3.4 Image Formation

Planes in Microscopy

Figure 3.12: Planes in Microscopy

The xy plane in microscopy is the sample plane; the ‘z’ axis is along the optical axis.

Image Formation in Microscopy

Figure 3.13: Image Formation in Microscopy

Image formation is step-wise process in microscopy: if one knows the image of a geometric point, then one also knows the image of the object.

3.4.1 Image of a Point Light Source

A PSF

Figure 3.14: A PSF

Light diffracts when it passes through a microscope; the three-dimensional image of an infinitely small light source is called the Point Spread Function (i.e., PSF).

3.4.2 Rayleigh Criterion

Rayleigh Criterion

Figure 3.15: Rayleigh Criterion

The spatial resolution is the smallest distance between two point light sources. The resolution is highly subjective.

The Rayleigh limit is the center of the first airy disk that coincides with the circumference of the second airy disk.

The resolution is the radius of an airy disk.

3.4.3 Micoscope Spatial Resolution

The spatial resolution xy of a microscope d is:

\[\begin{equation} d = \frac{1.22 \lambda}{NA_\text{condenser} + NA_\text{objective}} \end{equation}\]

In most cases, \(NA_\text{condenser} = NA_\text{objective}\), so:

\[\begin{equation} d = \frac{0.61 \lambda}{NA} \end{equation}\]

The resolution between along the z-axis of a microscope is about 2d. Light microscopy has a resolution limit of about 200 nm.

3.4.4 Diffraction-Limited Objects

Examples of Diffraction-Limited Objects

Figure 3.16: Examples of Diffraction-Limited Objects

These are objects that are smaller than a microscope’s resolution. The image of these objects will be the same as that of a point light source (i.e., a PSF or an Airy disk).

3.4.5 Convolution and Deconvolution

Differences Between Convolution and Deconvolution

Figure 3.17: Differences Between Convolution and Deconvolution

Good deconvolution can increase spatial resolution to a limited extent.