Abstract

Abstract Tapered fiber (TF) and D-shaped fiber (DF) are two types of widely investigated devices in facilitating evanescent-field interactions with external materials. Although they have been found to be particularly useful in various ultrafast regimes, to date there is still no clear or systematic investigation on their local nonlinearities as well as the exerted influences on ultrafast behaviors. Herein, we present such thorough investigation through local nonlinearity engineering on TF and then in contrast with a DF as a reference. Optically deposited black phosphorus quantum dots (BPQDs) are used for saturable absorption. The nanometer-scale extremely small sizes of the BPQDs helpfully eliminate size-induced uncertainties or distortions during both device fabrication and the latter light–matter interaction. For the TF, in the experiment, it is found that the local nonlinear effect starts to be rather appreciable as the TF shrinks to a moderate thickness. Remarkably in comparison, the local nonlinearity of the DF itself can even be neglected reasonably, but after coating with BPQDs, it possesses a much larger modulation depth than any of the used BPQDs-coated TFs with different thicknesses/lengths. Further, we theoretically analyze the related locally nonlinear effects and reveal, for the first time, the direct origin of saturable absorption with evanescent-field-based general structures.

Highlights

  • Since the successful application of carbon nanotubes (CNTs) and graphene as saturable absorbing materials in various ultrafast laser systems, especially fiber lasers [1,2,3,4,5,6,7,8,9], a wide variety of micro/nanomaterials have been explored and fabricated as saturable absorbers (SAs)

  • Dissipating them into a polymer film patch [1,2,3,4,5,6,7,8,9,10] and directly depositing them onto a reflective mirror/transmissive window [11,12, 26,27] are the earliest and most commonly adopted approaches, mainly due to the simplicity in fabrication and the ease to transfer. One limitation with these approaches is that they can only be used with low optical powers. This is because that such a type of thin film has a very low laser-induced damage threshold (LIDT) when exposed directly to the intensive light tightly confined within a fiber core, typically less than 100 μm2 in the mode-field area (MFA)

  • We have investigated in detail the local nonlinearities of both Tapered fiber (TF) and D-shaped fiber (DF) embedding in black phosphorus quantum dots (BPQDs)

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Summary

Introduction

Since the successful application of carbon nanotubes (CNTs) and graphene as saturable absorbing materials in various ultrafast laser systems, especially fiber lasers [1,2,3,4,5,6,7,8,9], a wide variety of micro/nanomaterials have been explored and fabricated as saturable absorbers (SAs) Those include nanoscale metal particles [10, 11], topological insulators [12,13,14], MXene [15, 16], transition metal dichalcogenides [17,18,19], black phosphorus [20,21,22,23,24,25], etc. The single-layer absorbance of BP can reach ∼2.8, which is greater than that of graphene ∼2.3% [55]

Fabrication of BPQDs
BPQDs-coated TFs for mode-locked fiber lasers
BPQDs-coated DF for mode-locked fiber laser
Discussion on the TF and DF related nonlinearities and modulation depths
Conclusions
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