Mode-Locked Bi-Doped All-Fiber Laser With Chirped Fiber Bragg Grating

We demonstrate a bi-doped fiber laser with dispersion compensation provided by a linearly chirped fiber Bragg grating. Reliable self-starting mode-locking was achieved by using an InGaAsN semiconductor saturable absorber mirror. The all-fiber laser generated short optical pulses with a duration of 1.9 ps at ~ 1165 nm. The large anomalous dispersion of the fiber grating ensured operation in the soliton pulse regime. This in turn enabled us to increase the repetition rate of the output pulse train up to 100.6 MHz via harmonic mode-locking.     

Frequency tuning and pulse generation in a fiber laser with anintracavity semiconductor active filter

The authors demonstrate optical frequency tuning by direct electrical means as well as FM and AM mode-locking in an erbium-doped fiber laser with an intracavity distributed Bragg reflector active filter/modulator. They obtained a 6 nm discrete tuning range and pulses of 38 and 78 ps duration in AM and FM mode-locking, respectively     

Active mode-locking of 1.3 μm extended-cavity silicon chip Braggreflector laser

The authors report active mode-locking of an extended-cavity silicon chip Bragg reflector laser. Pulses of 27 ps duration at repetition rates up to 7 GHz, have been achieved with a controllable narrow optical spectrum     

Integrated Low-Jitter 400-MHz Femtosecond Waveguide Laser

An integrated passively mode-locked waveguide laser generating 440-fs pulses at 394-MHz repetition rate is demonstrated on an 18 mm $, times ,$44 mm silica waveguide chip. The laser self-starts, and uses a saturable Bragg reflector for mode-locking.      

Erbium-ytterbium waveguide laser mode-locked with a semiconductorsaturable absorber mirror

Picosecond pulses are produced using a semiconductor saturable absorber mirror in a laser based on an Er-Yb codoped planar waveguide amplifier. Continuous-wave mode-locking (CWML) with 9.8-ps pulses is obtained at repetition rates up to 100 MHz. With intracavity spectral filtering, saturable pulsewidths of 1 ps are achieved, and tunable picosecond pulses are obtained from 1534 to 1553 nm. Absorber characterization suggests that two-photon absorption within the saturable absorber mirror influences the CWML stability     

Optical signal generation at millimeter-wave repetition rates usingsemiconductor lasers with pulsed subharmonic optical injection

A new technique is presented and investigated systematically which generates optical signals at millimeter-wave repetition rates from a semiconductor laser, without the need for an intracavity saturable absorber. Optical pulses are generated from a long-cavity semiconductor laser with a repetition rate equal to its cavity resonant frequency by injecting short optical pulses at one of the cavity resonance subharmonics. A rate-equation model is proposed to explain the mechanism of this subharmonic optical injection method. Optical pulses with repetition rates of 35 and 56 GHz are generated using the proposed scheme from a semiconductor laser with a distributed Bragg reflector and a Fabry-Perot laser diode, respectively. The performance of the generated pulses is also evaluated in terms of detected RF power at the repetition frequencies, the subharmonic suppression ratio, phase noise, and timing jitter as a function of frequency detuning, injected optical power, laser bias current, and, finally, the subharmonic number. It is found that the generated optical pulses exhibit large subharmonic suppression ratio (>17 dB), large locking ranges >400 MHz, low levels of phase noise (~-93 dBc/Hz@10 kHz) and timing jitter (<0.41 ps over 100 Hz to 10 MHz), and large tolerance to variations in operating parameters     

高次谐波锁模飞秒掺镱光纤激光器的噪声情况

高重复频率的飞秒激光在高速激光测距和三维成像等领域有着非常重要的作用。其中基于飞秒光纤激光器的高次谐波锁模是获得GHz量级以上高重复频率脉冲的重要手段之一。基于含腔内光栅对色散补偿的非线性偏振旋转（NPR）锁模的掺镱（Yb）光纤激光器,在180 mW泵浦光时获得了稳定的143 MHz基频锁模脉冲序列,当泵浦光功率升至1 W时获得了最高20次谐波（2.86 GHz）锁模脉冲序列输出。系统地对比研究了基频锁模与高次谐锁模状态下,脉冲重复频率精密锁定后的艾伦偏差和相位噪声,7次谐波锁模状态下重复频率锁定精度能够保持在10?13 Hz@1 s的稳定度,为高次谐波锁模飞秒激光脉冲序列用于精密测量提供了实验依据。     

Wavelength and Repetition-Rate Tunable Mode-Locked Semiconductor-Seed-Source for Yb-Fiber-Amplifier Systems

We present a wavelength and repetition-rate tunable passively mode-locked semiconductor-seed-source for ytterbium-doped fiber amplifiers (YDFAs). Ultrashort pulses 2-6 ps in duration are generated over a broad tuning range of 1030-1090 nm, while passive harmonic mode-locking permits pulse repetition rates to vary from 500 MHz to over 5 GHz. We compare the amplification characteristics under fundamental and eighth harmonic mode-locking using a single-mode YDFA.     

