研究目的
Investigating the use of quantum dots CdSe embedded in polymer film as a saturable absorber for passively Q-switched erbium-doped fiber lasers.
研究成果
The study successfully demonstrated a passively Q-switched EDFL operating at 1559.35 nm using a CdSe-PMMA based SA. The Q-switching operation was achieved with a pulse repetition rate from 33.2 to 68.45 kHz and pulse width from 10.04 to 4.30 μs, with a maximum pulse energy of 11.83 nJ. The results confirmed that CdSe-PMMA has good optical properties for SA applications in cost-effective Q-switched EDF lasers.
研究不足
The Q-switched pulses became unstable or disappeared at pump powers above 118 mW, attributed to over-saturation of the CdSe SA. The pulse width could be further reduced by shortening the laser cavity lifetime or improving the modulation depth of the CdSe PMMA based SA.
1:Experimental Design and Method Selection:
The study employed a passively Q-switched erbium-doped fiber laser (EDFL) setup using quantum dots (QD) CdSe as a saturable absorber (SA). The CdSe powder was synthesized and embedded into a poly(methyl methacrylate) (PMMA) film via emulsion polymerization process.
2:Sample Selection and Data Sources:
The CdSe powder was characterized using transmission electron microscopy (TEM), energy dispersive X-ray spectroscopy (EDS), and X-ray diffraction (XRD) to verify its nanoparticle size, composition, and crystal structure.
3:List of Experimental Equipment and Materials:
The experimental setup included a
4:4 m long Erbium-doped fiber (EDF) as the gain medium, pumped by a 980 nm laser diode via a 980/1550 nm wavelength division multiplexer (WDM). The CdSe PMMA SA device was inserted into the ring laser cavity. Experimental Procedures and Operational Workflow:
The Q-switched operation was achieved by varying the pump power within 30–118 mW. The output spectrum and pulse characteristics were measured using an optical spectrum analyzer (OSA) and a 500 MHz oscilloscope (OSC), respectively.
5:Data Analysis Methods:
The pulse repetition rate and pulse width were analyzed as functions of the incident pump power, and the average output power and pulse energy were calculated.
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