Point spread function


In microscopy, what you see is never exactly what is actually there. The Point Spread Function (PSF) is the fundamental reason for this discrepancy. Think of the PSF as the “signature” of your microscop — it describes how the system takes a single, infinitesimal point of light and smears it into a 3D diffraction pattern. If you are doing quantitative microscopy (measuring intensity, size, or distance), ignoring the PSF is like trying to do carpentry with a ruler that changes length depending on where you stand.


Prerequisites

Before starting this lesson, you should be familiar with:

Learning Objectives

After completing this lesson, learners should be able to:
  • Identify PSF-induced artifacts in microscopy images, specifically axial elongation (Z-distortion) and lateral blurring.

  • Predict the impact of the PSF on quantitative measurements, including how it inflates object size and dilutes signal intensity.

  • Understand how microscope hardware configurations change the PSF.

Concept map

graph TD A[Physical Object] -->|Convolution by PSF| B(Blurred Optical Image) B -->|Quantification Process| D{Measurement Type} D -->|Morphology| E[Size/Shape Distortion] D -->|Intensity| F[Signal Dilution/Crosstalk] D -->|Localization| G[Precision Limits]

Figure


Image formation in a confocal microscope: central longitudinal (XZ) slice. The 3D acquired distribution arises from the convolution of the real light sources with the PSF.



Activities

Explore the confocal 3-D PSF of beads: in two colors and with open and closed pinhole

Completely spherical objects appear very different (i.e. non-spherical) in a fluorescence microscope if their size approaches the diffraction limit. This appearance not only depends on microscope settings like a confocal pinhole, but also their fluorescence color. If your research is concerned with objects of such a small size (a few hundred nanometer), it is of critical importance to understand these distortions in order not to mistake them for biologically meaningful shapes.


Show activity for:  

ImageJ GUI

TODO




No optical sectioning in widefield microscopy


Show activity for:  

ImageJ GUI

  • Open the example image
  • Place a ROI around the object in the image
  • Use Image › Stacks › Plot Z-axis Profile to measure the mean intensity at each z-position
  • Compute the change in intensity in percent from the brightest to the dimmest plane: %change = 100% * (max - min) / (max - bg)
    • Do this for both the confocal and the wide-field channel and compare the results
  • Repeat, now using a much larger ROI such that all the blurred wide-field signal is always included in all z-planes






Assessment

Fill in the blanks

  1. In fluorescence microscopy, the PSF causes an apparent increase in object _____ and a decrease in peak _____. This is most pronounced for structures with a physical size below _____ .
  2. The PSF is typically elongated along the _____ axis, which explains why structures often appear stretched in that direction in 3D microscopy images.

Solution

  1. In fluorescence microscopy, the PSF causes an apparent increase in object size and a decrease in peak intensity. This is most pronounced for structures with a physical size below one micrometer.
  2. The PSF is typically elongated along the z axis, which explains why structures often appear stretched in that direction in 3D microscopy images.




Follow-up material

Recommended follow-up modules:

Learn more: