Visualizing myelination is an important goal for many researchers studying the nervous system. CARS is a technique that is compatible with immunofluorescence that can natively image lipids within tissue such as the brain illuminating specialized structures such as myelin.
Coherent anti-Stokes Raman spectroscopy (CARS) is a technique classically employed by chemists and physicists to produce a coherent signal of signature vibrations of molecules. However, these vibrational signatures are also characteristic of molecules within anatomical tissue such as the brain, making it increasingly useful and applicable for Neuroscience applications. For example, CARS can measure lipids by specifically exciting chemical bonds within these molecules, allowing for quantification of different aspects of tissue, such as myelin involved in neurotransmission. In addition, compared to other techniques typically used to quantify myelin, CARS can also be set up to be compatible with immunofluorescent techniques, allowing for co-labeling with other markers such as sodium channels or other components of synaptic transmission. Myelination changes are an inherently important mechanism in demyelinating diseases such as multiple sclerosis or other neurological conditions such as Fragile X Syndrome or autism spectrum disorders is an emerging area of research. In conclusion, CARS can be utilized in innovative ways to answer pressing questions in Neuroscience and provide evidence for underlying mechanisms related to many different neurological conditions.
Action potentials are the basic unit of information in the brain, and action potential propagation through axons forms one pillar of information processing1,2,3. Neurons typically receive afferent inputs from multiple other neurons and integrate these inputs within a given narrow time window4,5. Therefore, the mechanisms of action potential propagation in axons have received a significant amount of attention from investigators.
When propagating through an axon, an action potential is regenerated repeatedly along the axon to ensure reliable propagation6. In most neurons of jawed vertebrates (gnathostomes) axons are surrounded by a sheath of myelin, which is a lipid-rich substance produced by nearby oligodendrocytes or Schwann cells, which are types of glial cells (reviewed in7,8). This myelin sheath electrically insulates the axon, reducing its capacitance and allowing action potential propagation efficiently, quickly, and with lower energy consumption. Myelin does not cover the axon uniformly, but it sheaths the axon in segments that have short gaps in between them, called the nodes of Ranvier (reviewed in9,10). Both myelination thickness, which controls the level of electrical insulation of an axon, and the spacing of the nodes of Ranvier, which control the frequency with which action potentials are regenerated along an axon, influence the speed of action potential propagation (reviewed in11).
There is a large body of literature suggesting that myelination thickness affects the speed of action potential propagation in axons12,13,14. Moreover, alterations in axon myelination can result in a number of CNS deficits15,16,17,18,19,20,21. It is therefore not surprising that the focus of many research efforts involves the measurement and characterization of axon myelination. Measurements of myelin thickness have most commonly been done with electron microscopy, a technique that requires a significant amount of tissue preparation and is challenging to use in combination with immunohistochemistry. However, there is also a faster and simpler technique to measure axon myelination that is based on Coherent Anti-Stokes Raman Spectroscopy (CARS). A CARS laser can be tuned to various frequencies and when tuned to frequencies that are suitable to excite lipids, myelin can be imaged without the need for any additional labels22. The lipid imaging can be combined with standard immunohistochemistry such that lipids can be imaged together with several fluorescent channels23. Imaging myelination with CARS is significantly faster than electron microscopy and has a resolution that is, albeit lower than EM, sufficient to detect even small differences in myelination in the same type of axons.
All experiments complied with all applicable laws, National Institutes of Health guidelines, and were approved by the University of Colorado Anschutz Institutional Animal Care and Use Committee.
1. Animals
2. Tissue preparation
3. Staining
Figure 1: CARS imaging can be combined with immunofluorescent imaging. The graphs shows that CARS imaging occurs at 660/640 nm red signal spectrum26. This wavelength is sufficiently far removed from the green, blue, or UV range, allowing for combination of the CARS signal with immunofluorescence in these ranges. Specifically, the graph also indicates the excitation and emission for Nissl tagged with blue fluorophore, which was combined with CARS during the collection of representative results for this publication. Please click here to view a larger version of this figure.
4. Imaging
NOTE: The CARS laser set up contains a fiber laser that provides the 80 MHz clock, and an OPO (Optical Parametric Oscillator) laser with a tunable range of 770-990 nm with the Stokes beam fixed at 1031 nm, which are needed for collecting the CARS signal. There is one aperture for both beams.
