• Journal of the European Optical Society-Rapid Publications
  • Vol. 19, Issue 1, 2023008 (2023)
Pieter H. Neethling1,*, Ruan Viljoen1, Alexander M. Heidt2, Dirk Spangenberg1,2..., Thomas Feurer2 and Erich G. Rohwer1|Show fewer author(s)
Author Affiliations
  • 1Laser Research Institute, Stellenbosch University, 7600 Stellenbosch, South Africa
  • 2Institute for Applied Physics, University of Bern, 3012 Bern, Switzerland
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    DOI: 10.1051/jeos/2023008 Cite this Article
    Pieter H. Neethling, Ruan Viljoen, Alexander M. Heidt, Dirk Spangenberg, Thomas Feurer, Erich G. Rohwer. Novel time-resolved CARS implementation for application in microscopy[J]. Journal of the European Optical Society-Rapid Publications, 2023, 19(1): 2023008 Copy Citation Text show less
    (A) Spectrogram of the CS2/benzene mixture with three regions of interest (R1, R2, and R3) highlighted. R1 shows the resonant response from the CS2 656 cm−1 peak, while R2 shows the resonant response of the 991 cm−1 benzene peak. R3 highlights the instrument response function, used to measure the temporal profile of the probe pulse. (B) The instrument response as measured from a lineout in region R3, with a Gaussian fit to the central maximum, with full-width-at-half-maximum (FWHM) of 265 fs.
    Fig. 1. (A) Spectrogram of the CS2/benzene mixture with three regions of interest (R1, R2, and R3) highlighted. R1 shows the resonant response from the CS2 656 cm−1 peak, while R2 shows the resonant response of the 991 cm−1 benzene peak. R3 highlights the instrument response function, used to measure the temporal profile of the probe pulse. (B) The instrument response as measured from a lineout in region R3, with a Gaussian fit to the central maximum, with full-width-at-half-maximum (FWHM) of 265 fs.
    (A) A lineout from the spectrogram in Figure 1A taken at the 656 cm−1 CS2 peak. (B) A lineout from the spectrogram in Figure 1A taken at the 991 cm−1 benzene peak. In both figures the data was fitted with an exponential decay function (pink line) from 400 fs onwards.
    Fig. 2. (A) A lineout from the spectrogram in Figure 1A taken at the 656 cm−1 CS2 peak. (B) A lineout from the spectrogram in Figure 1A taken at the 991 cm−1 benzene peak. In both figures the data was fitted with an exponential decay function (pink line) from 400 fs onwards.
    (A) The spectrogram of the CS2/benzene mixture obtained by targeting different wavenumbers using quadratic phase spectral focussing and a probe delayed by 800 fs with respect to the pump. (B) The lineouts at 656 cm−1 and 991 cm−1 target wavenumbers, indicating the suppression of the non-resonant background.
    Fig. 3. (A) The spectrogram of the CS2/benzene mixture obtained by targeting different wavenumbers using quadratic phase spectral focussing and a probe delayed by 800 fs with respect to the pump. (B) The lineouts at 656 cm−1 and 991 cm−1 target wavenumbers, indicating the suppression of the non-resonant background.
    Pieter H. Neethling, Ruan Viljoen, Alexander M. Heidt, Dirk Spangenberg, Thomas Feurer, Erich G. Rohwer. Novel time-resolved CARS implementation for application in microscopy[J]. Journal of the European Optical Society-Rapid Publications, 2023, 19(1): 2023008
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