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1.
单偏振控制器环形腔光纤激光器实验研究   总被引:1,自引:0,他引:1  
申民常  徐文成  陈伟成  宋方  冯杰  刘颂豪 《光学学报》2007,27(11):2003-2007
理论分析了非线性偏振旋转环形腔作为类饱和可吸收体获得脉冲的物理机理。在光纤环形腔结构中,采用单个偏振控制器实现了非线性偏振旋转锁模,直接获得了脉冲宽度为131 fs的超短脉冲输出。实验中,采用性能稳定的976 nm半导体二极管激光器作为抽运源,使用高掺杂浓度的Er3 光纤为增益介质,通过调节偏振控制器,获得了光谱谱宽(3 dB带宽处)为23.5 nm的稳定锁模脉冲输出。脉冲中心波长为1535.9 nm,平均功率为5.91 mW,脉冲重复率为11.20 MHz。  相似文献   

2.
非线性放大环形镜“8”字腔光纤激光器实验研究   总被引:5,自引:3,他引:2  
张伟  陈国夫  赵卫  王屹山  李喆  侯洵 《光子学报》2006,35(12):1808-1811
使用976 nm半导体激光器作为抽运源,对利用非线性放大环形镜(NALM)锁模运行的掺Yb3+光纤激光器进行了实验研究,获得了脉冲宽度43.6 ps,中心波长为1053.3 nm的锁模脉冲激光输出, 光谱宽度8 nm, 输出功率为0.2 mW, 重复频率为18.2 MHz, 经过放大, 通过光栅对腔外色散补偿,在腔外产生了宽度616 fs的脉冲激光.  相似文献   

3.
Phase-matched parametric four-wave mixing in higher-order guided modes of a photonic crystal fiber is shown to result in an efficient decay of 40-fs 800-nm Ti:sapphire laser pump pulses into an anti-Stokes signal with a central wavelength around 590-600 nm and a Stokes signal centered at 1.25 microm. The photonic crystal fiber is designed in such a way as to minimize the group-velocity dispersion at the pump wavelength, phase match the parametric four-wave-mixing process, and reduce the group delay between the pump and the anti-Stokes pulses. The duration of the anti-Stokes pulse under these conditions, as shown by cross-correlation frequency-resolved optical gating measurements, is less than 200 fs.  相似文献   

4.
张攀政  范薇  汪小超  林尊琪 《物理学报》2011,60(2):24206-024206
讨论了利用光谱滤波器实现自启动的被动锁模掺Yb3+光纤环形激光器的锁模机理,并研制出全光纤结构超短脉冲掺Yb3+光纤环形激光器.使用980 nm二极管激光器作为抽运源,高掺杂浓度掺Yb3+光纤作为增益介质.在净群速度色散为正的环形腔中加入光谱滤波器,抑制Yb3+离子在1030 nm强发射峰的同时,通过对啁啾脉冲的光谱滤波实现脉冲压缩.光谱滤波器与光纤非线性偏振旋转效应相结合,实现了激光器在1053 nm可自启动、十分稳定的锁模运转.激光器锁模阈值功率300 mW,平均斜率效率18.3%,最大输出功率53.07 mW,对应最大输出脉冲能量3.2 nJ.锁模光脉冲中心波长1053.6 nm,3 dB带宽10.84 nm,重复频率16.45 MHz.锁模脉冲宽度为皮秒量级,经腔外光栅对压缩至188 fs. 关键词: 3+光纤激光器')" href="#">掺Yb3+光纤激光器 自启动锁模 全光纤  相似文献   

5.
A passively phase-locked laser source based on compact femtosecond Er:fiber technology is introduced. The carrier-envelope offset frequency is set to zero via difference frequency generation between a soliton at a wavelength of 2?μm and a dispersive wave at 860?nm generated in the same highly nonlinear fiber. This process results in a broadband output centered at 1.55?μm. Subsequently, the 40?MHz pulse train seeds a second Er:fiber amplifier, which boosts the pulse energy up to 8?nJ at a duration of 125?fs. Excellent phase stability is demonstrated via f-to-2f spectral interferometry.  相似文献   

6.
A saturable absorber is commonly employed to generate an ultrashort laser with a mode-locking scheme. In an erbium-doped fiber laser system, the laser regimes of either 1530 or 1550 nm wavelength are procured based on the absorption profile of the erbium-doped fiber. The absorption of the erbium-doped fiber is designed to emit at both wavelengths by controlling the net gain of the laser cavity. Subsequently, simultaneous erbium-doped fiber laser emission is attained at 1533.5 and 1555.1 nm with the pulse duration of 910 and 850 fs, respectively.Therefore, this work maximizes the output portfolios of a mode-locking fiber laser for dual-wavelength ultrashort pulses emission.  相似文献   