Figure 2: CARS instrument diagram showing CARS lasers (red arrows) and non-descanned (NDD) epi and forward detection incorporated onto a laser scanning confocal. In forward NDD we acquire CARS for C-H bonds (dark red arrows) and SHG (second harmonic generatioin) at 515 nm (orange arrow). In epi NDD, we acquire CARS for C-H bonds (dark red arrows) and 2PE (two-photon emission) autofluorescence (light blue arrow). Sequentially, fluorescence confocal images can be acquired (green arrows for visible laser, blue arrows for confocal detection). Please click here to view a larger version of this figure.
Figure 3: CARS can illuminate myelin (magenta) in brain tissue (brainstem) while also imaging Nissl (cyan) or fluorescent markers. The two panels show representative results from a Mongolian gerbil (single image M. unguiculatus, Figure 3A,C,E) and mouse (z-stack max projection M. musculus, Figure 2B,D,F) brain, indicating that this technique can be used across species. Figure 3A,B showing Nissl in cyan, C,D show the CARS signal in magenta, E,F combine the Nissl and CARS signals with each panel for gerbil or mouse, respectively. Both sets of images show a section of the medial nucleus of the trapezoid body (MNTB) in the brain stem. Neurons in the MNTB receive inputs from heavily myelinated axons, which terminate in the calyx of held, a type of giant synapse27. Scale bar is 20 µm. Please click here to view a larger version of this figure.
One of the biggest advantages of CARS microscopy over other techniques is the compatibility with fluorescent imaging23. Figure 1 shows the CARS spectra compared to Nissl tagged with immunofluorescent marker showing little/no overlap in spectra. Figure 2 illustrates the laser set up for CARS in combination with confocal microscopy. Figure 3 demonstrates two representative images, one as a single stack and one z-stack max projection from gerbil and mouse that might be obtained using CARS imaging showing both cell bodies (cyan) and myelin signal (magenta).
A growing body of literature emphasizes the role of myelin in brain function13,16,21,28. Moreover, we know that myelination thickness and myelination pattern can change in several neurological conditions such as multiple sclerosis (reviewed in29), aging (reviewed in30), autism20,31, and many others. It is therefore not surprising that more and more investigators need to assess myelination across brain tissues and animal models, in several medical conditions, and in a growing number of experimental situations. Traditional methods to image myelination in brain tissue include antibody labeling followed by light microscopy, and electron microscopy (EM). Both techniques are time consuming and require multi-step tissue preparation protocols, which are associated with possible errors and changes to tissue composition. We demonstrated an alternative method that can yield similar results much quicker due to the ability to image myelin much faster, and which can be combined with additional fluorescence light microscopy. Importantly, this technique can be used to image lipids in brain tissue without the need for additional markers or labels. This technique does not only allow for the imaging of myelin along intact axons, but it allows for the imaging of myelin breakdown products such as plaques or liquid droplets32, which have been shown to occur, for example, in multiple sclerosis33.
The frequency to which the CARS laser was tuned was suitable to bias the image heavily in favor of lipids, resulting in overall high-quality images of myelination, since myelin is by far the most common lipid-rich substance in the brain. The principle of this technique is that a CARS laser, which can be tuned to various frequencies, is tuned to 792.2 nm, which is a frequency suitable to excite CH2 bonds. These are abundant in lipids, which contain long chains of CH2 groups linked by carbon-carbon bonds with one terminal carboxylic acid group at the end. Exciting lipids with this frequency resulted in a signal that could then be imaged with standard confocal microscope detection technology. The quality of the resulting images supports quantitative analyses that can either be done by a human observer or automated algorithms34. However, this method does not exclusively label myelin since CH2 bonds are not exclusive to myelin, and therefore CARS is less specific than an antibody would be. As a result, the images show some label, which is not associated with myelin. Importantly, this background label does not compromise the quality of the measurements or the ability for quantitative analyses.
The resolution of CARS imaging is diffraction limited and similar to two photon microscopy (~250 nm) and thus lower than that of EM. Therefore, investigators who aim to assess very small differences in myelination thickness as it occurs, for example, in certain medical conditions, need to be aware of this limitation. Additional EM controls in a small sample can confirm that the resolution is sufficient for their research aim.
