5GHz的16.2ps超短光脉冲的产生

对采用法布里－珀罗腔和正常色散光纤联合消啁啾进行了理论和实验上的研究，实验得到啁啾小于孤子形成临界值，重复频率为５ＧＨｚ、脉宽为１６．２ｐｓ的超短光脉冲，并对消啁呼后的超短光脉冲进行了孤子传输实施。     

PDATS对ps脉冲的光限幅效应

应用脉宽为２１ｐｓ脉冲，波长为５３２ｎｍ的激光脉冲研究了新型光限幅材料５－（２－硫甲基－４－甲基－５－嘧啶基）－２，４－戊二炔－１醇的对甲苯磺酸酯的光限幅效应，其优点是限幅幅值和限幅阈值低，分别为Ｅｃ＝１８０ｍＪ／ｃｍ＾２，Ｅｔｈ＝１５０ｍＪ／ｃｍ＾２；可见了光透射率高。     

1.3μmDFB半导体激光超短脉冲的产生及其压缩

本文首次报道１．３μｍ单模超短脉冲产生及压缩实验。通过梳状波电脉冲直接调制ＤＣＰＢＨ－ＤＦＢ半导体激光器，获得２２ｐｓ单模光滑脉冲；然后利用Ｇ－Ｔ干涉仪压缩得到近变换极限超短脉冲。脉宽为９．３ｐｓ，峰值功率超过２００ｍＷ，重复频率１ＧＨｚ，时间带宽乘积为０．３９，脉冲压缩比为２．４。最后对实验结果进行了讨论。     

308nmXeCl准分子激光泵浦猝灭式可调谐染料激光器研究

描述了获得准分子激光超脉冲的一种方法，理论上扼要地介绍了淬来式染料激光器产生超短脉冲激光的机理。实验上以香豆素４９８染料得到波长为４９６ｎｍ，脉宽１ｎｓ，能量１．１ｍＪ的染料激光。     

X光激光实验研究进展

自１９８７年开发Ｘ光激光实验以来，在许多物理机制研究上取得重要进展，尤其利用电子碰撞激发机制实现了一系列类氖锗离子的Ｘ光激光增益。在驱动能量－６００Ｊ、脉宽－１．２ｎｓ条件下，首先获得１９．６－２８．６ｎｍ间的５条跃迁增益线，ＧＬ值约８，利用平面Ｘ光反射镜又实现双程放大，时间分辨的强度提高１０倍。     

Sr2准分子吸收离化及混合跃迁的研究

Ｎｄ－ＹＡＧ激光器三倍频泵浦的染料激光激发Ｓｒｌ原子,热二极管探共振离化信号,获得Ｓｒｌ高Ｒｙｄｂｅｒｇ５ｓｎｄＤ２系列双光子激光共振电离谱。实验发现激光汉长调４４０ｎｍ附近时,存在一Ｓｒ２准分子吸收光谱带,同时还观测到了５ｓ５ｐ＾１Ｐ１－５ｓ１１ｄ＾１Ｄ２,５ｓ５ｐ＾１Ｐ１－４ｄ＾２３Ｐ１混合共振跃迁现象。并对这种瞬态准分子的连续吸收光电离背景的形成和混合共振跃迁的机制作了初步探讨,同时对缓冲气     

含纳米随机微腔MEH-PPV/玻璃光波导激光

用浸涂法制备了ＭＥＨ－ＰＰＶ／ＴｉＯ２重量比分别为１∶０,１∶１,１∶２和１∶３四种不同纳米微晶薄膜。与已报道的亚微米散射体不同,本实验采用粒径约为２０ｎｍ的ＴｉＯ２纳米微晶作为多重散射体。可以不必考虑光在散射体上的出、入射方向和内部传播情况。飞秒激光器经ＯＰＡ调谐产生脉宽为１３０ｆｓ的超短脉冲,激发波长为５４４ｎｍ,重复频率为１ｋＨｚ,激发功率为３μＪ／ｐｕｌｓｅ。研究了不同激发强度下,光谱的增益窄化,激射强度和与激发光条长度的关系。这种激光发射的本质还是放大自发辐射（ＡＳＥ）为主。分析了在平均自由程 ｌ＝５．４ ×１０５ｎｍ下光的输运和光局域对这种随机激光产生的影响。     

有机高聚物PPQ薄膜的反常群速色散

通过对ＰＰＱ薄膜的吸收光学谱的计算分析，由Ｋｒａｍｅｒｓ－Ｋｒｏｎｉｇ关系得到ＰＰＱ膜在５５０ｎｍ～７００ｎｍ左右波段存在负群速色散区，并且色散量对相对较小，│β２│〉１．２ｐｓ＾２／ｍ，这使得对飞秒激光脉冲在ＰＰＱ平面光波导中的传输的传输的描述可以忽略色散顶，根据这一间化，仅考虑自相位调制（ＳＰＭ）效应，由于飞秒对撞锁激光脉冲的光谱展宽民计算的ＰＰＱ的非线性折射率系数ｎ２，与报道的结果吻合很好。     

富勒烯有机-无机杂化材料的非共珍三阶非线性光学特性

采用中心波长800 nm、脉宽30 fs的超短激光脉冲,通过飞秒光开关技术(Optical Kerr Shutter,OKS)对富勒烯有机-无机杂化材料的飞秒超快非线性特性进行了实验研究.获得270 fs的开关时间,所得的富勒烯有机-无机杂化材料的三阶非线性系数X~(3)约为4.5×10~(-4) esu,比C_(60)分子的三阶非线性系数X~(3)高一个数量级.通过实验测定的光克尔信号强度与激发光和探测光偏振方向夹角的依赖关系表明:30 fs的超短激光脉冲激发富勒烯有机-无机杂化材料的克尔信号主要是源于光诱导双折射效应,而非用200 fs的超短激光脉冲时来自瞬态栅的自衍射效应.     

