研究目的
Investigating the plasma density created at the temporal focus of a self-compressing higher-order pump soliton in a gas-filled hollow-core photonic crystal fiber using a counterpropagating probe soliton.
研究成果
The pump-probe technique effectively measures the plasma density in gas-filled hollow-core photonic crystal fibers, showing good agreement with numerical simulations. It provides a robust method for probing photoionization in various gases and gas mixtures, with potential applications in monitoring dispersion changes in other systems.
研究不足
The technique is limited by the travel range of the translation stage, affecting the maximum delay achievable. The accuracy of plasma density measurements may be influenced by slight reductions in probe energy during propagation and short-timescale plasma density changes not accounted for in modeling.
1:Experimental Design and Method Selection:
The study employs a pump-probe technique to monitor ultrafast polarizability changes, specifically measuring plasma density in a gas-filled hollow-core photonic crystal fiber. The method involves using a counterpropagating probe soliton to emit dispersive-wave radiation, whose wavelength shift indicates plasma density changes.
2:Sample Selection and Data Sources:
Experiments are conducted on argon- and krypton-filled hollow-core photonic crystal fibers. The fibers have a core diameter of 34 μm and are kept in a pressurized gas cell.
3:List of Experimental Equipment and Materials:
Ti:sapphire laser amplifier, fused-silica beam splitter, half-wave plate, thin-film polarizer, calcium fluoride planoconvex lenses, kagomé hollow-core photonic crystal fiber, magnesium fluoride windows, spectrometer, retroreflector mounted on a linear translation stage.
4:Experimental Procedures and Operational Workflow:
Pulses from a Ti:sapphire laser are divided and delivered to two arms, controlling pulse energies with a half-wave plate and thin-film polarizer. The pulses are launched into opposite ends of the fiber, and the probe light is reflected into a spectrometer. The relative delay between pump and probe is varied to map the plasma density distribution.
5:Data Analysis Methods:
The spectral centroid of the dispersive wave is calculated over a wavelength range of 50 nm. Numerical simulations are performed to compare with experimental results, using the unidirectional full-field nonlinear wave equation and finite element modeling.
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Ti:sapphire laser amplifier
Generates femtosecond laser pulses for the pump and probe arms of the experiment.
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fused-silica beam splitter
Divides the laser pulses into pump and probe arms.
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half-wave plate
Controls the pulse energies in conjunction with a thin-film polarizer.
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thin-film polarizer
Controls the pulse energies in conjunction with a half-wave plate.
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calcium fluoride planoconvex lenses
Launches the pulses into the hollow-core photonic crystal fiber.
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kagomé hollow-core photonic crystal fiber
Guides the laser pulses and contains the gas for ionization studies.
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magnesium fluoride windows
Allows in- and out-coupling of light in the pressurized gas cell.
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spectrometer
Measures the wavelength of the dispersive wave emission from the probe soliton.
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retroreflector mounted on a linear translation stage
Varies the relative delay between pump and probe pulses.
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