任意布拉格波长Chirped光栅的写入

提出了一种波长写入范围达30 nm 的Chirped 光栅的构造方法,这种方法只需要一个会聚柱透镜、一个发散柱透镜和相位掩膜板,并且对光纤与相位掩膜板的距离与写入光栅的Bragg

切趾线性chirped光纤光栅的制作及其色散特性

本文用扫描曝光法制作出12cm长切趾线性chirped光纤光栅，光栅在0．3nm带宽内时延曲线接近线性，曲线最大线性偏离度（时延振荡）小于±20ps，时延曲线斜率（光栅色散值）约为－1750ps/nm，可补偿100km常规单模光纤的色散。

Chirped Bragg光纤光栅的优化设计与优化指数

根据线性ChirpedBragg光纤光栅的一般原理 ,探讨了不同啁啾系数 ,准高斯耦合函数对Bragg反射光栅的反射率及色散补偿特性的响应。结果表明 :增大啁啾系数以及选取适当的准高斯耦合函数 ,在保证反射率较大的情况下 ,能有效地改善色散补偿特性。通过引入微波领域的“优化指数”这一概念 ,量化了色散补偿器的补偿能力。

取样线性chirped光纤光栅的制作及其色散特性

本文用扫描曝光法制作出8cm长取样线性chirped光纤光栅，并对其中三个主要的反射峰带宽范围内的时延特性进行测试。光栅三个反射峰内均有接近线性的时延曲线，且色散值基本相同。可见，一支样线性chirped光纤光栅可以用来补偿光通信系统中路波长信号的色散。

Chirped Bragg 光纤光栅色散补偿研究

分析ＣｈｉｒｐｅｄＢｒａｇｇ光纤光栅的色散特性，并作一定性分析．利用耦合模方程导出ＣｈｉｒｐｅｄＢｒａｇｇ光纤光栅的反射率方程，从而推导出ＣｈｉｒｐｅｄＢｒａｇｇ光纤光栅的色散计算公式，并用数值分析画出它们的响应曲线．

Chirped AM激光雷达中线性调频信号的产生

线性调频强度调制(Chirped AM)激光雷达将微波雷达中调频测距原理巧妙地应用于激光雷达,用一个线性调频的射频副载波调制激光输出强度。介绍了FM测距的基本数学原理,及激光雷达系统的基本构成和工作原理。在分析对比本体制激光雷达中一项关键技术——线性调频信号产生几种实现方法的基础上,依据直接数字频率合成和正交调制技术,提出了一种宽带线性调频信号产生方案。介绍了信号发生系统的基本结构以及工作原理,探讨了系统实现的关键技术、技术难点及改进办法。

成人CE-Chirp ABR反应阈与纯音听阈相关分析与比较

目的 采用听神经同步专利刺激声(CE-Chirp声)对成人听性脑干反应(auditory brainstem response,ABR)进行测试,分析CE-Chirp ABR测试的V波反应阈与纯音听阈的关系,研究CE-Chirp声在法医学鉴定听觉功能障碍评估中的作用。方法 选择常州市德安医院2018年1月—2019年6月进行CE-Chirp ABR测试的受试者(年龄为20~77周岁,共计100耳),获得V波反应阈值,并在0.5、1.0、2.0、4.0 kHz分别进行纯音气导听阈测试,获得纯音听阈值,按照不同听力水平及不同年龄对受试者进行分组。比较不同听力水平及不同年龄组平均纯音听阈与V波反应阈之间的差值及统计学差异;对所有受试者各频率两种方法之间的相关性、差值及统计学差异进行分析;建立所有受试者CE-Chirp ABR V波反应阈推断纯音听阈的线性回归方程,并检验其推断纯音听阈的可行性。结果 不同听力水平及不同年龄组各组之间CE-Chirp ABR反应阈与纯音听阈差值的差异无统计学意义(P>0.05);各频率成人CE-Chirp ABR V波反应阈与纯音听阈之间相关性良好,两者之间差异具有统计学意义(P<0.05),线性回归分析显示两者之间有线性相关关系(P<0.05)。结论 运用CE-Chirp ABR Ⅴ波反应阈在一定条件下能够评估受试者的纯音听阈,可以作为一种听力学测试方法用于法医学听觉障碍评估。

