Pulse generation by distributed feedback dye lasers

Equations describing the pulse generation by distributed feedback dye lasers are derived and solved by analytical methods. The dependence of the laser output on macroscopic parameters is discussed.On leave from the Department of Physics, Friedrich-Schiller-University, DDR-6900, Jena, German Democratic Republic     

Ultrashort pulse generation by distributed feedback dye lasers. II

The properties of distributed feedback dye lasers as novel sources for wavelength tunable ultrashort pulses in the visible and ultraviolet range are studied. Calculated and measured energy characteristics of the laser are in very good agreement. The shot-to-shot stability of the single ultrashort pulses has been measured to be ±7.1%.     

Ultrashort pulse generation by distributed feedback dye lasers. I

The N₂-laser pumped distributed feedback dye laser is a new type of picosecond light source. A rate equation model describing the ultrashort pulse formation is presented. The temporal behavior of the distributed feedback dye laser predicted by the model has been compared with experimental results obtained with a streak camera system. The observed good agreement allows application of the theoretical model for the engineering of an inexpensive picosecond laser     

Improved line narrowing and wavelength stabilization technique of distributed feedback dye lasers

A new method is described, for the wavelength stabilization and line narrowing of DFB dye lasers, using a dispersive pumping arrangement, where the wavelength shift of pumping light is compensated by a change in the incident beam angle. A predicted relation between pumping wavelength shift and DFB laser wavelength shift is verified experimentally. A twentyfold line narrowing in comparison with pumping linewidth, is realised in a preliminary experiment.     

Biharmonic pumping in dye lasers with distributed feedback

Conclusions We have shown that biharmonic pumping can effectively excite traveling population gratings in an active medium when m <(W_o/2 +1/T₁), and temperature gratings if m <(₀x_m)^–1. As the order m increases the population-grating excitation efficiency decreases, while that of the temperature gratings may either increase or decrease. The times taken for the thermal and resonance processes which form the gratings to build up are given by the expressions t=₀x_m, t =T₁/(1 +W₀T₁/2), respectively. In this case distributed feedback is formed by a thermal mechanism if (14) is satisfied, and by resonance mechanism if the opposite inequality is satisfied. The self-excitation threshold over a wide range of parameters depends logarithmically on the amplitude of the grating forming the distributed feedback. Hence, for a comparatively small excess of the threshold, self-excitation of a laser with distributed feedback is possible over a wide spectrum. Thus, for double excess of the self-excitation threshold and T₁ =10^–9 sec, =1, and H =8 lasing over a wide spectrum of 10 cm^–1 is possible.Translated from Zhurnal Prikladnoi Spektroskipii, Vol. 40, No. 2, pp. 195–202, February, 1984.We wish to thank A. A. Afanasev and P. A. Apanasevich for useful discussions.     

New jet stream technique for dye lasers

We report on a novel technique for generating large area flowing sheets of viscous fluids for use in dye lasers. The proposed technique allows one to control the shape, size and thickness of the fluid sheets of excellent optical quality. Rhodamine 6G/ethylene glycol jet streams have been investigated. Application to other dye/solvents, to saturable absorbers or to other fluids is straightforward.     

Simultaneous operation of distributed feedback and grating tuned dye lasers

Multiphoton absorption (MPA) of the CO₂ laser 9 μmR(30) line (pulse width 60 ns, FWHM) by NH₃ and NH₃/N₂ mixtures was studied as a function of gas composition, pressure and laser fluence (Φ). MPA occurs for Φ smaller than those that have been used for optically pumped NH₃/N₂ lasers; consequently a simple two-level absorption model will not adequately describe laser action in these systems. The photon energy deposited in NH₃/N₂ mixtures can be calculated from the MPA cross-section and the fluence dependence of the illumination geometry. An examination of the efficiency of conversion of this absorbed energy to the reported radiant energy of optically pumped NH₃/N₂ lasers shows an optimum value which depends on pressure, and gas composition.     

