Elsevier

Optical Materials

Volume 100, February 2020, 109635
Optical Materials

Sb4O5Cl2 for 34th-order-harmonic mode locking

https://doi.org/10.1016/j.optmat.2019.109635Get rights and content

Highlights

  • •We have systematically studied the structure characteristic and nonlinear optics property of Sb4O5Cl2.

  • The saturation intensity and modulation depth are 402.5 MW/cm2 and 1.3% measured by experiment.

  • Harmonic mode locking with 850-fs pulse duration, 202.3-MHz maximum repetition rate is generated based on Sb4O5Cl2 SA.

  • We think this work opens novel avenues toward optoelectronics device based on Sb4O5Cl2.

Abstract

Due to the excellent electrochemical characteristics, Sb4O5Cl2 has been potentially used in flame retardant, catalyst, and anode materials, etc. At the same time, it has broad application prospects in optics and optoelectronics because of its strong inoxidizability, high damage threshold and relatively high-photoelectric conversion efficiency. However, the application of Sb4O5Cl2 in ultra-fast photonics has not been reported so far. In this work, the structure characteristic and nonlinear optics property of Sb4O5Cl2 have been systematically studied. The result indicates saturation intensity and modulation depth are 402.5 MW/cm2 and 1.3%, which prove Sb4O5Cl2 could be utilized as a saturable absorber (SA) in ultrafast photonics. Especially, harmonic mode-locking with 850-fs pulse duration, 2.86-nm 3-dB bandwidth, 202.3-MHz maximum repetition rate in optical communication region is generated based on a tapered fiber incorporated with Sb4O5Cl2 for the first time to our knowledge. This work opens novel avenues toward optoelectronics device based on Sb4O5Cl2 in the fields of optical modulation, optical detection and optical communication, etc.

Introduction

Saturable absorbers (SAs) are materials which reduce light absorption with the increase of light intensity [[1], [2], [3], [4], [5], [6], [7], [8]]. In the past few years, SAs such as, graphene, transition metal disulfides (TMDs), carbon nanotubes, bismuthene and black phosphorus have been extensively studied because of their excellent optical properties [[9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22]]. But more stable and cheaper SAs are worth further to be explored. Sb is a nitrogen group element (V main group). Its compounds were used as cosmetics or decorations in ancient times. However, it was not until about the 17th century that Sb was known to be a separate chemical element. In recent years, Sb has attracted great interest as an alloy materials such as lead alloy for battery grids and thermoelectric alloys, or as a stuffing element of III–V semiconducting materials for example, GaSb, InSb and AlSb [[23], [24], [25], [26]]. Antimony oxides such as Sb2O3 are widely used in plastics, fibers, rubber, ceramics, flame retardants, catalysts, batteries, and other chemical industries [27]. However, the research of Sb compounds in the field of ultrafast optics mainly concentrated on Sb2Se3 [28]. Compared to Sb, Bi is also an important element of the V main group. Compounds of Bi, such as Bi2Te3 and Bi2Se3, have been widely studied in ultrafast optics [[29], [30], [31]]. Sb4O5Cl2 is a kind of antimony oxide with stable performance and lower manufacturing cost than other materials. It can be synthesized by electrochemical method with Sb anode, chloride salt and different metal cathodes dissolved in HCl or hydrothermal approach with SbCl3, NaOH, and ethylene glycol [32]. According to reports, three-dimensional bulk Sb4O5Cl2 can be used as flame retardant, lithium storage materials, and photo catalysts. But there are few applications in optics.

In addition, ultrafast pulses, with pulse width in picosecond and femtosecond range, are widely used in communication, medical treatment, mechanical processing, and other fields [33,34]. As a technique to generate ultrashort pulses from lasers, mode-locking can be divided into active mode-locking and passive mode-locking. Compared with active mode-locking, passive mode-locking can generate higher-quality pulses. In recent years, the performances of passively mode-locked lasers, such as repetition frequency, pulse width and peak power, etc, have been continuously improved through changing structures and devices. Among them, the most advanced one is fiber laser. The peak power, pulse width, spectrum, central wavelength of fiber laser can exceed 10 kW [35], narrower than 10 fs [36,37], broadened over 100 nm, extend to different bands [[38], [39], [40]], respectively. Moreover, fiber laser can be converted between different output states in the same cavity, which has been successfully realized in the experiment [41,42]. However, Sb4O5Cl2 for the applications in optics, especially in ultrafast optics, has not been reported yet [[43], [44], [45]].