正常成年人水平特异性CE-Chirp刺激声与Click刺激声诱发听性脑干反应的比较

目的研究正常成年人水平特异性CE-Chirp(level specific CE-Chirp,CE-Chirp LS)刺激声与Click刺激声诱发听性脑干反应(auditory brainstem response,ABR)反应阈与纯音听阈的关系及在不同声强下两种刺激声所诱发的ABR波形特点,探讨CE-Chirp LS声诱发的ABR在听觉功能客观评估中的应用价值。方法选择正常成年人21例(共42耳)分别在0.5、1.0、2.0、4.0 kHz进行纯音气导听阈测试,获取其双耳各频率的纯音听阈,分别采用CEChirp LS刺激声与Click刺激声诱发ABR,测量2种刺激声在80、60、40 dB nHL的Ⅴ波波幅,获得2种刺激声下受试者的Ⅴ波反应阈,获取其在80 dB nHL刺激强度时Ⅰ、Ⅲ、Ⅴ波潜伏期。按照自身对照的方法对相同刺激强度下2种刺激声诱发的ABR潜伏期及波幅差异性进行统计分析,比较2种刺激声下Ⅴ波反应阈与纯音听阈差值。结果正常成年人80、60、40 dB nHL刺激强度下,CE-Chirp LS刺激声诱发的ABR的Ⅴ波波幅均大于Click刺激声,差异有统计学意义(P<0.001);CE-Chirp LS刺激声诱发的ABR的V波反应阈与纯音平均听阈差值均低于Click刺激声,差异有统计学意义(P<0.05);80 dB nHL声强下CE-Chirp LS刺激声Ⅰ波潜伏期长于Click刺激声,差异有统计学意义(P<0.001),CE-Chirp LS刺激声Ⅲ、Ⅴ波潜伏期与Click刺激声比较,差异无统计学意义(P>0.05)。结论正常成年人CE-Chirp LS刺激声与Click刺激声比较,无论在高强度还是低强度刺激下波幅均明显增大,Ⅴ波反应阈更接近于纯音听阈,更有利于纯音听阈判定,但潜伏期个体差异更大。

Interference effect of photoionization of hydrogen atoms by ultra-short and ultra-fast high-frequency chirped pulses

The photoionization of a hydrogen atom from its ground state with ultra-fast chirped pulses is investigated by numerically solving the time-dependent Schrodinger equation within length,velocity,and Kramers-Henneberger gauges.Converged results for all gauges for chirp-free pulses agree with the prediction of dynamic interference for ground state hydrogen atoms predicted recently by Jiang and Burgdorfer[Opt.Express 26,19921(2018)].In addition,we investigated photoelectron spectra of hydrogen atoms by chirped laser pulses,and showed that dynamic interference effect will be weaken for pulses with increasing linear chirp.Our numerical results can be understood and discussed in terms of an interplay of photoelectron wavepackets from first and second halves of laser enevelop,including the ac Stark energy level shift of the photoelectron final state and atomic stabilization effect at ultra-high intensities.

Extension of high-order harmonics and generation of an isolated attosecond pulse in the chirped laser field

This paper theoretically investigates the high-order harmonic generation cutoff extension using intense few-cycle linearly chirped laser pulses. It shows that the cutoff of the harmonic can be extended remarkably by optimising the chirping parameters. The time-frequency characteristics of high-order harmonics with different chirping parameters are analysed by means of wavelet transform of the dipole acceleration. It also gives out the classical three-step model pictures of electron. By superposing a properly selected range of the harmonic spectrum, it obtains an isolated 65as pulse.

Ionization of atoms by chirped attosecond pulses

We investigate the ionization dynamics of atoms by chirped attosecond pulses using the strong field approximation method. The pulse parameters are carefully chosen in the regime where the strong field approximation method is valid. We analyse the effects of the chirp of attosecond pulses on the energy distributions and the corresponding left-right asymmetry of the ionized electrons. For a single chirped attosecond pulse, the ionized electrons can be redistributed and the left-right asymmetry shows oscillations because of the introduction of the chirp. For time-delayed double attosecond pulses at different intensities with the weaker one chirped, exchanging the order of the two pulses shows a relative shift of the energy spectra, which can be explained by the different effective time delays of different frequency components because of the chirp.

Above-threshold ionization of hydrogen atom in chirped laser fields

Above-threshold ionization （ATI） of a hydrogen atom exposed to chirped laser fields is investigated theoretically by solving the time-dependent Schrodinger equation. By comparing the energy spectra, the two-dimensional momentum spectra, and the angular distributions of photoelectron for the laser pulses with different chirp rates, we show a very clear chirp dependence both in the multiphoton and tunneling ionization processes but no chirp dependence in the single-photon ionization. We find that the chirp dependence in the multiphoton ionization based ATI can be attributed to the excited bound states. In the single-photon and tunneling ionization regimes, the electron can be removed directly from the ground state and thus the excited states may not be very important. It indicates that the chirp dependence in the tunneling ionization based ATI processes is mainly due to the laser pulses with different chirp rates,

Wavefront evolution of the signal beam in Ti:sapphire chirped pulse amplifier

We studied the evolution of wavefront aberration(WFA) of a signal beam during amplification in a Ti:sapphire chirped pulse amplification(CPA) system. The results verified that the WFA of the amplified laser beam has little relation with the change of the pump beam energies. Transverse parasitic lasing that might occur in CPA hardly affects the wavefront of the signal beam. Thermal effects were also considered in this study, and the results show that the thermal effect cumulated in multiple amplification processes also has no obvious influence on the wavefront of the signal beam for a single-shot frequency. The results presented in this paper confirmed experimentally that the amplification in a Ti:sapphire CPA system has little impact on the WFA of the signal beam and it is very helpful for wavefront correction of single-shot PW and multi-PW laser systems based on Ti:sapphire.

