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Raman spectroscopy
Raman spectroscopy is a spectroscopic technique that provides non-destructive analysis capable of identifying components within mixtures with chemical specificity without complex sample preparation. Raman spectroscopy relies on photon scattering following visible light radiation, where the shift in photon energies corresponds to information about the system’s vibrational modes and their frequencies. Upon obtaining vibration mode frequencies, qualitative classifications about the system can be both made and reinforced.

Raman spectroscopy works well in parallel with microfluidic devices for many qualitative biological applications. For some applications, Raman spectroscopy is preferred over other detection methods such as infrared (IR) spectroscopy as water has a strong interference signal with IR but not with Raman. Likewise, methods such as high-performance liquid chromatography (HPLC), nuclear magnetic resonance (NMR), mass spectrometry (MS), or gas chromatography (GC) are also not ideal as these methods require larger sample sizes. Since microfluidics enables experiments with small volumes (including analysis of single cells or few cells), Raman is a leading microfluidic detection method. Specifically, Raman integration with microfluidic devices has strong applications in systems where lipid identification is necessary, common in biofuel research. For example, a lipid fluorescent assay is not selective enough and thus cannot identify molecular differences the way Raman can through molecular vibrations. Raman, when coupled with microfluidic devices, can also monitor fluid mixing and trapping of liquids and can also detect solid and gas phases within microfluidic platforms, an ability that is applicable to the study of gas-liquid solubility.

Raman spectroscopy in microfluidic devices is applied and detected using either integrated fiberoptics within a microfluidic chip or by placing the device on a Raman microscope. Furthermore, some microfluidic systems utilize metallic colloids or nanoparticles within solution to capitalize on Surface-enhanced Raman spectroscopy (SERS). SERS can improve Raman scattering by up to a factor of 1011 by forming charge transfer complexes on the surfaces. It follows that these devices are commonly fabricated out of nanoporous polycarbonate membranes allowing for easy coating of nanoparticles. However, if fabricated out of polydimethylsiloxane (PDMS), signal interference with the Raman spectrum can occur. PDMS generates a strong Raman signal which can easily overpower and interfere with the desired signal. A common solution for this is fabricating the microfluidic device such that a confocal pinhole can be used for the Raman laser. Typical confocal Raman microscopy allows for spectroscopic information from small focal volumes less 1 micron cubed, and thus smaller than the microfluidic channel dimensions. Raman signal is inherently weak; therefore, for short detection times at small sample volumes in microfluidic devices, signal amplification is utilized. Multi-photon Raman spectroscopy, such as stimulated Raman scattering (SRS) or coherent anti-Stokes Raman scattering (CARS) help enhance signals from substances in microfluidic devices.

For droplet-based microfluidics, Raman detection provides online analysis of multiple analytes within droplets or continuous phase. Raman signal is sensitive to concentration changes, therefore solubility and mixing kinetics of a droplet-based microfluidic system can be detected using Raman. Considerations include the refractive index difference at the interface of the droplet and continuous phase, as well as between fluid and channel connections.