| Literature DB >> 29302348 |
Katherine J I Ember1,2, Marieke A Hoeve2, Sarah L McAughtrie1, Mads S Bergholt3,4,5, Benjamin J Dwyer2, Molly M Stevens3,4,5, Karen Faulds6, Stuart J Forbes2, Colin J Campbell1.
Abstract
The field of regenerative medicine spans a wide area of the biomedical landscape-from single cell culture in laboratories to human whole-organ transplantation. To ensure that research is transferrable from bench to bedside, it is critical that we are able to assess regenerative processes in cells, tissues, organs and patients at a biochemical level. Regeneration relies on a large number of biological factors, which can be perturbed using conventional bioanalytical techniques. A versatile, non-invasive, non-destructive technique for biochemical analysis would be invaluable for the study of regeneration; and Raman spectroscopy is a potential solution. Raman spectroscopy is an analytical method by which chemical data are obtained through the inelastic scattering of light. Since its discovery in the 1920s, physicists and chemists have used Raman scattering to investigate the chemical composition of a vast range of both liquid and solid materials. However, only in the last two decades has this form of spectroscopy been employed in biomedical research. Particularly relevant to regenerative medicine are recent studies illustrating its ability to characterise and discriminate between healthy and disease states in cells, tissue biopsies and in patients. This review will briefly outline the principles behind Raman spectroscopy and its variants, describe key examples of its applications to biomedicine, and consider areas of regenerative medicine that would benefit from this non-invasive bioanalytical tool.Entities:
Year: 2017 PMID: 29302348 PMCID: PMC5665621 DOI: 10.1038/s41536-017-0014-3
Source DB: PubMed Journal: NPJ Regen Med ISSN: 2057-3995
Fig. 1"Jablonski" style diagram of energetic transitions involved in Raman scattering. Rayleigh scattering is elastic; the incident photon is of the same energy as the scattered photon. Raman scattering is inelastic; in Stokes scattering, the incident photon is of greater energy than the scattered photon, while in anti-Stokes scattering, the incident photon is of lower energy
Fig. 2a Schematic diagram of a Raman spectrometer adapted from Butler et al.[20] (Permission obtained from Nature Publishing Group). Excitation light is represented by a blue line, while the green line represents scattered light. Excitation light travels from the laser source, through narrow band pass filters, beam expander and a dichroic mirror. It is then reflected off a mirror into a system of optics where it is directed onto the sample. Light scattered from the sample is collected by the optics and is directed by focusing mirror and long pass filters onto a grating through which it is dispersed. This dispersed light is finally focused onto the detector. b Raman spectrum of phenylalanine crystals using a 532 nm laser at 30 mW power and 1 s exposure using a 50× air objective. Spectral resolution of the system is 0.5 cm−1
Summary of Raman spectroscopy techniques
| Raman technique | Brief description | Advantages | Applications in biomedicine |
|---|---|---|---|
| Spontaneous Raman spectroscopy | Detects intrinsic Raman scattering of molecules. Can be combined with fibre probes or microscopy to give spatial and biochemical information | Label free, non-invasive and non-destructive, no sample preparation required | Diagnostics, guided surgery,[ |
| RRS | Particular bands enhanced by matching the excitation wavelength with electronic resonance of molecules, can be coupled with SERS | 103–105-fold increase in signal-to-noise, chromophores can be investigated | Characterising specific biomolecules e.g., carotenoids, cytochrome[ |
| SERS | Raman signal is enhanced using roughened metal surface e.g., nanoparticles, metal coated slide | 106-fold increase in signal-to-noise, functionalised nanoparticles | pH and redox measurements,[ |
| SORS | Raman signal measured at site offset from point of excitation, to collect diffusely scattered photons | Allows greater penetration into sample, more depth information in thicker tissues | Potential detection of calcifications and cancer margins in breast tissue[ |
| SRS/CARS | Non-linear variants requiring pulsed, synchronised laser source. | Video rate, label free biomolecular imaging, 5× increase in signal-to-noise | Imaging specific molecules of interest e.g., hydroxyapatite, lipids, drugs[ |
Fig. 3a False colour map of peak due to ring breathing (associated with cytochrome, signal integrated between 740–760 cm−1) in cryosection of murine liver tissue. Regions of low peak signal intensity are marked in red, while regions of high intensity are marked in yellow. Raman spectra were acquired with a 532 nm laser at 6 mW power, 3 s exposure and 1 μm resolution using a 50× air objective. False colour scale bar of signal-to-baseline intensity (arbitrary units) is shown to the right of the map. b Example Raman spectrum from the acquired map
Fig. 4Multivariate analysis such as linear discriminant analysis can be used to separate Raman data into pathologically diagnostic classes. Here, PC-LDA (principal component linear discriminant analysis) was used to separate mucosal tissues into three clinically distinct subsets. Numbers in brackets indicate the number of spectra in each subset. This methodology allowed correct prediction of disease states in 93% of measured spectra compared to histopathology.[96] (Figure reproduced from ref. 96 with permission from Prof. N. Stone and Journal of Pathology, John Wiley and Sons). LDA, unlike PCA, does require a priori knowledge of how many subsets of data are expected. Nevertheless, a way of analysing the data could be instrumental in accurate diagnoses
Fig. 5Advantages and disadvantages of Raman spectroscopy
Fig. 6Summary of some potential applications for Raman spectroscopy to the field of regenerative medicine