In this work, nonlinear optical and ultrafast photonics properties of Sb4O5Cl2 are investigated for the first time. The saturable absorption of Sb4O5Cl2 is measured by a double balance detector, the saturation intensity and modulation depth are 402.5 MW/cm2, 1.3% respectively. When Sb4O5Cl2 SA is inserted into an Er-doped fiber laser, a harmonic mode-locked all-fiber laser based on evanescent field interaction with Sb4O5Cl2 is achieved. The pulse duration is 850-fs with central wavelength of 1563.1 nm. When the pump power is above 214 mW, a 34th-order-harmonic mode-locked pulse (corresponding to repetition of 202.3 MHz) has been obtained. Our work provides an effective scheme for the development of Sb4O5Cl2 in nonlinear optics. The obtained results show that Sb4O5Cl2 has outstanding saturable absorption properties and valuable potential applications.

Section snippets

Material characterization

The Sb4O5Cl2 dispersion solution is made by mixing Sb4O5Cl2 powder with acetone solvent. After that, it is shaked in ultrasonic machine at least 24 h. The purity, morphology and crystallinity of Sb4O5Cl2 are characterized by scanning electron microscope (SEM),  transmission electron microscope (TEM), energy dispersive spectrometer (EDS), x-ray diffraction (XRD), and ultraviolet–visible-near-infrared (UV–VIS-NIR) spectroscopy. Fig. 1 (a) is the atomic structure of Sb4O5Cl2 with different angle.

Experiments and results

Fig. 4 (a) shows the schematic diagram of Er-doped mode-locked fiber laser with Sb4O5Cl2 as SA. A laser diode (LD) with a central wavelength of 976 nm is used as an excitation source to provide energy for the ring cavity. A 980/1550 nm wavelength division multiplexer (WDM) is used to couple the 980 nm and 1550 nm light into the cavity. Er-doped fiber (EDF) is used as an gain medium in the cavity. A polarization independent isolator (PI-ISO) is added after the EDF to ensure that light is

Conclusion

The morphology, optical properties of Sb4O5Cl2 are analyzed by SEM, EDS, XRD, UV. In these ways, we find that it is a three-dimensional cubic structure material with good crystallinity. The modulation depth and saturation intensity measured by a home-made instrument are about 1.3% and 402.5 MW/cm2, respectively. In addition, we achieve a harmonic mode-locking by adding Sb4O5Cl2 into the fiber laser and increasing the power appropriately. Its central wavelength, 3-dB bandwidth, pulse width,

Author contributions section

Shu-yuan Lv:Investigation, Revise. Ya-xin Chen:Investigation, Resources, Data Curation, Writing - Original Draft, Writing - Review & Editing, Visualization. Xiao-hui Li:Project administration, Funding acquisition, Investigation, Revise. Wen-feng Luo:Revise. Ya-min Wang:Revise. Wen-xiong Xu: Revise. Abdul Qyyum:Investigation. Han Zhang: Revise.

Declaration of competing interest

We declare that we have no financial and personal relationships with other people or organizations that can inappropriately influence our work, there is no professional or other personal interest of any nature or kind in any product, service and/or company that could be construed as influencing the position presented in, or the review of, the manuscript entitled " Sb4O5Cl2 for 34th-order-harmonic mode locking".

Acknowledgement

This research was supported by the National Natural Science Foundation of China (61605106); Funded projects for the Academic Leader and Academic Backbones, Shaanxi Normal University (18QNGG006); Starting Grants of Shaanxi Normal University (grant number 1112010209, 1110010717); Fundamental Research Funds For the Central Universities (GK201802006, 2018CSLY005); Open Research Fund of State Key Laboratory of Pulsed Power Laser Technology, Electronic Engineering Institute (No. SKL2017KF02); Open

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