When two adjacent Airy patterns reach the Rayleigh criterion, the resolution equation reduces to : This figure plots the ratio of the numerical apertures of the condenser and objective versus the minimum resolved distance between Airy patterns (Rayleigh criterion) in units of wavelength divided by the objective aperture. Where the working numerical aperture of the condenser ( NA(cond)) is determined from :įigure 1 illustrates the calculated impact of condenser numerical aperture on resolution and includes values where the objective numerical aperture is less than that of the condenser. If the specimen is not self-luminous or when the objective and condenser numerical apertures do not match, the equation for r is given by : Where n is the refractive index of the medium separating the objective front lens and the specimen, and is the half-cone of light captured by the objective. According to Abbe diffraction theory, the objective numerical aperture is determined by : Where λ is the wavelength of light with air as the immersion medium and NA(obj) is the numerical aperture of the objective (and condenser). When the objective numerical aperture matches that of the substage condenser, r is determined from the equation : In the ideal case, when the objective is aberration-free and provides a uniform circular aperture, two adjacent points are just resolved when the centers of their Airy disks are separated by r (the central Airy disk radius). In the latter instance, the two Airy patterns are said not to be resolved. At even closer approach, the separation distance is less than the central disk radius and the sum of the two peaks merges into a single peak. ![]() As the disks approach each other, the separation distance will reach a value equal to the central disk radius, a condition known as the Rayleigh criterion. When the separation distance ( D) between adjacent Airy patterns is greater than the central disk radius ( r), the sum of the intensities yields two individual peaks. In the case of Airy patterns produced by coherent illumination, the minimum separation distance must be ascertained by adding the pattern amplitudes rather than their intensities. This allows the determination of the minimum separation distance between adjacent Airy patterns by examination of the total intensity distribution (the sum of intensities) when these patterns are closely spaced or overlapping. Objects in the optical microscope that are either self-luminous or illuminated by a large-angle cone of light form Airy patterns at the intermediate image plane that are incoherent and do not interfere with each other. Airy patterns are modified to alternative diffraction patterns by lens aberrations or non-standard aperture conditions. This tutorial assumes that virtual objective lenses are completely free of aberrations, that the Airy patterns are of identical brightness, and that the unit diffraction pattern generated by the specimen through a circular aperture is in fact an Airy disk. As the Airy patterns approach each other, by adjustment of the Separation Distance slider, they eventually reach the Rayleigh Criterion limit of separation (discussed below), followed by the Sparrow limit. The Numerical Aperture slider can also be used to adjust Airy pattern size by changing the numerical aperture of a virtual microscope objective. As this value is decreased, note how the Airy disk size decreases (and resolution ( r) increases). To operate the tutorial, use the Wavelength slider on the left to adjust the wavelength of illumination. A decrease in wavelength at fixed numerical aperture will result in a decrease in Airy pattern size. The light cone size will increase with numerical aperture (at fixed wavelength) and produce a corresponding decrease in the size of the Airy disks (and an increase in resolution). Above the sliders is a simulated illumination cone that becomes wider or narrower as the numerical aperture is changed. ![]() ![]() Beneath the sliders is real-time calculation of the resolution according to Abbe diffraction theory that changes with adjustments to the sliders. ![]() Also upon initialization, the virtual Numerical Aperture slider is set to a value of 0.16 and the two Airy patterns are separated by a distance ( D) of 4.3 micrometers. The tutorial initializes with the Wavelength slider set to 528 nanometers in the green color region of the visible light spectrum. This tutorial explores how Airy disk sizes, at the limit of optical resolution, vary with changes in objective numerical aperture ( NA) and illumination wavelength, and how these changes affect the resolution ( r) of the objective (lower values for r indicate increasing resolution).
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