Nanotube and graphene saturable absorbers for fibre lasers

By Amos Martinez, Zhipei Sun. Nature Photonics, 2013

730 citations recorded by the source corpus.

Subfields: Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering

View Paper: https://www.semanticscholar.org/paper/2079491ace747231bcd259b43440be42532396eb

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Atomic and Molecular Physics, and Optics

1. Edmund J. R. Kelleher
2. R. I. Woodward
3. Tawfique Hasan
4. F. Torrisi
5. Zhipei Sun
6. Meng Zhang
7. R. Howe
8. G. Hu

In Electrical and Electronic Engineering

1. Edmund J. R. Kelleher
2. R. I. Woodward
3. F. Torrisi
4. Tawfique Hasan
5. Meng Zhang
6. G. Hu
7. R. Howe
8. Han Zhang

Citations in the corpus

• Solution processed MoS2-PVA composite for sub-bandgap mode-locking of a wideband tunable ultrafast Er:fiber laser (2015, background): “This combination of properties makes MoS2 a suitable saturable absorber (SA) for ultrafast mode-locked pulsed lasers, with the potential for pulse generation at visible wavelengths, something that is yet to be demonstrated using graphene and its derivative materials [27].”
• Broadband Graphene Saturable Absorber for Pulsed Fiber Lasers at 1, 1.5, and 2 μm (2014, background): “7% [35], which is much larger than what is typically reported for single layer graphene devices [6], [36], [37] (e.”
• Few-layer antimonene decorated microfiber: ultra-short pulse generation and all-optical thresholding with enhanced long term stability (2017, background): “3% per layer for graphene [13]) and difficult to create a band-gap.”
• Topological-Insulator Passively Q-Switched Double-Clad Fiber Laser at 2 $\mu$m Wavelength (2014, background): “could be difficult for activating ultrafast lasers; 2) the wavelength dependence of its saturation fluence [24] could be blocking the”
• 2D Saturable Absorbers for Fibre Lasers (2015, methodology): “For SAs in fibre lasers, this transition from SA to RSA can influence the intra-cavity pulse dynamics and affect the transition between Q-switching and mode-locking regimes [61].”
• 1-, 1.5-, and 2-μm Fiber Lasers Q-Switched by a Broadband Few-Layer MoS2 Saturable Absorber (2014, neutral): “as Q-switcher or mode-locker, the large number of CNTs is not in resonance, leading to the high non-saturable loss in laser cavity [40].”