An experimental and theoretical study of high repetition rate Q-switched Nd: YA1G lasers

An acoustooptic loss modulator made by bonding an X-cut quartz transducer to a fused silica scattering medium offers a practical means for repetitively Q-switching continuously pumped Nd : YAlG lasers at repetition rates up to 50 kHz. The peak power output of a multitransverse mode laser is typically enhanced by a factor of about 500 relative to CW operation at low (≪5 kHz) repetition rates and by larger factors when the transverse mode structure is suitably restricted. At high repetition rates, the peak power becomes smaller and the average power output approaches the CW level. The theoretical Q-switching behavior derived from the rate equations governing an ideal four-level laser is presented in graphical form, and is found to describe the observed behavior well when the laser is restricted to oscillation in the TEM00transverse mode. Similar calculations for Q-switched intracavity second harmonic generation indicate that the peak output power available at the second harmonic slightly exceeds that available at the fundamental, and that the harmonic coupling necessary to optimally couple the Q-switched laser is several orders of magnitude smaller than that required for CW intracavity conversion. Experiments using Ba2NaNb5O15For intracavity Q-switched harmonic generation roughly verified these predictions. A peak power output of 220 watts at 0.532 µ in the TEM00mode was achieved. Surface pitting of the nonlinear crystal after a few hours of operation prevented a thorough comparison with the calculated results. Preliminary experiments using the doubled Q-switched Nd : YAlG laser and an ammonia dihydrogen phosphate crystal to generate ultraviolet (the 0.266-µ harmonic) yielded a peak output power of 40 watts.     

Gigabit optical pulse generation with FM mode-locked LiNdP4O12lasers

FM mode locking of an LiNdP4O12(LNP) laser with an intracavity modulator is reported. Mode-locked optical pulses with a pulse width of 49 ps at a repetition rate of 960 MHz, corresponding toc/2L(c:light velocity,L:cavity length), have been obtained. A pulse repetition rate as high as 2.88 GHz has been achieved with a multiple mode-locking technique.     

Tuning characteristics of monolithic passively mode-lockeddistributed Bragg reflector semiconductor lasers

Tuning characteristics of multicontact passively mode-locked distributed Bragg reflector (DBR) semiconductor lasers are investigated in terms of center wavelengths and pulse repetition frequencies. It is shown that the center wavelength of the pulses can be tuned over a wide range by changing the refractive index of the Bragg reflector section either by means of carrier injection or by thermal effects while maintaining the pulses to be nearly transform-limited. Tuning of the pulse repetition rates is realized by using four different approaches, i.e., current injection to a passive phase-control section, varying of the reverse bias to the absorber, varying of the injection current to the gain region, and thermal effects. Injecting current into the phase-control region results in a tuning range of more than 400 MHz while maintaining the pulses at transform-limited condition. Varying the reverse bias voltage to the absorber is shown to be an alternative to achieve large repetition rate tuning, by which a tuning range of 600 MHz is obtained. By combining these tuning schemes, a total tuning range of more than 1 GHz is realized     

Repetition-rate-multiplication in actively mode-locking fiber laser by using phase modulated fiber loop mirror

We demonstrate a simple scheme to multiply the repetition rate in an actively mode-locking fiber laser by using a phase modulated optical fiber loop mirror (PMOLM). The PMOLM can convert phase modulation to amplitude modulation at double the modulation frequency. In principle, it is easy to double the repetition rate. However, the PMOLM also induces residual chirp which can disable this method in some cases. Numerical simulation shows that the best results can be obtained when the intracavity dispersion is negative and the modulation frequency is an odd harmonic of half of the cavity fundamental frequency. This agrees with the experimental results, in which an 80-GHz 1.74-ps transform limited pulse was obtained. By using rational harmonic modulation which requires detuning the modulation frequency and adjusting the modulation index, the repetition rate can be increased by three or four times.     

Characteristics of dispersion-tuning in harmonically mode-lockedfiber laser

We investigate the characteristics of dispersion-tuning in an actively mode-locked fiber ring laser. A continuous tuning range over 20 nm at about 1-GHz operation is realized. The range can be extended by optimizing the polarization to attain a flattened spectral gain in the Er-doped fiber. The influence of the harmonic order of operation together with the amount of dispersion in the fiber ring have been experimentally studied. Rational harmonic mode-locking is first demonstrated in the dispersion-tuned laser to increase the output repetition rate. Our results agree well with theory, showing that dispersion-tuning is a reliable, economic, and effective way to generate widely tunable pulses     