Large-signal modulation in distributed feedback quantum cascade lasers for coherent multiharmonic signal generation

In this Letter, an experimental analysis for coherent multiharmonic signal generation in quantum cascade lasers is presented. The underlying principle relies on the direct modulation of the laser with a large sinusoidal wave to drive the laser above and below threshold. This generates a multiharmonic optical signal in the frequency domain as the device is forced to respond in a nonlinear fashion. The impact of the modulation parameters is assessed in the resultant optical spectrum of a continuous-wave distributed feedback quantum cascade laser. Despite not creating pulses due to the ultrafast dynamics of the laser, the results reveal that a comb structure with uniform line spacing and high phase correlation between teeth can be straightforwardly generated.     

Raman fiber distributed feedback lasers

We demonstrate fiber distributed feedback (DFB) lasers using Raman gain in two germanosilicate fibers. Our DFB cavities were 124 mm uniform fiber Bragg gratings with a π phase shift offset from the grating center. Our pump was at 1480 nm and the DFB lasers operated on a single longitudinal mode near 1584 nm. In a commercial Raman gain fiber, the maximum output power, linewidth, and threshold were 150 mW, 7.5 MHz, and 39 W, respectively. In a commercial highly nonlinear fiber, these figures improved to 350 mW, 4 MHz, and 4.3 W, respectively. In both lasers, more than 75% of pump power was transmitted, allowing for the possibility of substantial amplification in subsequent Raman gain fiber.     

Pulse linewidth and lifetime broadening study of multi-pulse pumped distributed feedback dye lasers

Results on characterization of spectral width and lifetime broadening mechanism in picoseconds multiple-pulse pumped distributed feedback dye lasers (DFDL) is presented. An experimental study was carried out to investigate the impact of pump pulse energy, dynamic grating length and dye concentration on the spectral width and lifetime characteristics of single and multi-pulse pumped DFDL. To implement this study the solution of Rh6G in ethanol was pumped by 2nd harmonic of a passively q.switched and modelocked ND:YAG laser. Further to study the effect of grating chirp factor on spectral characteristics of the luminescence spectra of the DFDL, the dye cell was pumped by multiple time delayed pulses. Results show that pump power, grating length, dye concentrations and temperature effects cause spectral and life time broadening of simultaneously oscillating multiple lasing lines.     

Random distributed feedback fibre lasers

The concept of random lasers exploiting multiple scattering of photons in an amplifying disordered medium in order to generate coherent light without a traditional laser resonator has attracted a great deal of attention in recent years. This research area lies at the interface of the fundamental theory of disordered systems and laser science. The idea was originally proposed in the context of astrophysics in the 1960s by V.S. Letokhov, who studied scattering with “negative absorption” of the interstellar molecular clouds. Research on random lasers has since developed into a mature experimental and theoretical field. A simple design of such lasers would be promising for potential applications. However, in traditional random lasers the properties of the output radiation are typically characterized by complex features in the spatial, spectral and time domains, making them less attractive than standard laser systems in terms of practical applications. Recently, an interesting and novel type of one-dimensional random laser that operates in a conventional telecommunication fibre without any pre-designed resonator mirrors–random distributed feedback fibre laser–was demonstrated. The positive feedback required for laser generation in random fibre lasers is provided by the Rayleigh scattering from the inhomogeneities of the refractive index that are naturally present in silica glass. In the proposed laser concept, the randomly backscattered light is amplified through the Raman effect, providing distributed gain over distances up to 100 km. Although an effective reflection due to the Rayleigh scattering is extremely small (∼0.1%), the lasing threshold may be exceeded when a sufficiently large distributed Raman gain is provided. Such a random distributed feedback fibre laser has a number of interesting and attractive features. The fibre waveguide geometry provides transverse confinement, and effectively one-dimensional random distributed feedback leads to the generation of a stationary near-Gaussian beam with a narrow spectrum. A random distributed feedback fibre laser has efficiency and performance that are comparable to and even exceed those of similar conventional fibre lasers. The key features of the generated radiation of random distributed feedback fibre lasers include: a stationary narrow-band continuous modeless spectrum that is free of mode competition, nonlinear power broadening, and an output beam with a Gaussian profile in the fundamental transverse mode (generated both in single mode and multi-mode fibres).     