富勒烯有机-无机杂化材料的非共珍三阶非线性光学特性

采用中心波长800 nm、脉宽30 fs的超短激光脉冲,通过飞秒光开关技术（Optical Kerr Shutter,OKS）对富勒烯有机-无机杂化材料的飞秒超快非线性特性进行了实验研究.获得270 fs的开关时间,所得的富勒烯有机-无机杂化材料的三阶非线性系数χ(3)约为4.5×10－14 esu,比C60分子的三阶非线性系数χ(3)高一个数量级.通过实验测定的光克尔信号强度与激发光和探测光偏振方向夹角的依赖关系表明：30 fs的超短激光脉冲激发富勒烯有机-无机杂化材料的克尔信号主要是源于光诱导双折射效应,而非用200 fs的超短激光脉冲时来自瞬态栅的自衍射效应.     

Flat Supercontinuum Generation at 1550 nm in a Dispersion-Flattened Microstructure Fibre Using Picosecond Pulse

The generation of a flat supercontinuum of over 80nm in the 1550nm region by injecting 1.6ps 10 GHz repetition rate optical pulses into an 80-m-long dispersion-flattened microstructure fibre is demonstrated. The fibre has small normal dispersion with a variation smaller than 1.5 （ps·nm^-1·km^-1） between 1500 and 1650nm. The generated supercontinuum ranging from 1513 to 1591 nm has the flatness of ±1.5 dB and it is not so flat in the range of several nanometres around the pump wavelength 1552nm. Numerical simulation is also used to study the effect of optical loss, fibre parameters and pumping conditions on supercontinuum generation in the dispersion-flattened microstructure fibre, and can be used for further optimization to generate flat broad spectra.     

Supercontinuum generation in seven-core photonic crystal fiber pumped by a broadband picosecond pulsed fiber amplifier

We report a supercontinuum source generated in seven-core photonic crystal fibers(PCFs) pumped by a self-made all-fiber picosecond pulsed broadband fiber amplifier. The amplifier's output average power is 60 W at 1150 nm with spectral width of 260 nm, and its repetition rate is 8.47 MHz with pulse width of 221 ps. With two different lengths of seven-core PCF, different output powers and spectra are obtained. When a 10 m long seven-core PCF is chosen, the output supercontinuum covers the wavelength range from 620 nm to 1700 nm, with the output power of 11.7 W. With only 2 m long seven-core PCF used in the same experiment, the wavelength of the supercontinuum spans from 680 nm to 1700 nm,with the output power of 20.4 W. The results show that the pulse width is 385 ps in the 10 m long seven-core PCF and 255 ps in the 2 m long one, respectively, due to the normal dispersion of the PCF.     

利用锁模光纤激光器在色散位移光纤中产生超连续谱的研究

采用主动锁模光纤激光器输出的重复频率10GHz、脉宽7．97ps的脉冲作为抽运光源,无需压缩后直接抽运4．2km的普通色散位移光纤(DSF)．利用色散位移光纤中自相位调制、交叉相位调制等非线性效应的联合作用,获得了20dB带宽达125nm、覆盖整个C波段、L波段和部分S波段的超连续(SC)谱。实验研究了抽运光脉冲峰值功率和抽运波长对超连续谱宽度的影响,结果表明抽运光脉冲峰值功率越高,得到的超连续谱的带宽越宽;通过对抽运波长的优化,可以实现最大程度的超连续展宽;分析了滤波器带宽对脉冲质量的影响;利用0．4nm带宽的可调谐滤波器对从超连续谱中滤出脉冲的特性进行了研究,在超连续谱的不同波长处获得了脉宽为8．90～9．80ps、时间一带宽积为0．44～0．49的稳定的窄光脉冲。     

