Experimental and theoretical analysis of nondegenerate ultrabroadband chirped pulse optical parametric amplification

Experimental investigations of nondegenerate ultrabroadband chirped pulse optical parametric amplification have been carried out. The general mathematical expressions for evaluating parametric bandwidth, gain and gain bandwidth for arbitrary three-wave mixing parametric amplifiers are presented. In our experiments, a type-I noncollinear phase-matched optical parametric amplifier based on lithium triborate, which was pumped by a 5-ns second harmonic pulses from a Q-switched Nd:YAG operating at 10 Hz, seeded by a 14-fs Ti:sapphire laser at 800 nm, was presented. The 0.85 nJ energy of input chirped signal pulse with 57-FWHM has been amplified to 3.1 muJ at pump intensity 3 GW/cm(2), the corresponding parametric gain reached 3.6 x 10(3), the 53 nm-FWHM gain spectrum bandwidth of output signal has been obtained. The large gain and broad gain bandwidth, which have been confirmed experimentally, provide great potentials to amplify efficiently the broad bandwidth femtosecond light pulses to generate new extremes in power, intensity, and pulse duration using optical parametric chirped pulse amplifiers pumped by powerful nanosecond systems.

An experimental study of ultrashort pulsed ytterbium-doped fibre laser and amplifier

We report the generation of ultrashort pulses in ytterbium-doped fibre oscillator emitting around 1.05 mum at a repetition rate of 17.6MHz. A diode laser with single silica fibre at 976 nm pumps the ytterbium fibre laser, the all-fibre picosecond pulsed oscillator has excellent stability and compact size, and freedom from misalignment. After amplifying, pulse energy of 3.4 nJ and an average power of 60mW are obtained. The compression is obtained with a grating pair out of the cavity. The compressor produces 307 fs with the peak power 5.47 kW. A practical fibre-based source with good performance is thus demonstrated.

Generation of the high efficiency high peak-power femtosecond blue optical pulse

The analysis and calculation of the compensation for the phase mismatch of the frequency-doubling using the frequency space chirp introduced from prisms are made. The result shows that suitable lens can compensate the phase mismatch in a certain extent resulting from wide femtosecond spectrum when the spectrum is space chirped. By means of this method, the experiment of second harmonic generation is carried out using a home-made femtosecond KLM Ti:sapphire laser and BBO crystal. The conversion efficiency of SHG is 63 %. The average output power of blue light is 320 mW. The central wavelength is 420 nm. The spectrum bandwidth is 5.5 nm. It can sustain the pulse width of 33.6 fs. The tuning range of blue light is 404-420 nm,when the femtosecond Ti:sapphire optical pulse is tuned using the prisms in the cavity.

Non-collinear CPOPA seeded by an Yb3+-doped self-starting passive mode-locked fiber laser

Using a home-made seed at 1053 nm from a Yb3+-doped passively mode-locked fiber laser of 1.5 nJ/pulse, 362 ps pulse duration with a repetition rate of 3.842 MHz, a compact, low cost, stable and excellent beam quality non-collinear chirped pulse optical parametric amplifier omitting the bulky pulse stretcher has been demonstrated. A gain higher than 4.0 x 10(6), single pulse energy exceeding 6 mJ with fluctuations less than 2% rms, 14 nm amplified signal spectrum and recompressed pulse duration of 525 fs are achieved. This provides a novel and simple amplification scheme. (c) 2007 Optical Society of America.

Generation of 207-femtosecond pulses from a ytterbium figure-of-eight fibre laser

We report the generation of 207-fs pulses with 1.2mW average power at 1036 nm directly from a passively mode-locked Yb-doped fibre laser with a nonlinear optical loop mirror for mode-locking and pairs of diffraction gratings for intracavity dispersion compensation. These results imply a 4-fold reduction in pulse duration over previously reported figure-of-eight cavity passively mode-locked Yb-doped fibre lasers. Stable pulse trains are produced at the fundamental repetition rate of the resonator, 24.0MHz. On the other hand, this laser offers a cleaner spectrum and greater stability and is completely self-starting.

SOA-based actively mode-locked fiber ring laser by forward injecting an external pulse train

An actively mode-locked fiber ring laser based on cross-gain modulation (XGM) in a semiconductor optical amplifier (SOA) is demonstrated to operate stably with a simple configuration. By forward injecting an easily-generated external pulse train, the mode-locked fiber laser can generate an optical-pulse sequence with pulsewidth about 6 ps and average output power about 7.9 mW. The output pulses show an ultra-low RMS jitter about 70.7 fs measured by a RF spectrum analyzer. The use of the proposed forward-injection configuration can realize the repetition-rate tunability from I to 15 GHz for the generated optical-pulse sequences. By employing a wavelength-tunable optical band-pass filter in the laser cavity, the operation wavelength of the designed SOA-based actively mode-locked fiber laser can be tuned continuously in a wide span between 1528 and 1565 nm. The parameters of external-injection optical pulses are studied experimentally to optimize the mode-locked fiber laser. (C) 2009 Elsevier B.V. All rights reserved.

