Coupling scheme for graphene saturable absorber in a linear cavity mode-locked fiber laser

Abstract

A saturable absorber based on a graphene layer covered single-mode fiber with inner short waveguides is proposed and demonstrated for a linear cavity Er-doped mode-locked fiber laser. A pair of short waveguides is written in the fiber by using femtosecond micromachining technology, and the propagating light is guided by one short waveguide to the cladding-air interface and interacts with the graphene layer in the form of evanescent waves before being collected back to the core by another short waveguide, and, as a result, the saturable absorption is excited. The designed saturable absorber is used in the passively mode-locked fiber laser to generate traditional soliton mode-locked pulse output with the center wavelength of 1564.9 nm and pulse width of 758 fs at the fundamental frequency of 22.58 MHz. The fabricated saturable absorber device is stable in operation, compact in structure, safe for thermal damage, and can effectively overcome the shortcomings of poor robustness of the saturable absorbers based on a tapered fiber and D-shaped fiber. This provides a new optical coupling scheme for saturable absorbers based on 2D materials such as graphene and has great potential application in the field of ultrashort pulse lasers.

Indium antimonide-based saturable absorber to demonstrate passively Q-switched and mode-locked operation

“…However, the real application of NPR and NALM is constrained by limited output power, weak ambient stability and difficulty in self-starting [22]. Currently, semiconductor saturated absorption mirrors (SESAMs) [23][24][25][26], graphene [27][28][29] and single-walled carbon nanotubes (SWCNTs) are the three most common SAs for passively Q-switched and mode-locked laser manipulation [30][31][32][33]. SESAMs have become the primary SAs used in commercial fiber lasers.…”

Dual-Wavelength Mode-Locked Oscillation with Graphene Nanoplatelet Saturable Absorber in Erbium-Doped Fiber Laser

“…This includes materials from the group of transition metal oxides [11][12][13], transition metal dichalcogenides [14,15] and topological insulators [16,17]. Undeniably, the advancement of these materials can be traced back to the superiority and versatility of their pioneer, graphene, which is still worthy of investigation to date [18][19][20][21][22][23][24][25]. This is attributed to its desirable properties such as gapless linear dispersion of Dirac-electrons, short recovery time and ultra-broadband absorption [21].…”