Summary

Rejection of Fluorescence Background in Resonance and Spontaneous Raman Microspectroscopy

Published: May 18, 2011
doi:

Summary

We discuss the construction and operation of a complex nonlinear optical system that uses ultrafast all-optical switching to isolate Raman from fluorescence signals. Using this system we are able to successfully separate Raman and fluorescence signals utilizing pulse energies and average powers that remain biologically safe.

Abstract

Raman spectroscopy is often plagued by a strong fluorescent background, particularly for biological samples. If a sample is excited with a train of ultrafast pulses, a system that can temporally separate spectrally overlapping signals on a picosecond timescale can isolate promptly arriving Raman scattered light from late-arriving fluorescence light. Here we discuss the construction and operation of a complex nonlinear optical system that uses all-optical switching in the form of a low-power optical Kerr gate to isolate Raman and fluorescence signals. A single 808 nm laser with 2.4 W of average power and 80 MHz repetition rate is split, with approximately 200 mW of 808 nm light being converted to < 5 mW of 404 nm light sent to the sample to excite Raman scattering. The remaining unconverted 808 nm light is then sent to a nonlinear medium where it acts as the pump for the all-optical shutter. The shutter opens and closes in 800 fs with a peak efficiency of approximately 5%. Using this system we are able to successfully separate Raman and fluorescence signals at an 80 MHz repetition rate using pulse energies and average powers that remain biologically safe. Because the system has no spare capacity in terms of optical power, we detail several design and alignment considerations that aid in maximizing the throughput of the system. We also discuss our protocol for obtaining the spatial and temporal overlap of the signal and pump beams within the Kerr medium, as well as a detailed protocol for spectral acquisition. Finally, we report a few representative results of Raman spectra obtained in the presence of strong fluorescence using our time-gating system.

Protocol

1. Some care must be taken in preparing and placing a Raman sample within this system. Because the system typically makes use of very high numerical aperture objectives with very short working distances, the samples are placed on a coverslip. Biological samples are typically placed on a No. 1 thickness coverslip mounted in an Attofluor cell chamber (Invitrogen, Carlsbad, CA). Liquid samples, particularly those toxic to humans, are placed in a small glass bottle with a coverslip cem…

Discussion

The field of biomedical Raman spectroscopy has seen increasing interest over the past several years as a result of its demonstrated potential for solving several difficult challenges in biological diagnostics. For example, Raman spectra have been shown to have diagnostic value in cancer detection 3, 4, 5, 6. Raman spectroscopy has also been used in bacterial quantitation 7, 8 and bacterial drug response 9. It has also found application in a broad range of other biomedical applications ran…

Divulgazioni

The authors have nothing to disclose.

Acknowledgements

This work was funded by NSF award DBI 0852891. Part of this work was also funded by the Center for Biophotonics Science and Technology, a designated NSF Science and Technology Center managed by the University of California, Davis, under Cooperative Agreement No. PHY0120999.

Materials

Name Company Catalog Number Comments
Lenses ThorLabs Various All lenses coated to have maximum transmission losses of 1% each
Tunable Ti:Sapph laser Coherent Chameleon 30 nJ, 200 fs, 80 MHz
40X oil immersion objective Olympus UApo/340 NA = 1.35
Inverted microscope Olympus IX-71 Modified to remove all lenses in side port
Half wave plate Thorlabs AHWP05M-600  
Glan-Thompson polarizer Thorlabs GTH10M ˜10% transmission loss
Spectrometer PI Acton SP2300i  
CCD PI Acton Pixis 100B  
Mathmatical software The MathWorks MATLAB version 2008a
Faraday isolator EOT BB8-5I  
Piezo-electric mirror Newport AG-M100  
BBO crystal CASIX custom 1 mm thickness
Bandpass filter 1 Andover 008FC14 808 ± 0.4 nm
Dichroic mirror Semrock FF662-FDI01 band edge at 662 nm
Long-pass filter Semrock BLP01-405R band edge at 417 nm
Bandpass filter 2 Semrock FF02-447/60 417-447 nm
CS2 Sigma-Aldrich 335266 99% purity
Coumarin 30 Sigma-Aldrich 546127 99% purity
Immersion oil Cargille 16242 Type DF

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Citazione di questo articolo
Smith, Z. J., Knorr, F., Pagba, C. V., Wachsmann-Hogiu, S. Rejection of Fluorescence Background in Resonance and Spontaneous Raman Microspectroscopy. J. Vis. Exp. (51), e2592, doi:10.3791/2592 (2011).

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