研究目的
To experimentally demonstrate the DW dark pulse in the 1950-nm region from a thulium-doped fiber (TDF) laser cavity using the nanomaterial-based SA.
研究成果
The experimental demonstration of DW dark pulses in the 1956-nm wavelength region from a thulium-doped fiber laser using the bulk-structured Bi2Te3 SA was successful. The results are the first demonstrated for the generation of DW dark pulses from a thulium-doped fiber laser using nanomaterial-based saturable absorbers.
研究不足
The generation of the DW dark pulse under a normal dispersion regime was not checked due to the lack of normal dispersion fibers in the laboratory. Further investigation is needed on the effect of dispersion on the generation of the DW dark pulse.
1:Experimental Design and Method Selection
The SA was prepared by dropping a small amount of a mixed solution containing Bi2Te3 and distilled water onto the end surface of a FC/PC fiber ferrule. The nonlinear transmission of the prepared SA was measured using a lab-made, ~1.5 ps fiber laser with a repetition rate of 24 MHz at 1.93 μm.
2:Sample Selection and Data Sources
Commercially available bulk-structured Bi2Te3 powder was used to fabricate the SA. The Bi2Te3 powder was characterized through scanning electron microscopy (SEM) and energy dispersive spectroscopy (EDS).
3:List of Experimental Equipment and Materials
Bi2Te3 powder (Sigma Aldrich, Bi2Te3 metal basis),SEM (S-4700, Hitachi, Tokyo, Japan),EDS (7200-H, Horiba, Kyoto, Japan),Index matching gel (G608N, Thorlabs, Newton, NJ, USA),Optical spectrum analyzer (AQ6375, Yokogawa, Tokyo, Japan),Oscilloscope (6050A, Lecroy, Chestnut Ridge, NY, USA),Photodetector (ET-5010F, EOT, Traverse City, MI, USA),Electrical spectrum analyzer (USB-SA124B, Signalhound, Battle Ground, WA, USA),Autocorrelator (FR-103MN, Femtochrome Research, Berkeley, CA, USA)
4:Experimental Procedures and Operational Workflow
The Bi2Te3 powder was mixed with distilled water and dropped onto the facet of the ferrule, left to dry for 24 hours. The SA was inserted within a TDF ring cavity. The laser output was measured by various instruments to analyze the generated dark pulses.
5:Data Analysis Methods
The nonlinear transmission was fitted using a specific curve to determine modulation depth and saturation intensity. The laser output was analyzed for pulse width, repetition rate, and signal-to-noise ratio.
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SEM
S-4700
Hitachi
Characterization of Bi2Te3 powder.
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Index matching gel
G608N
Thorlabs
Reduces scattering loss and ensures firm fixation of the Bi2Te3 particles between the fiber ferrules.
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Optical spectrum analyzer
AQ6375
Yokogawa
Measurement of the laser output.
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Oscilloscope
6050A
Lecroy
Measurement of the laser output.
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Autocorrelator
FR-103MN
Femtochrome Research
Measurement of the laser output.
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Bi2Te3 powder
Bi2Te3 metal basis
Sigma Aldrich
Used as a saturable absorber in the fiber laser.
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EDS
7200-H
Horiba
Characterization of Bi2Te3 powder.
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Photodetector
ET-5010F
EOT
Measurement of the laser output.
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Electrical spectrum analyzer
USB-SA124B
Signalhound
Measurement of the laser output.
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