Chinese Journal of Lasers, Volume. 47, Issue 8, 811002(2020)
Effect of Parallel Plate Constraint on CN Molecular Spectra in Laser-Induced PMMA Plasma
Fig. 1. Schematic of experimental setup for nanosecond laser-induced PMMA plasma spectroscopy
Fig. 2. Time-resolved spectra of CN molecule (Δν=0). (a) Without spatial confinement cavity; (b) with spatial confinement cavity
Fig. 3. Evolution of CN (0-0) spectral peak intensity with delay time and wavelength. (a) Delay time; (b) wavelength
Fig. 4. Evolution of CN(0-0) spectral peak intensity with delay time. (a) Without spatial confinement cavity; (b) with spatial confinement cavity
Fig. 5. Evolution of CN(0-0) spectral peak intensity with laser energy at delay time of 5 μs
Fig. 6. Comparison of CN(Δν=0) spectra. (a) Without spatial confinement cavity; (b) with spatial confinement cavity
Fig. 7. Evolution of vibration temperatureof CN molecule with delay time under different laser energies. (a) 70 mJ; (b) 80 mJ
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Yang Xue, Chen Anmin, Li Suyu, Jiang Yuanfei, Jin Mingxing. Effect of Parallel Plate Constraint on CN Molecular Spectra in Laser-Induced PMMA Plasma[J]. Chinese Journal of Lasers, 2020, 47(8): 811002
Category: spectroscopy
Received: Feb. 20, 2020
Accepted: --
Published Online: Aug. 17, 2020
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