Erbium-doped photonic crystal fiber chaotic laser

An erbium-doped photonic crystal fiber laser has been designed, constructed and characterized in order to examine the feasibility of this kind of devices for secure communications applications based on two identical chaotic lasers. Inclusion of a tailored photonic crystal fiber as active medium improves considerably the security of the device because it allows customization of the mode transversal profile, very influential on the laser dynamics and virtually impossible to be cloned by undesired listeners. The laser design has been facilitated by the combination of characterization procedures and models developed by us, which allow prediction of the most suitable laser features (losses, length of active fiber, etc.) to a given purpose (in our case, a laser that emits chaotically for a wide assortment of pump modulation conditions). The chaotic signals obtained have been characterized by means of topological analysis techniques. The underlying chaotic attractors found present topological structures belonging to classes of which very scarce experimental results have been reported. This fact is interesting from the point of view of the study of nonlinear systems and, besides, it is promising for secure communications: the stranger the signals, the more difficult for an eavesdropper to synthesize another system with similar dynamics.

[1]  S. Selleri,et al.  Amplification Properties of Erbium Doped Photonic Crystal Fibers , 2002, 2002 28TH European Conference on Optical Communication.

[2]  Adonis Bogris,et al.  Chaos-based communications at high bit rates using commercial fibre-optic links , 2006, SPIE/OSA/IEEE Asia Communications and Photonics.

[3]  Javier Used,et al.  Multiple topological structures of chaotic attractors ruling the emission of a driven laser. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[4]  Fan Zhang,et al.  Photonic crystal fiber for fundamental mode operation of multicore fiber lasers and amplifiers , 2008 .

[5]  Louis M. Pecora,et al.  Synchronization in Chaotic Systems, Concepts and Applications , 2006 .

[6]  Robert Gilmore,et al.  The Topology of Chaos , 2003 .

[7]  Alan V. Oppenheim,et al.  Circuit implementation of synchronized chaos with applications to communications. , 1993, Physical review letters.

[8]  Experimental observation of a chaotic attractor with a reverse horseshoe topological structure , 1997 .

[9]  Reverse horseshoe and spiral templates in an erbium-doped fiber laser. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[10]  Y. Imai,et al.  Chaos synchronization characteristics in erbium-doped fiber laser systems , 2003 .

[11]  J. M. Álvarez,et al.  Unidirectional ring erbium doped fibre laser modelization for characterization in transient regime , 2006 .

[12]  M. A. Rebolledo,et al.  Erbium-Doped-Silica Photonic Crystal Fiber Characterization Method: Description and Experimental Check , 2010, IEEE Journal of Quantum Electronics.

[13]  Rajarshi Roy,et al.  OPTICAL COMMUNICATION WITH CHAOTIC WAVEFORMS , 1998 .

[14]  J. Martin Erbium transversal distribution influence on the effectiveness of a doped fiber : optimization of its performance , 2001 .

[15]  Gilmore,et al.  Structure in the bifurcation diagram of the Duffing oscillator. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[16]  P. Colet,et al.  Synchronization of chaotic semiconductor lasers: application to encoded communications , 1996, IEEE Photonics Technology Letters.