Ce travail est consacré à l’étude des interactions d’un grand nombre de solitons dans un laser à fibre dopée erbium/ytterbium. Les impulsions interagissent entre elles et se structurent pour former des distributions plus ou moins organisées. Deux cavités ont été réalisées, l’une basée sur la rotation non-linéaire de la polarisation (RNLP) et l’autre sur le miroir optique à boucle non-linéaire (NOLM) en configuration de laser en forme de huit. Avec la RNLP, nous nous sommes intéressés d’abord à une distribution où les impulsions sont liées (cristal de solitons). Ce cristal, stable pour des puissances moyennes, devient instable lorsque la puissance augmente : il se disloque. Les solitons se réorganisent pour former un régime de verrouillage harmonique (HLM) de 50 cristaux. Nous avons ensuite cherché s’il était possible de contrôler les distributions de solitons par l’injection d’une composante continue externe. Nous avons montré que le HLM peut être forcé par l’injection de cette composante. Nous avons développé deux approches afin de modéliser un laser verrouillé en phase et soumis à l'injection d'une composante continue, l'une est scalaire et l'autre vectorielle. Ces modèles démontrent que le signal injecté peut modifier les interactions entre les solitons. Enfin, le NOLM a permis d’observer plusieurs dynamiques : pluie de solitons, gaz de solitons, liquide de solitons, poly-cristal de solitons, multi-cristal de solitons, cristal de solitons, états liés et verrouillage harmonique d’états liés. Ce laser a permis également d’observer une émission laser continue et impulsionnelle autour de 1600 nm. / This work has been devoted to study the interaction of the large number of solitons in the erbium/ytterbium doped fiber laser. The interaction of pulses with each other causes to form more or less organized distribution. Two laser cavities have been constructed, one based on the non-linear polarization rotation (NLPR) and the other based on the nonlinear optical loop mirror (NOLM) in a figure-eight laser configuration. With the NLPR, we were interested to the distribution of coherent pulses (crystal solitons). This crystal, stable for moderate power, becomes unstable at high power, which means to get loose from the initial soliton. These solitons rearrange their relative position to form one harmonic-mode locking regime (HML) of 50 crystals. Afterward, we have investigated the possibility of controlling the solitons distribution by injecting an external continuous wave (cw). It has been observed that cw could force the laser to operate at HLM regime. Moreover, we have developed two theoretical approaches, such as scalar and vectorial, to model the passively mode-locked fiber laser submitted to the cw. Both models confirm that the injected signal could modify the interactions between the solitons. Finally, the NOLM allowed us to observe several dynamics, including rain solitons, gas solitons, liquid solutions, poly-crystal solitons, multi-crystal solitons, crystal solitons, bound states and harmonic-mode locking of bound states. Furthermore, it made possible to observe the continuous as well as pulsed laser emission around 1600 nm.

Les travaux de recherche, rapportés dans ce manuscrit, portent sur l’étude d’un laser à fibre en forme de huit et le développement de sources à 1.6 µm. En premier temps, nous avons étudié la dynamique impulsionnelle d’un laser à fibre micro-structurée en forme de huit. L’objectif est de montrer l’impact des propriétés de la fibre micro-structurée sur le comportement impulsionnel du laser. Nous avons également étudié le phénomène d’hystérésis dans cette cavité. Nos résultats numériques ont permis de démontrer l’universalité de ce phénomène dans les cavités lasers. Autrement, il est indépendant de la technique de verrouillage de modes. En second lieu, nous avons développé une source laser émettant à 1.6 µm à partir d’un amplificateur fonctionnant dans la bande C. La méthode que nous avons explorée est basée sur la gestion des pertes linéaires. L’émission, en continu et en verrouillage de modes, a été démontrée dans deux configurations différentes. Enfin et en se basant sur ce concept, nous avons rapporté des sources accordables sur une large fenêtre spectrale. Nous avons également étudié différentes formes des régimes harmoniques autour de 1.6 µm. / During our research, we are interested in studying of the figure of eight fiber laser based on the microstructured optical fiber and developing a 1.61 µm mode locked fiber laser from a C-band double-clad Er : Yb doped fiber amplifier. In the first step and based on a theoretical model, we have investigated the multi-pulse emission of a microstructured figure-of eight fiber laser operating in passive mode-locking. The proposed laser is mode locked by the nonlinear amplifying loop mirror (NALM). We further study the hysteresis dependence and the number of pulses in steady state as a function of both the small signal gain and the nonlinear coefficient of microstructured fiber. Our results demonstrate that the nonlinear coefficient of microstructured fiber plays a key role in the formation of multi-soliton. In the second step and based on the control of the linear losses of the cavity, we demonstrate the possibility to achieve filter less laser emission above 1.6 μm, from a C-band double-clad Er: Yb doped fiber amplifier, using a figure-of-eight geometry and a unidirectional ring cavity. We also reported a widely tunable mode locked fiber laser and harmonic mode locking of twin and third pulse around 1.61 µm.

Rational harmonic mode-locking (RHML) fiber lasers generating picoseconds pulsewidth at high-repetition-rate have emerged as a key component for the high-bit-rate optical time-division multiplexing (OTDM) communication system. In this research, we have discovered higher order RHML semiconductor optical amplifier fiber laser (SOAFL) has the degradation on mode-locking capacity, and an output pulse-train with un-equalized peak amplitudes. Therefore, the main focus of the dissertation is focused on the pulse quality analysis and improvement of RHML-SOAFL via optical pulse injection. First, we observed the degradation on mode-locked mechanism of the dark-optical-comb injection mode-locked semiconductor optical amplifier fiber laser (SOAFL) at RHML order increases to >8. Such a less pronounced RHML mechanism at higher orders is mainly attributed to the weak mode-locking strength at high RHML orders as compared to continuous-wave (CW) lasing mechanism, which has been quantified by reduction of spectral linewidth and pulse-shortening force, and the ratio of DC/pulse amplitude enhancement for discriminating 1st to 20th-order RHML capability. To overcome the un-equalized RHML peak intensity, optical injection induced gain modulation of a SOA are demonstrated to equalize the peak intensity of 5-GHz and 40-GHz RHML-SOAFL by using 1-GHz inverse-optical-pulse and a reshaped 10-GHz gain-switching FPLD pulse injection, respectively. The optical injection mode-locking models are constructed to simulate the compensation of uneven amplitudes between adjacent RHML pulse peaks before and after pulse-amplitude equalization. The optimized RHML pulse exhibits a signal-to-noise suppression ratio of 45-dB, and the clock amplitude jitter below the threshold limitation of 10%. On the other hand, to avoid the mode-locked degradation on RHML, a 2nd-order fractional Talbot effect induced frequency-doubling of 10-GHz optical pulse-train is demonstrated to backward inject a SOAFL for 40-GHz RHML. In comparison with the SOAFL pulse-train repeated at 40-GHz generated by the 4th-order purely RHML process, the optimized 2nd-order fractional Talbot effect in combination with the 2nd-order RHML mechanism significantly enhances the modulation-depth of RHML, thus improving the on/off extinction ratio of the 40-GHz SOAFL pulse-train. Such a new scheme also provides a more stable 40-GHz RHML pulse-train from the SOAFL with its timing jitter reduce. Finally, we established a SHG-FROG to distinguish linear and nonlinear chirp of 10-GHz soliton HML-SOAFL, and further extracted intra-cavity linear dispersion via simulation of Schrodinger equation. After the procedure, the linear chirp almost dominates chirp characteristics for optical pulse injection HML-SOAFL system.

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