Super-Resolution Imaging: Beyond the Diffraction Limit
Introduction
Super-resolution imaging overcomes the diffraction limit in microscopy, enabling visualization of structures at a nanoscale level. Pointillism, exemplified by Georges-Pierre Seurat, serves as an analogy.
Techniques like dSTORM (direct Stochastic Optical Reconstruction Microscopy) enhance resolution significantly. Myocyte confocal and dSTORM are key examples.
Nobel Prize in Chemistry 2014
The Nobel Prize in Chemistry 2014 was awarded to Eric Betzig, Stefan W. Hell, and William E. Moerner for their development of super-resolved fluorescence microscopy.
The Diffraction Limit
The diffraction limit restricts the resolution of traditional light microscopy.
Abbe Limit: Defines the resolution limit based on wavelength (λ) and numerical aperture (NA).
Formula: \α = \frac{λ}{2NA}, where (λ=488nm) and (NA=1.4), resulting in resolution around ~250nm to ~600nm. The point spread function (PSF) describes how a point light source is spread out in the image.
Super-resolution microscopy allows us to see beyond this diffraction limit.
Diffraction-Limited Resolution
In diffraction-limited resolution, images of relatively large beads reflect the true size of the object.
As bead size decreases, the diffraction-limited spot does not become smaller, limiting resolution.
Fluorescence Imaging Fundamentals
Image formation is described by the convolution of the object with the point spread function (PSF):
Object⊗PSF=Image
Numerical Aperture and Airy Disc Size
The numerical aperture (NA) and Airy disc size are critical factors influencing resolution.
4Pi Microscopy
4Pi microscopy uses two lenses to enhance resolution. Confocal microscopy is often used in conjunction.
Deconvolution
Deconvolution algorithms can improve image resolution by computationally removing the effect of the PSF.
Why Super-Resolution Microscopy?
Electron microscopy (EM) offers sub-nanometer resolution but lacks contrast and is not suitable for living specimens.
Fluorescence microscopy provides good contrast, color/multichannel imaging, flexibility, and ease of labeling, making it suitable for living and thick 3D specimens.
Biological structures of interest (genes, macromolecular protein machines) often fall within the 100-300 nm range, tantalizingly close to the classical resolution limit.
Genes: ~100-300nm (in interphase nucleus).
Macromolecular protein machines: ~100-300nm.
Cardiac dyad (RyR and DHPR protein clusters).
Replication foci.
Protein N-mers, large proteins, individual channels.
RyR 4-Mer ~30nm, nucleosomes ~10nm.
Advantages of Super-Resolution/Nanoscopy
Resolution: ~20 nm.
High contrast.
Macromolecular complex imaging.
2D and 3D imaging.
Live cell imaging.
Correlative imaging.
Ease of use and sample preparation.
dSTORM
dSTORM (direct Stochastic Optical Reconstruction Microscopy) is a super-resolution technique.
It involves acquiring a confocal image run and performing stochastic optical reconstruction.
Technical Specifications of dSTORM
Highest resolution: ~10 nm.
Limited to: 10 µm imaging depth.
Imaging time: 20-40 minutes or 24,000 to 48,000 frames.
Requires specialized fluorophores.
Factors Affecting Localization Accuracy
Quantization: Minimized by good design.
Statistical Noise: Fundamental limit.
Background: Practically very important.
Localization Accuracy: σ=Npsf std. dev., where N = number of photons. It's also related to pixel size (a) and background (b).
Photo Activated Localization Microscopy (PALM) and STORM
Photo Activated Localization Microscopy (PALM).
STORM: J Rust, M Bates, X Zhuang, Nature Methods, Aug 2006.
CD63 Lyosomal transmembrane protein
Effective resolution < 25nm Betzig et Al, Science, Aug. 2006
FPALM - S Hess, T Girirajan, M Mason, Biophysical Journal, Sept 2006
PALMIRA - Egner, A. et al., Biophys. J. , 2007
Process of Photoactivated Localization Microscopy
Normal dyes produce a diffraction-limited image.
Photoactivatable dyes are turned on by photoactivation.
After many cycles, positions of activated fluorophores are measured.
A generated image is produced.
PALM Simplified
Activate fluorophores.
Measure positions.
Bleach fluorophores.
'Paint' the result.
Photo-switchable Fluorescent Proteins (FPs)
Photoactivation: Dark -> Bright (irreversible).
Examples: PA-GFP, PA-CFP, PA-mCherry.
Photoconversion: Eg. Green -> Red (usually irreversible).
Examples: mEos, Kaede.
Photoswitching: Dark
Carbocyanine Dyes
Used in STORM (e.g., Cy3-Cy5 pairs) and direct STORM (e.g., Cy5, Cy5.5, Alexa 647).
Entry to dark state: covalent attachment of thiol, e.g., mercapto-ethyl amine (MEA).
Exit from dark state: short wavelength light, thermal oxidation, or energy transfer from activator dye.
Switching improved by oxygen removal.
Rhodamine and Oxazine Derivatives
Switching is based on different oxidation states.
Dark state: partially reduced radical.
Entry: reduction of triplet (usually via a Thiol eg MEA).
Exit: thermal oxidation, or optically.
Examples: Alexa 488, Alexa 568, Atto 655.
Application of Super-Resolution Microscopy
Imaging RyR clusters in cardiac myocytes.
Near Single-Protein Resolution
Multicolor Imaging
Sequential: measure red fluorophore, then green. Issues with bleaching & crosstalk.
Simultaneous: use ratio to categorize fluorophores. Adjustable aperture and dichroic beamsplitter cube.
Multi-Color Localization Microscopy
Application of Super-Resolution in Disease
Confocal and super-resolution imaging of fibrosis of transverse tubules in human heart failure.
3D Localization
Dye molecules switch & bleach, preventing normal z-stacks.
Need to acquire all information for 3D position simultaneously.
Encode 3D position in PSF shape by recording multiple 2D images at different defocuses.
Encoding 3D Position in Shape
Change PSF so lateral shape gives information on defocus.
3D position information is obtained from a single frame.