生物医学领域中超连续激光光谱技术的研究进展

超连续谱激光指的是当泵浦激光穿过特殊光波导时,一系列的非线性效应引起入射激光束的光谱展宽,从而输出宽光谱激光束。随着超快激光和光子晶体光纤技术的发展,利用超短脉冲在光子晶体光纤中的传播链产生相干的且亮度高的超连续谱激光成为了一种理想的白光源。自从超连续谱激光源投入应用以来,其应用领域越来越广。尤其在生物医学的细胞、血液等样品分析当中,荧光光谱学、流式细胞仪、共焦显微、光学相干层析等技术都是强有力的分析工具,在采用这些先进技术的科学仪器中,超连续谱激光源成为了一种主要光学部件。首先对超连续谱激光源的国际研究进展作了详细介绍,然后对超连续激光光谱技术在显微成像、流式细胞仪、荧光寿命成像显微、荧光共振能量转移、光学相干层析、共焦显微生物医学分析等生物医学领域中的发展及应用作了综合阐述。对超连续激光光谱技术在非接触式血液制品鉴别的需求、方案及研究进展进行了重点论述,包括覆盖400～2 000 nm光谱范围的光纤化轻型超连续谱激光光源研究;采用超连续谱激光光谱方法探索不同物种血液的种属特征;根据大数据的血液样品光谱特征元数据库分析建立数学模型,利用数学模型实现对血液样品种属光谱学判定;血液鉴别光谱分析便携式整机系统研发等。对超连续激光光谱技术在生物医学领域的应用前景作了展望。     

Supercontinuum generation at 1.55μm using highly nonlinear photonic crystal fiber for telecommunication and medical applications

In this paper, we present a theoretical calculation of a highly nonlinear germanium (Ge) doped photonic crystal fiber with all-normal group velocity dispersion to design a supercontinuum (SC) light source at 1.55 μm. By doping 3% higher refractive index Ge inside the host silica, the nonlinear coefficient is increased to a value as large as 60.5 W^?1 km^?1 at 1.55 μm. A 10 dB bandwidth of a 120 nm SC spectrum for a 2.5 ps input optical pulse and a 10 dB bandwidth of a 190 nm SC spectrum for a 1.0 ps input optical pulse have been found using the same fiber length of 200m and input optical power of 18 W. The coherent lengths of the generated SC light sources are found to be 8.8 μm for a 2.5 ps input optical pulse and 5.6 μm for a 1.0 ps input optical pulse. Therefore, the highest longitudinal resolution at 1.55 μm is found to be about 4.0 μm for biological tissues.     

Parametrically amplified ultrashort pulses from a shaped photonic crystal fiber supercontinuum

By seeding a noncollinear optical parametric amplifier with a photonic crystal fiber supercontinuum, temporally well-defined amplified output pulses have been generated with durations down to 13 fs. The phase of the supercontinuum seed has been characterized by the ZAP-SPIDER technique and can be tailored with a femtosecond pulse shaper. Thus, a very flexible source for arbitrarily shaped, amplified ultrashort laser pulses has been realized.     

High-efficiency generation of a supercontinuum in an optical fiber

The results of experimental studies of high-efficiency generation of a supercontinuum in different types of single-mode optical fibers by pulses with a width of ～20 ps and with a wavelength widely tunable within the regions of normal and anomalous dispersion of the fibers are reported. A high efficiency of transformation of initially monochromatic radiation into a wide-spectrum supercontinuum with intense wings (in the range of 1000–2100 nm at a transformation efficiency of 95%) is demonstrated.     

Yb:CaF2–YF3 transparent ceramics ultrafast laser at dual gain lines

Yb³⁺:CaF₂-YF₃ transparent ceramics with excellent optical quality was successfully fabricated by hot-pressed method. Pulsed laser properties of this ceramics were investigated for the first time. Laser diode (LD) was applied as the pump source to generate a dual-wavelength mode-locked (ML) laser. The maximum average output power was 310 mW, which represents the highest output power of ultrafast calcium fluoride ceramic laser. The spectrum separated at 1048.9 nm and 1049.7 nm with a total pulse duration of 8.9 ps. The interval period between the beating signals was about 4.3 ps, corresponding to a 0.23 THz beat pulse repetition rate. These results demonstrate its potential in producing dual-wavelength ultrashort pulses. These Yb³⁺:CaF₂-YF₃ ceramics with low-cost and short-preparation period are ideal candidate materials for ultrafast lasers.     

7 W all-fiber supercontinuum source

Combine a section of photonic crystal fiber and a picosecond fiber laser to realize an all-fiber supercontinuum source. The picosecond laser exhibits 20 W average output power, 14 ps pulse duration at 480MHz repetition rate. Approximately 7 W supercontinuum with over 1100 nm spectral range is obtained with an optical-optical conversion efficiency of 34%. Further improvements for higher average power are discussed in this paper.     

Chirped pulse amplification in single mode Tm:fiber using a chirped Bragg grating

We report femtosecond pulse generation and chirped pulse amplification in Tm:fiber. A mode-locked oscillator operating in the soliton regime produced 800 fs pulses with 5 nm spectral bandwidth, at 40 pJ pulse energy. This oscillator seeded a pre-amplifier that utilizes a Raman soliton self-frequency shift to produce wavelength tunable pulses with 3 nJ energy, reduced pulse duration of 150 fs, and increased bandwidth of 30 nm. For further amplification, the pulses were stretched up to 160 ps using a chirped Bragg grating (CBG). Stretched pulses were amplified to 85 nJ after compression in single-mode Tm:fiber and recompressed with the CBG as short as 400 fs. Compressed pulses were coupled into a highly nonlinear tellurite fiber to investigate the potential of this ultrashort pulse 2-μm fiber source as a pump for mid-IR supercontinuum generation.