{"id":8211,"date":"2024-10-19T23:17:10","date_gmt":"2024-10-19T21:17:10","guid":{"rendered":"https:\/\/soliton-gmbh.de\/?post_type=glossary&p=8211"},"modified":"2026-11-11T17:43:37","modified_gmt":"2026-11-11T16:43:37","slug":"coherent-anti-stokes-raman-scattering-with-comparison-to-raman-spectroscopy","status":"publish","type":"glossary","link":"https:\/\/soliton-gmbh.de\/en\/glossary\/coherent-anti-stokes-raman-scattering-mit-vergleich-zur-raman-spektroskopie\/","title":{"rendered":"CARS versus Raman"},"content":{"rendered":"
\n Brief explanation<\/strong>\n

\n CARS (Coherent Anti-Stokes Raman Scattering) is a nonlinear, coherent spectroscopic method for the investigation of molecular vibrations. Unlike spontaneous Raman spectroscopy, the signal is generated by the interaction of multiple laser fields. This enables CARS to perform particularly fast, sensitive, and spatially resolved chemical imaging under suitable conditions \u2013 often without additional labeling of the sample.\n <\/p>\n<\/div>\n\n\n\n

CARS is a spectroscopy method that has been known for decades and was used in particular to study combustion processes such as in engines and car engines. The CARS effect is a third-order nonlinear effect. Here, two laser beams intersect (pump beam \u03c9P<\/sub> and Stokes beam \u03c9S<\/sub>) in a medium and the antistoke ray \u03c9aS<\/sub> is generated. With this, the chemical structure, the temperature and the pressure can be determined based on the Raman selection rules.<\/p>\n\n\n\n

Until now, these experiments were complex and required expensive fs laser devices. Leukos has now developed a white light laser that enables the construction of cost-effective, easy-to-use and quickly adjustable broadband CARS systems.<\/p>\n\n\n\n

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The figure above shows the schematic structure of our CARS system, which is coupled to a high-performance Raman system from Renishaw. A supercontinuum source from Leukos consisting of a sub-ns pulsed microChip laser (Nd:YAG @ 1064nm) and a photonic crystal fiber (PCF) serves as excitation for CARS. Part of the beam goes into the PCF, which broadens the pulse spectrally to 400 to 2000 nm, with wavelengths <1064 nm being blocked by means of a long-pass filter, which would otherwise overlay the anti-Stokes signal. The remaining longer-wave portion >1064nm represents the broadband Stokes source. The narrow-band pump beam is radiated into a delay line to compensate for the path length difference of the PCF. The two beams are superimposed using a dichroic mirror. However, these parts could be used for other processes, such as the stimulated Raman effect or the stimulated CARS effect. The lens is used to focus on the sample, thus generating the CARS signal in transmitted light. The light is captured with the lens of the \u203aRaman Renishaw inVia\u2039 and analyzed using the spectrometer and CCD of the Raman system.<\/p>\n\n\n\n

In this way, the CARS signal traverses the same optical path as the Raman signal. A motorized change of the filter sets in the Raman system in a matter of seconds enables the user to carry out CARS and Raman measurements at the same location and almost simultaneously. This allows a direct comparison of both methods and a direct decision to be made as to which measurement method is more effective.<\/p>\n\n\n\n

CARS versus Raman<\/h2>\n\n\n\n

CARS measurements are significantly more sensitive than Raman measurements at comparable parameters due to nonlinearity. This is especially true for strong Raman scatterers and to a lesser extent for weak ones. The nonlinearity of the CARS effect also leads to a higher local resolution, which is illustrated in the lower graph. With lenses with 20x magnification, CARS achieves a factor \u22484 in better depth resolution than Raman, with the resolution shown here being limited by the sample setup. With suitable lenses, resolutions that are significantly in the sub-\u03bc range can be achieved and do not suffer from Abbe\u2019s resolution limitation.<\/p>\n\n\n\n

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In addition, the anti-Stokes signal is blue-shifted and therefore has a shorter wavelength than the irradiated laser. In contrast to Raman, with CARS there are no disruptive fluorescence effects that would otherwise be superimposed on the signal. With more intensive CARS signals, measurement times can be drastically reduced while the resolution is increased at the same time. This means that fast 2D and 3D mappings can be implemented on dynamic processes, such as concentration measurements in microchannels.<\/p>\n\n\n\n

However, a disadvantage is the interference with a non-resonant background caused by non-resonant four-photon interaction, which changes the line shape and complicates the analysis of the spectra. This can be corrected using mathematical methods or suppressed experimentally using polarization techniques.<\/p>\n\n\n\n

Folded BoxCARS, in which the pump beam is split into two beams, is particularly suitable for this. This leads to a further narrowing of the scattering volume due to the smaller overlapping of the beams. With this method, even higher spatial resolutions can be achieved, with which volumes in the attoliter range can be examined. Another advantage results from the anti-Stokes beam, which is spatially separated from the other beams, which simplifies the spectral analysis with regard to the choice of filters.<\/p>\n\n\n\n

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Because of the new structure and the reduced costs, we see completely new application possibilities in addition to the study of combustion processes mentioned above:<\/p>\n\n\n\n