7.
We report what is believed to be the first demonstration of a high-power passively mode-locked diode-pumped femtosecond laser based on an Yb3+:CaF2 single crystal, directly pumped by a 15-W fiber-coupled laser diode. With a 5-at. % Yb3+ -doped sample and prisms for dispersion compensation we obtained pulses as short as 150 fs, with 880 mW of average power and up to 1.4-W average output power, with a pulse duration of 220 fs, centered at 1049 nm. The laser wavelength could be tuned from 1040 to 1053 nm in the femtosecond regime. Using chirped mirrors for dispersion compensation, the oscillator provided up to 1.74 W of average power, with a pulse duration of 230 fs, corresponding to a pulse energy of 20 nJ and a peak power of 85 kW.  相似文献   

8.
An original scheme of an all-fiber all-normal-dispersion ring mode-locked Yb laser is proposed and experimentally studied. A single fiber element serves as a wavelength-division multiplexer for the pumping radiation, an optical isolator, and a spectrally selective element for the radiation of the Yb laser. The output pulse duration is 900 fs, and the intracavity compression yields the pulses with a duration of 200 fs. The maximum laser power is 35 mW at a wavelength of 1070 nm.  相似文献   

9.
Sotor J  Sobon G  Abramski KM 《Optics letters》2012,37(11):2166-2168
All-polarization-maintaining, self-starting Erbium-doped fiber laser based on graphene-saturable absorber is presented. Scalar soliton pulses with 570 fs duration and 114.1 MHz repetition rate were achieved at a 1557 nm center wavelength and with 6 nm bandwidth. The graphene-saturable absorber was formed by mechanical exfoliation of pure graphite. The laser was environmentally stable and could operate for long periods of time with linearly polarized output and degree of polarization at the level of 98%.  相似文献   

10.
赵卫  杨鸿儒  王水才 《光学学报》2000,20(7):47-951
描述了用激光二极管抽运的全固体Nd:LMA自锁模飞秒激光振荡器,通过理论计算和分析,在其腔内加入-非线性系数较大的介质,同时对腔结构进行优化设计,实现了自锁模。它直接产生波长为1054nm的激光,输出激光脉冲的宽度达610fs,光谱宽度为2.1nm,输出功率达15mW。  相似文献   

11.
Compression of sub-nanojoule laser pulses using a commercially available photonic crystal fiber (PCF) with zero dispersion wavelength of 860 nm is discussed. A twofold pulse compression starting from 24 fs transform limited seed pulses around 800 nm is experimentally demonstrated as a verification of our simulations. Theory shows that by the optimization of input and output chirp parameters up to the third order, high quality, 5.7 fs pulses can be generated from a cost efficient experimental setup. Further calculations show that 1 ps pulses with central wavelength of 800 nm can be compressed down to 50 fs in the normal dispersion regime of the fiber with proper dispersion compensation. Calculations also show that dispersion flattened fibers can improve both the quality and the duration of compressed pulses. PACS 42.65.Re  相似文献   

12.
We report a femtosecond optical parametric oscillator based on MgO-doped PPLN synchronously pumped by a mode-locked Ti:sapphire laser. The wavelengths of the signal and idler are continuously tuned from 1100 to 1300hm and from 2080 to 2930nm, respectively, by changing the pump wavelength and the OPO cavity length. The maximum signal output power of 130mW at the wavelength of 1225nm is obtained, pumped by 900roW of 800hm laser radiation. This corresponds to a total conversion efficiency of 22.1%. The signal pulse duration is measured to be 167fs by intensity autocorrelation with chirped mirrors for intracavity dispersion compensation.  相似文献   

13.
We present a mode-locked ytterbium fiber laser with a higher-order mode fiber compensating the group-velocity dispersion and partially the third-order dispersion of the single-mode fiber at a wavelength of 1 microm. The generated pulses had an energy of 0.5 nJ and could be dechirped externally to a pulse duration of less than 60 fs. The power spectrum shows a spectral full width at half-maximum of 57 nm.  相似文献   

14.
A femtosecond fiber laser based on thulium-doped double-clad silica fiber with an internal dispersion compensation is presented that generates pulses at a center wavelength of 1976 nm with an energy of 4.3 nJ and a duration of 1.2 ps. The dechirped pulse duration is 294 fs. The pulse energy is more than 2 orders of magnitude above the pulse energy demonstrated previously. Mode locking is achieved using additive pulse mode locking, and dispersion compensation is facilitated by a grating stretcher arrangement.  相似文献   

