研究目的
To investigate the spectral stability and noise levels in fiber-based DUV sources by generating an SC spectrum that extends from 180 nm to 4 μm and characterizing the long-term stability and the pulse-to-pulse relative intensity noise (RIN) of the DW at 275 nm.
研究成果
The study demonstrates the importance of pump laser stabilization for DUV SC sources based on gas-filled HC-ARFs, as the noise performance is significantly influenced by the pump laser's RIN. The findings provide a crucial understanding of the noise mechanisms in such sources and suggest the need for further optimization to achieve lower noise levels.
研究不足
The study highlights the high RIN of the DW pulses at 275 nm, attributed to the high RIN of the mid-IR pump laser, which was not previously considered in numerical modeling. This indicates a limitation in the noise performance of such DUV SC sources.
1:Experimental Design and Method Selection:
The study involved generating an SC spectrum by pumping an argon-filled hollow-core anti-resonant fiber at a mid-IR wavelength of 2.45 μm. The methodology included numerical simulations to investigate the spectral distribution of the RIN.
2:45 μm. The methodology included numerical simulations to investigate the spectral distribution of the RIN.
Sample Selection and Data Sources:
2. Sample Selection and Data Sources: The experiments used a single-ring HC-ARF with a 44 μm core diameter and 7 non-touching capillaries filled with argon at 27 bar.
3:List of Experimental Equipment and Materials:
The setup included a Ti:Sapphire laser pumping an OPA, long pass filter, silver coated mirror, neutral density filters, linear polarizer, CaFl2 Plano-convex lenses, gas cells, power meter, bandpass filter, and photodiode.
4:Experimental Procedures and Operational Workflow:
The output power was monitored for 110 hours, and the RIN was measured by filtering the SC with a 10 nm FWHM bandpass filter and sending it to a fast Si detector.
5:Data Analysis Methods:
The RIN was calculated from the standard deviation of the amplitude of the peaks divided by the mean of the amplitude of the peaks from 10,000 recorded pulses.
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