Strain Multipoint Measurements Based on Chirped Bragg Grating Sensors

In this paper,we propose the novel system of multipoint measurement.The sensors of measurements are chirped Bragg grating and the interrogation of sensors is sub-carrier phase.The wavelength division multiplexing technique is used for addressing a network of FBG sensors and the time-division multiplexing technique is used for multipoint measurements.In the system,the modulation frequency of 200 MHz is adopted.The range of dectetion is from 0 to 900μεand the resolution is 12με. The time of the sensor response is about 1ns.

Propagation properties of chirped Airy vortex beams with x-polarization through uniaxial crystals

The propagation dynamics of a chirped Airy vortex（CAiV） beam with x-polarization in uniaxial crystals orthogonal to the optical axis is studied analytically and numerically. The effect of the ratio of extraordinary and ordinary refractive indices, the chirp parameter, as well as the propagation distance is analyzed, which shows that the focused position of the CAi V beams can be controlled through changing the ratio of the extraordinary and ordinary refractive indices. In addition,with the propagation distance increasing, the asymmetry of the intensity and the angular momentum of the CAi V beam during propagation becomes much more visible. The variation of the chirp parameters can change the attenuation velocity of the vortex as well.

Efficiency droop suppression in GaN-based light-emitting diodes by chirped multiple quantum well structure at high current injection

Gallium nitride （GaN） based light-emitting diodes （LEDs） with chirped multiple quantum well （MQW） structures have been investigated experimentally and numerically in this paper. Compared to conventional LEDs with uniform quantum wells （QWs）, LEDs with chirped MQW structures have better internal quantum efficiency （IQE） and carrier injection efficiency. The droop ratios of LEDs with chirped MQW structures show a remarkable improvement at 600 mA/mm2, reduced down from 28.6% （conventional uniform LEDs） to 23.7% （chirped MQWs-a） and 18.6% （chirped MQWs-b）, respectively. Meanwhile, the peak IQE increases from 76.9% （uniform LEDs） to 83.7% （chirped MQWs-a） and 88.6% （chirped MQWs-b）. The reservoir effect of chirped MQW structures is the significant reason as it could increase hole injection efficiency and radiative recombination. The leakage current and Auger recombination of chirped MQW structures can also be suppressed. Furthermore, the chirped MQWs-b structure with lower potential barriers can enhance the reservoir effect and obtain further improvement of the carrier injection efficiency and radiative recombination, as well as further suppressing efficiency droop.

Nonparaxial propagation properties of the chirped Airy Gaussian vortex beams in uniaxial crystals orthogonal to the optical axis

In this article, we investigate the nonparaxial propagation properties of the chirped Airy Gaussian vortex（CAiGV）beams in uniaxial crystals orthogonal to the optical axis analytically and numerically. We discuss how the linear chirp parameters, the quadratic chirp parameters, and the Gaussian factors influence the nonparaxial propagation dynamics of the CAiGV beams. The intensity, the energy flow, the beam center, and the angular momentum of the CAiGV beams are deeply investigated. It is shown that the Gaussian factors have a great effect on the intensity and the centroid positions of the CAiGV beams. With the Gaussian factors increasing, the intensity of CAiGV beams decreases rapidly. The main lobes of the transverse intensity distribution of the CAiGV beams are similar to triangles.

Lithium atom population transfer by population trapping in a chirped microwave pulse

Using a time-dependent multilevel approach, we demonstrate that lithium atoms can be transferred to states of lower principle quantum number by exposing them to a frequency chirped microwave pulse. The population transfer from n = 79 to n = 70 states of lithium atoms with more than 80% efficiency is achieved by means of the sequential two-photon △n=-1 transitions. It is shown that the coherent control of the population transfer can be accomplished by the optimization of the chirping parameters and microwave field strength. The calculation results agree well with the experimental ones and novel explanations have been given to understand the experimental results.

Two-photon double ionization of helium by chirped few-cycle attosecond pulses:From nonsequential to sequential regime

The two-photon double ionization（TPDI） dynamics of helium by chirped attosecond pulses are theoretically studied by solving the two-electron time-dependent Schr o¨dinger equation in its full dimensions. We show that both the differential and the total double ionization probability can be significantly controlled by adjusting the chirp. The dependence of the TPDI on the chirp can be quite different for different photon energies, relying on the central photon energy being in the sequential region, nonsequential region, or translation region. The physics which lead to the chirp dependence for different photon energies are addressed. Present findings are well reproduced by a model based on the second-order time-dependent perturbation theory.

Propagation properties of the chirped Airy–Gaussian vortex electron plasma wave

We introduce a new class of the chirped Airy–Gaussian vortex electron plasma(CAiGVEP)wave which constitutes the exact and continuous transition modes between the chirped Airy vortex and the chirped Gaussian vortex electron plasma wave.The intensity,the phase,and the angular momentum density flow of the CAiGVEP wave are discussed under different distribution factors and different chirp modes.