15.
吕志国  杨直  李峰  李强龙  王屹山  杨小君 《物理学报》2018,67(18):184205-184205
高集成、高可靠性宽调谐飞秒激光源在超快光谱学、量子光学及生物成像等研究与应用领域具有重要价值.如在生物多光子显微成像中,具有适中能量的宽调谐飞秒激光源不仅可满足多种生物组织荧光激发所需的峰值功率与激发波长,而且也可以显著提升非线性荧光产生效率、成像分辨率以及增大成像穿透深度.采用自主研发的高可靠性全保偏光纤飞秒激光器作为抽运源,基于低色散光纤中高峰值功率飞秒激光脉冲非线性传输引起的光谱加宽机制,本文开展了多波长全光纤飞秒激光产生技术研究.通过采用中心波长在980, 1000,1050, 1070与1100 nm的带通滤波片选择性地对单模光纤输出光谱中最左边与最右边光谱旁瓣进行滤波,在上述中心波长处分别可获得203, 195, 196, 187与194 fs的激光输出.本文提出的基于全光纤飞秒激光脉冲在单模光纤中非线性传输引起的光谱加宽机制与特定光谱选择技术的实验方案为高集成、高可靠性宽调谐飞秒激光源的实现提供了新的研究途径.  相似文献   

16.
The initial results of the experimental and numerical study of a fiber supercontinuum generator based on a wavelength-tunable femtosecond Yb:KYW laser are presented. It is demonstrated that a variation in the pumping wavelength in the vicinity of the zero-dispersion wavelength of a microstructured fiber at about 1040 nm allows for a wide-range variation in the supercontinuum spectral width at a constant mean pumping power. The experimentally measured strong dependence of the supercontinuum spectral width (from 70 to 390 nm) on the pumping wavelength (1040–1049 nm) at a pulse energy of about 1 nJ and a pulse duration of 250 fs is qualitatively reproduced in the simulation.  相似文献   

17.
X. Yang  C. X. Yang 《Laser Physics》2009,19(11):2106-2109
An erbium-doped fiber laser based on nonlinear polarization rotation (NPR) and negative group velocity dispersion (GVD) is built up. Two different Q-switched mode-locked (QML) operation states which can be distinguished by the properties in time and frequency domains are demonstrated. Besides the QML, stable continuous-wave mode-locked pulses centered at 1560 nm wavelength with pulse-width of 670 fs, harmonic mode-locking, Q-switching, and pulse splitting have been observed, respectively.  相似文献   

18.
锁模脉冲波长连续可调谐光纤激光器   总被引:2,自引:1,他引:1  
利用在腔内加入可调谐光纤光栅滤波器使“8”字形腔掺Yb3+光纤激光器在锁模状态下实现波长连续可调谐.实验中,在保证锁模状态稳定的情况下,通过调节可调谐光纤光栅滤波器,使激光器输出锁模脉冲的中心波长在1 047 nm~1 055 nm范围内连续调谐,重复频率稳定维持在4.9 MHz.在中心波长1 053 nm处,测得锁模脉冲输出平均功率为8.02 mW,光谱带宽1 nm,脉冲宽度为259.3 ps.这种“8”字形腔被动锁模光纤激光器在锁模状态下对波长连续可调谐,并可长时间稳定工作.  相似文献   

19.
Single-mode Nd3+-doped phosphate glass fiber with a core diameter of 8 μm was prepared. Laser properties pumped by an 800 nm laser diode were measured using a Fabry-Petor cavity. Laser emission centered at the wavelength of 1.053 μm,and a 1.053 μm CW laser with output power of 8.36 mW and slope efficiency of 30.6% were observed.  相似文献   

20.
沈忠伟  王兆华  范海涛  秦爽  滕浩  何鹏  魏志义 《物理学报》2014,63(10):104211-104211
针对高能量千赫兹重复频率飞秒激光的应用需求,设计了一套采用线性再生腔结构的高效率飞秒钛宝石激光啁啾脉冲放大系统.通过优化腔型设计,在重复频率为1 kHz、单脉冲能量为20 mJ的527 nm激光抽运下,将展宽后的800 nm啁啾脉冲激光的能量放大到5.8 mJ,对应斜效率达到30.7%.进一步通过色散补偿压缩脉冲宽度,获得了单脉冲能量为4 mJ、脉冲宽度为45.7 fs的输出,稳定性测量表明激光的能量抖动仅为0.18%(均方根值).  相似文献   

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