Nine-thousand-fold pulse shortening by an excimer laser-pumped cascade of two distributed feedback dye lasers

Transform-limited single pulses of 2.6 ps and 1.7 ps duration are generated in the red spectral region by an excimer laser-pumped cascade of two distributed feedback dye lasers. Compared with the 15 ns-long excimer pumping pulse, these pulse durations mean pulse shortening of 6000 and 9000 times, respectively.     

具有内部相移的分布反馈半导体激光器电路模型

以耦合波方程为基础,经过适当的近似处理,给出一个比较简单的适用于有内部相移的单模分布反馈半导体激光器电路模型。该模型可用于直流、交流和瞬态分析。适于在开发光电集成回路电路级模拟软件中采用,亦可加入到现有电路模拟软件中。     

Relaxation oscillations in distributed feedback lasers

Using approximate solutions for over-coupled (KL > 1) distributed feedback lasers above threshold and a small-signal perturbation analysis, the frequency and damping of DFL relaxation oscillations are calculated.     

Two-photon-pumped distributed feedback zirconia waveguide lasers

Distributed feedback laser action of narrow line-width output was demonstrated in zirconia waveguides doped with trans-4-[p-(N-hydroxyethyl-N-methylamino) styryl]-N-methylpyridinium p-toluene sulfonate, a compound of strong two-photon up-converted emission near 620 nm. Single-beam pumping at 1.06 m led to intense up-converted amplified spontaneous emission at 620 nm. Transient gratings for coherent scattering were generated in the waveguides by crossing two 1.06-m beams. Narrow line-width distributed feedback laser emission was observed at 627 nm. PACS 42.55.Mv; 42.70.Jk; 42.79.Gn     

面发射分布反馈半导体激光器

本文详细阐述了面发射分布反馈半导体激光器(SE-DFB-LD)的基本工作原理、结构设计及其工作性能,针对国内外研究最新进展与发展现状进行了总结和评述,并在此基础上,对面发射半导体激光器的研究工作和发展趋势做出了进一步的讨论和展望。随着面发射分布反馈半导体激光器各性能指标的不断优化提升和后期加工、装调技术的逐渐成熟,其将不断满足科学研究及工业、军事等实际应用领域对半导体激光器的需求,具有很大的发展潜力。     

Offset quantum-well method for tunable distributed Bragg reflector lasers and electro-absorption modulated distributed feedback lasers

Tunable distributed Bragg reflector (DBR) lasers are essential components for future optical fiber communi- cation systems[1]. A tunable laser can replace a large number of distributed feedback (DFB) lasers as sparing source in wavelength division multiplexing (WDM) sys- tems. Moreover they allow flexible switching and routing for distributed data in future network[2]. There are several methods for integrating gain sec- tion with DBR section, such as butt-joint method, bundle method, and …     

Offset quantum-well method for tunable distributed Bragg reflector lasers and electro-absorption modulated distributed feedback lasers

A two-section offset quantum-well structure tunable laser with a tuning range of 7 nm was fabricated using offset quantum-well method. The distributed Bragg reflector (DBR) was realized just by selectively wet etching the multiquantum-well (MQW) layer above the quaternary lower waveguide. A threshold current of 32 mA and an output power of 9 mW at 100 mA were achieved. Furthermore, with this offset structure method, a distributed feedback (DFB) laser was integrated with an electro-absorption modulator (EAM),which was capable of producing 20 dB of optical extinction.