石墨烯锁模的全保偏光纤激光器

报道了一种基于反射式石墨烯可饱和吸收镜锁模的全保偏掺铒光纤激光器。分别使用单层和十层石墨烯作为可饱和吸收器件,通过全保偏结构,避免了外界环境对腔内偏振态的影响,获得了高稳定性、高偏振度、易自启动的锁模脉冲输出,脉冲宽度分别为697 fs和502 fs。实验表明,十层石墨烯相比于单层石墨烯能够获得更窄的脉冲宽度,更高的峰值功率,具有好的锁模效果。研究同时发现,经十层石墨烯锁模,进一步提高泵浦功率,可在全保偏光纤腔中获得重复频率62.94 MHz的二阶谐波锁模脉冲输出。并通过非线性薛定谔方程对谐波锁模产生的机理进行了分析。这种基于反射式可饱和吸收镜的全保偏锁模光纤激光器有望成为实现基频锁模与谐波锁模可切换的单偏振激光源。     

Passive harmonic mode-locking in all-fibre soliton laser: energystates and stability aspects

The behaviour of a passively mode-locked soliton laser, under different energy states, is studied by using a numerical simulation. The shorter pulse obtainable is determined, pointing out the soliton properties of the output pulses. In the case of harmonic mode-locking, power quantisation related to the number of existing pulses in the cavity, is obtained and repetition rate instability is detected. It is found that by introducing a narrow band optical filter in the cavity and by optimising the filter bandwidth, this instability is substantially reduced     

Rational harmonic mode locking of an optically triggered fiberlaser incorporating a nonlinear optical loop modulator

Rational harmonic mode locking is first demonstrated in an erbium-doped fiber laser using an all-optical approach. Both bright and dark pulse trains up to 4.58 GHz are obtained at 1.55 μm by adjusting the initial reflection state of the intracavity loop mirror. The nonlinear loop modulator serves as a mode locker and an adjustable end reflector in the laser. The setup is useful for optional bit-rate multiplication while providing a means for the conversion of wavelength, as well as the conversion between bright and dark pulses. The output wavelength is also tunable upon the adjustment of a cavity fiber Fabry-Perot filter     

Synchronous mode-locking in passively mode-locked semiconductor laser diodes using optical short pulses repeated at subharmonics of the cavity round-trip frequency

Synchronous mode-locking was achieved in passively mode-locked semiconductor lasers using optical pulses with repetition rates at subharmonics of the cavity round-trip frequency. Stable and continuous mode-locked pulses at 8.5 GHz were generated when the repetition rate of the control optical pulses was 4.25 GHz (2nd subharmonic). The timing jitter of the mode-locked pulses was reduced to 1 ps. The relationship between repetition rates of the control pulses and the realization of stable and continuous mode-locking was examined.     

Intracavity contacts for low-threshold oxide-confinedvertical-cavity surface-emitting lasers

Very low threshold vertical-cavity surface-emitting lasers are demonstrated using intracavity contacts, an upper dielectric Bragg reflector, and an undoped lower AlAs-GaAs Bragg reflector. The undoped lower mirror allows the demonstration of the highest differential efficiency yet achieved for sub-100-μA threshold, which is 60% for a 67-μA threshold. Devices with smaller output coupling show threshold current densities as low 98 A/cm², and a minimum threshold current of 23 μA for a small aperture     

6 MHz重频调谐范围的稳定锁模掺镱光纤激光器

针对精密测量的实际应用需求,开发了具有6 MHz重复频率调谐范围的掺镱锁模光纤激光器。该光纤激光器利用啁啾光纤光栅实现色散补偿,可以实现不同色散域的锁模。实验中,系统研究了不同腔内净色散对锁模激光器输出特性和稳定性的影响,发现当具有一定负腔内净色散时,在不同的重复频率下都可以输出相同的光谱,同时输出光谱具有较好的高斯型。根据以上研究,特殊设计了稳定的简化腔结构和空间延迟线,同时优化了腔参数,保证了大范围的重复频率调谐和稳定的锁模运转。当中心重复频率为26 MHz 时,调谐比率达到23%。激光器稳定输出平均功率为3.23 mW的飞秒激光脉冲,去啁啾后脉冲宽度为347 fs。基于此,将光纤锁模激光器重复频率锁定于铷原子钟,在1 s的平均时间内获得了2×10?10的艾伦方差。     

有理数谐波锁模掺铒光纤环形激光器

在主动谐波锁模光纤环形激光器实验中获得数倍于调制频率ｆｍ的高重复率脉冲序列,其中ｆｐ＝２ｆｍ的输出脉冲序列极为稳定,所得的最高锁模脉冲重复频率ｆｐ＝４ｆｍ≈６ＧＨｚ。实验证实了一种被称之为有理数谐波锁模（ＲＨＭＬ—ＲａｔｉｏｎａｌＨａｒｍｏｎｉｃＭｏｄｅ－ｌｏｃｋｉｎｇ）新技术在较低的调制频率和极简单的腔构条件下也同样成立。实验观察到ＲＨＭＬ激光器允许失谐范围不小于±２ｋＨｚ,失谐比大于１０－６。