• Chinese Optics Letters
  • Vol. 13, Issue 12, 121401 (2015)
Dongjia Han1, Yanyan Li1, Juan Du1、*, Kun Wang2, Yongfang Li2, Tomohiro Miyatake3, Hitoshi Tamiaki4, Takayoshi Kobayashi5、**, and Yuxin Leng1、6、***
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Laboratory of Advanced Optoelectronic Materials, College of Chemistry, Chemical Engineering and Materials Science, Soochow University, Suzhou 215123, China
  • 3Department of Materials Chemistry, Ryukoku University, Otsu, Shiga 520-2194, Japan
  • 4Department of Bioscience and Biotechnology, Ritsumeikan University, Kusatsu, Shiga 525-8577, Japan
  • 5Advanced Ultrafast Laser Research Center, University of Electro-Communications, 1-5-1, Chofugaoka, Chofu, Tokyo 182-8585, Japan
  • 6FSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
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    DOI: 10.3788/COL201513.121401 Cite this Article Set citation alerts
    Dongjia Han, Yanyan Li, Juan Du, Kun Wang, Yongfang Li, Tomohiro Miyatake, Hitoshi Tamiaki, Takayoshi Kobayashi, Yuxin Leng. Ultrafast laser system based on noncollinear optical parametric amplification for laser spectroscopy[J]. Chinese Optics Letters, 2015, 13(12): 121401 Copy Citation Text show less
    Schematic of the two-color pump–probe setup. Pulses with 50 fs duration at a 5 kHz repetition rate are used to drive the NOPA and white light generation. BS: beam splitter; SHG: second-harmonic generation; VA: variable attenuator; WLG: white-light generation; MLA: multi-channel lock-in amplifier.
    Fig. 1. Schematic of the two-color pump–probe setup. Pulses with 50 fs duration at a 5 kHz repetition rate are used to drive the NOPA and white light generation. BS: beam splitter; SHG: second-harmonic generation; VA: variable attenuator; WLG: white-light generation; MLA: multi-channel lock-in amplifier.
    (a) Spectra of the different visible compressed wavelength pulses. The green line represents the spectra obtained by pumping the zinc chloride aggregate, and the red line represents the spectra for the PTB7-Th polymer in the subsequent experiments. The insert is the shortest compressed pulse duration according to the pink line (the black line is the duration measured, while the red line and blue fit are the Lorentzian fit and Gaussian fit, respectively). (b) Spectra of NIR. Insert is the stationary absorption spectrum of the PTB7-Th polymer (red line).
    Fig. 2. (a) Spectra of the different visible compressed wavelength pulses. The green line represents the spectra obtained by pumping the zinc chloride aggregate, and the red line represents the spectra for the PTB7-Th polymer in the subsequent experiments. The insert is the shortest compressed pulse duration according to the pink line (the black line is the duration measured, while the red line and blue fit are the Lorentzian fit and Gaussian fit, respectively). (b) Spectra of NIR. Insert is the stationary absorption spectrum of the PTB7-Th polymer (red line).
    (a) Two-dimensional pattern of the, different absorbances (ΔA), which are dependent on the time delay from −200 to 2800 fs in the whole probe spectral region (670–760 nm); (right) time trace of different absorbance rates. (b) Two-dimensional pattern of the different absorbances (ΔA) dependent on the time delay from −0.4 to 100 ps in the whole probe spectral region (960–1040 nm); (right) time trace of different absorbances.
    Fig. 3. (a) Two-dimensional pattern of the, different absorbances (ΔA), which are dependent on the time delay from 200 to 2800 fs in the whole probe spectral region (670–760 nm); (right) time trace of different absorbance rates. (b) Two-dimensional pattern of the different absorbances (ΔA) dependent on the time delay from 0.4 to 100 ps in the whole probe spectral region (960–1040 nm); (right) time trace of different absorbances.
    Dongjia Han, Yanyan Li, Juan Du, Kun Wang, Yongfang Li, Tomohiro Miyatake, Hitoshi Tamiaki, Takayoshi Kobayashi, Yuxin Leng. Ultrafast laser system based on noncollinear optical parametric amplification for laser spectroscopy[J]. Chinese Optics Letters, 2015, 13(12): 121401
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