Transfer property of electron pulse in a femto-second electron diffraction system

An ultra-fast electron diffraction system has been designed. The static and dynamic characters of an electron pulse with 150 fs temporal dispersion are studied during its transmission in the whole ultra-fast electron diffraction system, including the size of the electron spot, temporal dispersion, distribution of azimuths and elevation angles. The initial status of the photoelectrons are put down by Monte Carlo method, both the two dimensional and three dimensional electric fields are calculated by finite difference method and the magnetic flux are. calculated by finite element method.

澜沧江姬鼠（Apodemus ilex）种群遗传结构及其生物地理分析

澜沧江姬鼠（Apodemus ilex）为小型啮齿类动物，长期以来常被认为是中华姬鼠（A. draco）或长尾姬鼠（A. orestes）的同物异名，但近年基于线粒体Cyt b 的研究证明，该类群与中华姬鼠的遗传距离达到了种间水平，并被认为是一个独立种。本文提取、扩增并测定了来自云南14个地区42个产地156个澜沧江姬鼠的Cyt b 全序列，并将GenBank中的3条澜沧江姬鼠的Cyt b 全序列纳入分析，选取福建武夷山与四川峨眉山的2个中华姬鼠样品的Cyt b 全序列，以及台湾姬鼠、大耳姬鼠、高山姬鼠Cyt b 全序列作为外群，利用贝叶斯法和最大似然法构建系统发育树，并使用Network分析，分子变异分析（AMOVA）分析、错配分析（Mismatch analysis）与Fu`Fs检验等方法，探讨了这些地区澜沧江姬鼠的种群遗传结构，种群动态及生物地理格局。结果表明：云南地区过去被鉴定为中华姬鼠的样品均属于澜沧江姬鼠，澜沧江姬鼠与中华姬鼠间的遗传距离（K2P-ds+v）达到0.091，显著超过姬鼠属内种间差距（0.080），支持澜沧江姬鼠独立种的地位；该种不同地理种群可大致以澜沧江为界分为两大支系，且每个支系又各分为两个亚支系；进一步的AMOVA分析表明遗传变异主要来源于两大支系之间，而错配分析与Fu`Fs检验表明澜沧江姬鼠各地理种群及其两个支系都经历过多次扩张事件，这可能是和冰期与间冰期的轮回交替有关；分子系统树和中介网络图表明地理环境的隔离对于澜沧江姬鼠种群分化存在明显影响，其中澜沧江的阻隔作用最为显著。基于松散分子钟（Relax molecular clock）分析，中华姬鼠和澜沧江姬鼠的分歧时间大约在2.98 Ma（95％HPD: 4.32-1.88），而澜沧江姬鼠则在1.13 Ma（95％HPD: 1.95-0.65）分成两个支系。按照平均分歧时间来看，澜沧江姬鼠两个支系的的分歧事件发生在鄱阳冰期（1.2-0.9 Ma），两个支系内部进一步分化为两支的时间非常接近，分别为：Clade 1中为0.67 Ma （95％HPD: 1.17-0.34）和Clade 2 中为0.64 Ma (95％HPD: 1.17-0.36)，这种隔离种群各自产生分化的时间却非常接近，这提示其分化事件可能是受到古气候如冰期或间冰期的影响所产生。