One major advantage of CARS for imaging of myelin, besides the speed and ease, is the ability to combine the label-free lipid imaging with fluorescence confocal microscopy. Depending on the microscope that is used for CARS, two or even three additional channels can be imaged such that myelin imaging can be combined with antibody labeling, Nissl stain, transgenic mouse lines expressing fluorescent proteins, or similar. Potential limitations using longer wavelength fluorophore are mostly because the CARS signal is observed through 640-680 nm bandpass filters that can catch the emission of green and/or red fluorophores. However, the picosecond laser used for CARS excitation has a peak pulse energy of ~10 times less than standard femtosecond laser used for two-photon excitation, translated into ~100 less fluorescence. Moreover, the 797.2 nm pulse picosecond laser used for CARS excitation is spectrally far from the peak of the two-photon cross-section absorption of the visible fluorophores. Therefore, the CARS picosecond laser is very inefficient for two-photon excitation of visible fluorophores, making the fluorescent signal negligible for crossing into the CARS detection. However, this should be tested by imaging a negative control sample that doesn’t have any fluorescent labels compared with a sample with fluorescent markers.
In conclusion, CARS imaging is a suitable technique to image myelin in brain tissue. While the resolution is comparable to standard light microscopy and thus is lower than EM, the speed, and ease of use make this technique an attractive alternative to existing methods.
The authors have nothing to disclose.
Supported by NIH R01 DC 17924, R01 DC 18401 (Klug), and NIH 1R15HD105231-01, T32DC012280, and FRAXA (McCullagh). The CARS imaging was performed in the Advanced Light Microscopy Core part of the NeuroTechnology Center at the University of Colorado Anschutz Medical Campus supported in part by NIH P30 NS048154 and NIH P30 DK116073.
Anesthetic: | |||
1 mL disposable syringe with needle 27 GA x 0.5" | Exel int | 260040 | |
Fatal + | Vortech | ||
Surgery: | |||
Spring Scissors – 8mm Cutting Edge | Fine Science Tools | 15024-10 | |
Standard tweezers | Fine Science Tools | 11027-12 | |
Perfusion: | |||
4% Paraformaldehyde | Fisher Chemical | SF994 (CS) | |
Fine Scissors – Sharp | Fine Science Tools | 14063-11 | |
Kelly hemostats | Fine Science Tools | 13019-14 | |
Millipore H2O | |||
Needle tip, 23 GA x 1" | BD precision glide | 305193 | |
Phosphate buffered saline (PBS): | |||
Potassium chloride | Sigma | P9333 | |
Potassium phosphate monobase | Sigma | P5655 | |
pump with variable flow or equivalent | |||
Sodium chloride | Fisher Chemical | s271-1 | |
Sodiumphosphate dibasic | Sigma | S7907 | |
Dissection: | |||
50 mL vial with 4% PFA | |||
Bochem Chemical Spoon 180mm | Bochem | 230331000 | |
Fine Scissors – Sharp | Fine Science Tools | 14063-11 | |
Noyes Spring Scissors | Fine Science Tools | 15011-12 | |
Pair of fine (Graefe) tweezers | Fine Science Tools | 11050-10 | |
Shallow glass or plastic tray, approximately 10" x 10" | |||
Standard tweezers | Fine Science Tools | 11027-12 | |
Surgical Scissors – Blunt | Fine Science Tools | 14000-20 | |
Slicing: | |||
Agar, plant | RPI | 9002-18-0 | |
Vibratome | Leica | VT1000s | |
well plate | Alkali Sci. | TPN1048-NT | |
Staining: | |||
AB Media: | 1n 1,000 mL of Millipore H2O | ||
Phosphate buffered (PB): | |||
Potassium Phosphate Monobase | Sigma | P5655 | |
Sodium Phosohate Dibasic | Sigma | S7907 | |
BSA (Bovine serum albumin) | Sigma life science | A2153-100g | |
Sodium Chloride | Fisher Chemical | s271-1 | |
Triton X-100 | Sigma – Aldrich | x100-500ml | |
Nissl 435/455 | Invitrogen | N21479 | |
CARS: | |||
APE picoemerald laser | Angewandte Physik & Elektronik GmbH | ||
bandpass filter (420-520 nm) | Chroma Technology | HQ470/100m-2P | |
bandpass filter (500-530 nm) | Chroma Technology | HQ515/30m-2P | |
bandpass filters (640-680 nm) | Chroma Technology | HQ660/40m-2P | |
Confocal microscope | Olympus | FV1000 | |
Cut Transfer pipet | Fisher | 13-711-7M | |
dichroic longpass 565 nm | Chroma Technology | 565dcxr | |
dichroic longpass 585 nm | Chroma Technology | 585dcxr | |
dichroic shortpass 750 nm | Chroma Technology | T750spxrxt | |
glass bottom culture dish | MatTek | P35G-0-10-C | |
glass weight (10 mm x 10 mm boro rod) | Allen Scientific Glass Inc | ||
multiphoton shortpass emission filter 680 nm | Chroma Technology | ET680sp-2p8 | |
PBS |