration of 15 μs. These results indicate that the proposed method could be used for improving frame rates in CTHI while providing comparable image quality to CTHI-PI.  相似文献   

20.
Yuee Li  Xiaoping Zhang   《Optics Communications》2008,281(19):5009-5013
Pulse propagation equation of nonlinear dispersion surface plasmon waveguide is educed strictly from wave equation. The nonlinear coefficient is defined and then used to assess and compare the nonlinear characteristic of three popular 1-D surface plasmon waveguides: the single metal–dielectric interface, the metal slab bounded by dielectric and the dielectric slab bounded by metal. SPM (self-phase modulation) of the typical surface plasmon waveguide is predicted and discussed.  相似文献   

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