应激对大鼠海马突触可塑性和学习记忆的影响

突触可塑性参与学习记忆，是学习记忆过程中必不可少的重要环节。应激能损伤或提高学习记忆、抑制长时程增强（Long一termPotentiation，LTP）、易化长时程抑制（Long一termdePressfon，LTD）。然而，应激经历依赖的长时程抑制（StressexperiencedePendentLTD，SLTD）在学习记忆中有什么意义还不清楚，这正是本文首先要探讨问题。其次，尽管我们在不同年龄时期的学习记忆能力不同，但是对所经历的重大应激事件仍然能产生牢固的记忆，这就有必要进一步通过阐明应激对突触可塑性的影响是否有年龄差异来解释SLTD的意义。再者，我们甚至不清楚为什么有的时候应激损伤学习记忆而有的时候又提高学习记忆。为了阐明这个问题，本文在最后一部分研究了哪些因素决定应激损伤还是提高学习记忆。为了探讨SLTD与学习记忆的关系，我们在第一部分实验中研究急性或亚急性的高台（ElevatedPlatform，EP）或足部电击（Footshock，Fs）对4周龄诚star大鼠海马CAI区LTD诱导的影响，以及这些应激条件对大鼠空间学习记忆的影响。结果显示：（l）急性EP易化LTD，亚急性EP不易化LTD；急性和亚急性FS都易化了LTD。（2）急性EP损伤空间记忆，亚急性EP对空间记忆没有影响；急性FS不影响空间记忆，亚急性FS却提高了空间记忆。这部分的实验结果表明：sLTD存在与否与应激对空间记忆的影响不是一一对应的关系，提示sLTD可能参与了应激记忆（对应激经历产生的记忆）。如果SLTD参与应激记忆，那么，研究应激对突触可塑性的影响是否有年龄依赖性将有助于解释不同年龄时期的学习记忆能力不同但是都能牢固记忆应激事件这一现象。为此，我们在第二部分实验中进一步研究EP对幼年、中年和老年动物（4，10和74周龄的Wistar大鼠）海马CAI区LTP／LTD诱导的影响。结果表明：（1）没有应激的情况下，LTP的大小随动物年龄的增加呈明显的倒U型关系，而低频刺激都不能诱导出LTD。（2）EP易化了这些年龄段大鼠的LTD，并完全阻断它们的LTP。值得注意的是，在三个年龄段大鼠中，EP易化的LTD大小一样。该部分实验结果提示：SLTD没有年龄依赖性，这与人和动物在不同年龄时期对所受到的重大应激事件都能产生牢固记忆这一现象相一致。所以，该部分结果进一步加强了第一部分结果的推测：SLTD参与应激记忆。应激有的时候提高动物的空间记忆能力，有的时候又损伤其空间记忆。为了阐明是什么因素决定应激损伤还是提高学习记忆，我们在第三部分实验中研究EP、FS和水迷宫游泳应激经历对六个年龄段动物（4，10，13，20，67，76周龄）在水迷宫任务中的影响。结果显示：（l）EP应激损伤无水迷宫游泳应激经历大鼠的空间记忆。（2）EP应激提高有游泳应激经历幼年大鼠的空间记忆；训练前外源性补充皮质酮或FS都抑制皮质酮或FS导致的空间记忆受损。（3）糖皮质激素受体的拮抗剂RU38486阻断上述的空间记忆成绩提高。所以，不同的应激经历和动物年龄两个因素共同决定了应激损伤还是提高学习记忆。

Room-Temperature Continuous-Wave Operation of InGaN-Based Blue-Violet Laser Diodes with a Lifetime of 15.6 Hours

We report our recent progress of investigations on InGaN-based blue-violet laser diodes (LDs). The room-temperature (RT) cw operation lifetime of LDs has extended to longer than 15.6 h. The LD structure was grown on a c-plane free-standing (FS) GaN substrate by metal organic chemical vapor deposition (MOCVD). The typical threshold current and voltage of LD under RT cw operation are 78 mA and 6.8 V, respectively. The experimental analysis of degradation of LD performances suggests that after aging treatment, the increase of series resistance and threshold current can be mainly attributed to the deterioration of p-type ohmic contact and the decrease of internal quantum efficiency of multiple quantum well (MQW), respectively.

MODELING OF ELECTRON-TUNNELING TIMES IN ASYMMETRIC DOUBLE QUANTUM-WELLS

A scattering process modeled by an imaginary potential V(I) in the wide well of an asymmetric double quantum well structure (DQWS) is used to model the electron tunneling from the narrow well. Taking V(I) approximately -5 meV, the ground resonant level lifetimes of the narrow well in the DQWS are in quantitative agreement with the experimental resonance and non-resonance tunneling times. The corresponding scattering time 66 fs is much faster than the intersubband scattering time of LO-photon emission.

LIQUID-PHASE EPITAXY GROWTH AND PROPERTIES OF GAINASSB/ALGAASSB/GASB HETEROSTRUCTURES

The GaInAsSb/AlGaAsSb/GaSb heterostructures were grown by the liquid phase epitaxy (LPE) technique. The materials were characterized by means of optical microscopy, electroprobe microanalysis (EPMA), double-crystal X-ray diffraction, capacitance-voltage (C-V) and Van der Pauw measurments, infrared absorption spectra, photoluminescence and laser Raman scattering. The results show that the materials have fine surface morphology, low lattice mismatch and good homogeneity. Room-temperature light-emitting diodes with an emission wavelength of 2.2-mu-m were obtained by using the GaInAsSb/AlGaAsSb DH structures.

Pulse Compression by Filamentation in Argon with an Acoustic Optical Programmable Dispersive Filter for Predispersion Compensation

We have experimentally demonstrated pulses 0.4 mJ in duration smaller than 12 fs with an excellent spatial beam profile by self-guided propagation in argon. The original 52 fs pulses from the chirped pulsed amplification laser system are first precompressed to 32 fs by inserting an acoustic optical programmable dispersive filter instrument into the laser system for spectrum reshaping and dispersion compensation, and the pulse spectrum is subsequently broadened by filamentation in an argon cell. By using chirped mirrors for post-dispersion compensation, the pulses are successfully compressed to smaller than 12 fs.

半导体可饱和吸收镜自启动的Kerr锁模Cr~(4+)∶YAG激光器

采用传统的X型像散腔,利用一块精心设计的半导体可饱和吸收镜(SESAM)做启动元件,实现了自启动的Kerr锁模Cr4+∶YAG激光器.输出脉冲的最窄脉宽小于80 fs,脉冲重复频率为120 MHz,脉冲峰值功率可以达到100 W以上.