2018
DOI: 10.1364/boe.9.006116
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Broadband hyperspectral stimulated Raman scattering microscopy with a parabolic fiber amplifier source

Abstract: Hyperspectral stimulated Raman scattering (hsSRS) microscopy has recently emerged as a powerful non-destructive technique for the label-free chemical imaging of biological samples. In most hsSRS imaging experiments, the SRS spectral range is limited by the total bandwidth of the excitation laser to ~300 cm −1 and a spectral resolution of ~25 cm −1 . Here we present a novel approach for broadband hsSRS microscopy based on parabolic fiber amplification to provide linearly chirped broadened Stokes pulses. This no… Show more

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Cited by 50 publications
(40 citation statements)
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“…Currently, the spectral coverage of 200 cm −1 is due to the spectral bandwidth of the laser sources. However, since the delay range is freely tunable, if combined with broadband lasers by fiber amplification 54 or supercontinuum laser sources, the scheme can potentially be used to obtain the entire fingerprint SRS spectrum within 20 µs. In addition, the high-speed delay scanning scheme can be applied to a broad range of modalities requiring a long delay scan, such as transient absorption spectroscopy and impulsive SRS imaging.…”
Section: Discussionmentioning
confidence: 99%
“…Currently, the spectral coverage of 200 cm −1 is due to the spectral bandwidth of the laser sources. However, since the delay range is freely tunable, if combined with broadband lasers by fiber amplification 54 or supercontinuum laser sources, the scheme can potentially be used to obtain the entire fingerprint SRS spectrum within 20 µs. In addition, the high-speed delay scanning scheme can be applied to a broad range of modalities requiring a long delay scan, such as transient absorption spectroscopy and impulsive SRS imaging.…”
Section: Discussionmentioning
confidence: 99%
“…Broadband rea-time ratiometric SRS imaging: A femtosecond dual-beam laser system (Insight DS + from Spectra-Physics) was used for hyperspectral SRS imaging based on an orthogonal modulation spectral focusing scheme as described in our earlier publication. 39 Briefly, we used a parabolic fiber amplifier to increase the Stokes laser bandwidth from 6 nm to ~40 nm, 40 increasing the bandwidth from the original laser system of ~200 cm to ~500 cm -1 , which allows us to acquire both C-H region at 2935 cm -1 and the lower shoulder of the Raman spectral signature of water around 3190 cm -1 . We then employed an orthogonal modulation technique on our Stokes laser for simultaneous dual-band imaging, which was previously used for real-time microscale thermal imaging with SRS.…”
Section: Methodsmentioning
confidence: 99%
“…The Stokes pulse was modulated at 20 MHz using an electro-optic modulator (EOM) and split into two separate arms, one of which was then delayed by 12.5 ns (1/80 MHz) relative to the other. The two arms were recombined using a 50:50 beamsplitter and stretched to 2 ps using a grating-based pulse stretcher 30,31 . The tunable source was centered at 798 nm, and the pulses were dispersed using 60 cm of glass rods.…”
Section: Methodsmentioning
confidence: 99%
“…The tunable source was centered at 798 nm, and the pulses were dispersed using 60 cm of glass rods. The average spectral width is estimated to be 300 cm −1 31 . The pump and Stokes beams were then combined with a dichroic mirror and overlapped temporally using a delay line in the tunable arm.…”
Section: Methodsmentioning
confidence: 99%