Frontiers in Neurophotonics – More
You will find below a collection of images from previous editions of the Frontiers in Neurophotonics Summer School.
Video-rate multimodal imaging in vivo
Real-time X/Y Stabilization (Software)
Real-time Z Dynamics Focusing (Hardware)
CARS Microscopy of Spinal Cord
The spontaneous Raman effect is the process by which a photon sees its frequency changed after scattering off a molecule. This change in frequency is due to the fact that the photon gives energy to the molecule to initiate a vibration (called a Stokes process) or takes energy away from the molecule to stop a vibration (called an anti-Stokes rocess).
The change in frequency is simply equal to the vibration frequency of the molecule. Since all molecules have a set of well-defined vibration frequencies that uniquely characterizes them, the measurement of the complete spectrum of photons that have scattered from a molecule can permit the identification of the molecule simply with light. This is very powerful, but somewhat inefficient.
Recent advances in laser physics have enabled the development of a new kind of microscopy based on stimulated Raman scattering. This new technique known as
Coherent anti-Stokes Raman scattering (CARS) is sensitive to the same vibrational signatures of molecules seen in Raman spectroscopy. Unlike spontaneous Raman spectroscopy (where only one beam of light is used to excite the sample), CARS employs multiple simultaneous photons (that is, multiple simultaneous beams) to excite the molecular vibrations, and produces a signal where the emitted waves are coherent with one another. As a result, the CARS signal is much stronger than the spontaneous Raman emission for similar excitation powers.
CARS is a third-order nonlinear optical process involving three laser beams (two of which have the same frequency in our setup): a pump beam of frequency ωp, a Stokes beam of frequency ωs and a probe beam at frequency ωpr (in our case ωp=ωpr). These beams interact with the sample and generate a coherent optical signal at the anti-Stokes frequency (ωp – ωs + ωpr). The latter is resonantly enhanced when the frequency difference between the pump and the Stokes beams (ωp – ωs) coincides with the frequency of a Raman resonance, which is the basis of the technique’s intrinsic vibrational contrast mechanism.
CARS microscopy allows vibrational imaging with high sensitivity, high spectral resolution and three-dimensional sectioning capabilities. It allows noninvasive characterization and imaging of chemical species and biological systems without preparation or labeling with natural or artificial fluorophores that are prone to photobleaching.
Imaging protein trafficking in and out of dendritic spines
Time lapse images of GFP-CaMKII translocation to synapses in a cultured hippocampal neuron upon synaptic stimulation (2 min) and subsequent wash.
The fluorescent protein is initially distributed throughout the cytosol of the neuron and then accumulates rapidly at synaptic sites upon stimulation.
A large fraction of the fluorescence returns to a diffuse pattern after the stimulation.
Single membrane receptor tracking
Fluorescence lifetime approaches
FLIM Setup – (Fluorescence lifetime imaging microscopy )
Fluorescence decay curve recorded with our FLIM system.
The fluorescence lifetime is extracted from the exponential fitting of the data. This lifetime is independent of fluorophore concentration and photobleaching which is very useful in many applications.
Photobleaching and Photoactivation techniques
Time lapse series of images of dendrites and spines in neurons transfected with mCherry (to highlight the morphology) and a photo-activatable GFP tagged to a synaptic protein. Using a two-photon laser, a small region (circles) is photo-activated to “light up” the protein in spines and to follow its diffusion out of the spine over time. In active neurons, this protein resides for much longer time in the synapse.