Why do output pulses split in actively Q-switched fiber lasers?

Pulse evolutions of a typical actively Q-switched fiber laser are numerically investigated by using the traveling wave method. Unlike those conventional actively Q-switched solid-state lasers, the output pulses in a few actively Q-switched fiber lasers often tend to break into multiple peaks in Q-switched envelopes. In this paper, the multipeak phenomena of output pulses are analyzed, and the mechanism for these phenomena is detailed. It is shown that the first transient pulse in the cavity is initiated by a quick switching of the Q-switching element, which actually injects part of amplified spontaneous emission (ASE) into the cavity in the form of a pulse; and then the formation of multipeak structures is related to the complicated evolution of the switching-induced perturbation, and is determined by the rise time of switching and conditions of photon density and population inversion during the Q switching. It is also shown that under certain conditions of cavity, pump and switching, a split-pulse output can turn to a single-pulse output. The new understanding of laser dynamics and the precise explanation for the pulse splitting in actively Q-switched fiber lasers are given in this paper.

[1]  J. Chrostowski,et al.  High-power Q-switched erbium-doped fiber laser , 1991 .

[2]  Kazimierz Jędrzejewski,et al.  Q-switched neodymium-doped phosphate glass fiber lasers , 1993 .

[3]  David J. Richardson,et al.  Characteristics of Q-switched cladding-pumped ytterbium-doped fiber lasers with different high-energy fiber designs , 2001 .

[4]  J Chrostowski,et al.  Self-mode locking in a Q-switched erbium-doped fiber laser. , 1993, Applied optics.

[5]  Yong Wang,et al.  Pulse evolution of a Q-switched ytterbium-doped double-clad fiber laser , 2003 .

[6]  Yong Wang,et al.  Analysis of a Q-switched ytterbium-doped double-clad fiber laser with simultaneous mode locking , 2003 .

[7]  D. Pagnoux,et al.  Analysis and Optimization of a Q-Switched Erbium Doped Fiber Laser Working with a Short Rise Time Modulator , 1996 .

[8]  Yahei Koyamada,et al.  Analysis and design of Q-switched erbium-doped fiber lasers and their application to OTDR , 2002 .

[9]  Michel J. F. Digonnet,et al.  Rare earth doped fiber lasers and amplifiers , 1993 .

[10]  A. A. Demidov,et al.  Efficient operation of double-clad Yb3+-doped fiber lasers with a novel circular cladding geometry. , 2003, Optics letters.

[11]  Yong Wang,et al.  Experimental study of stimulated Brillouin and Raman scatterings in a Q-switched cladding-pumped fiber laser , 2004 .

[12]  U. Keller,et al.  Self-starting and self-Q-switching dynamics of passively mode-locked Nd:YLF and Nd:YAG lasers. , 1993, Optics letters.

[13]  J. Nilsson,et al.  Compact high-energy Q-switched cladding-pumped fiber laser with a tuning range over 40 nm , 1999, IEEE Photonics Technology Letters.

[14]  J. J. Degnan,et al.  Theory of the optimally coupled Q-switched laser , 1989 .

[15]  Yuan Shi,et al.  High Repetition Rate Q-Switched Ring Laser in Er3+-Doped Fiber , 1995 .

[16]  C. C. Cutler,et al.  Why does linear phase shift cause mode locking , 1992 .

[17]  William G. Wagner,et al.  Evolution of the Giant Pulse in a Laser , 1963 .

[18]  Yung-Fu Chen,et al.  Analysis of passively Q-switched lasers with simultaneous mode locking , 2002 .

[19]  Trevor P. Newson,et al.  Diode pumped high power simultaneously Q-switched and self mode-locked erbium doped fibre laser , 1996 .

[20]  J. W. Thomas Numerical Partial Differential Equations: Finite Difference Methods , 1995 .