Blue shift due to CHA

Why Cone Half Angle (CHA or AOI) in Filter is important in Bio Imaging

This article will share what is cone half angle (CHA) or Angle of incidence ( AOI) and why they are important in bio fluorescent imaging system.

In bio imaging system, it is common to see cone angle reported as an AOI (angle of incidence) range instead of in terms of CHA (cone half angle) or f-number, but the effects of AOI and CHA differ, so they should be stated as separate parameters.  This article will share what is cone half angle  or Angle of incidence ( AOI) and why they are important in bio fluorescent imaging system.

Cone half angle  describes the extent to which an incident beam is converging or diverging. It is defined as the angle between the AOI (angle of incidence) of the incident beam and the most oblique marginal ray (Figures a-c). Therefore, a 0˚ CHA  is synonymous with collimated light, and larger cone half angles designate a pronounced convergent or divergent beam.

dichroic filters reflect specific wavelength ranges while transmitting others.

Diagrams showing uncollimated light and cone half angle for (a) an optical filter at 0° AOI (b) a dichroic filter at 45° AOI, and (c) a high-reflectivity mirror at 45° AOI (angle of incidence). Both numerical aperture (NA) and f-number (F#) are alternate properties used to describe the cone of a beam. The following formulas derived using Abbe’s Sine Condition relate CHA and f-number:

Where:

θ = half cone angle

n = refractive index of incident medium ( nair≈1 )

F# = f-number

Like increasing AOI (angle of incidence), increasing CHA  values result in a blue shift of interference filter spectra. However, because cone angle essentially represents an average of many angles of incidence, the spectral shift due to CHA is less dramatic than the shift due to tilt. The averaging effect also results in filter edges that become less steep as CHA increases. Bandpass filters, for example, will exhibit a cone shaped passband with a large CHA instead of the square spectral shape seen with collimated light. The effect of CHA is especially apparent for narrowband and ultra-narrow bandpass filters, which show decreased transmission even when Cone half angle is relatively small.

Graph demonstrating the effect of differing cone half angle values on optical filter transmission spectra. Theory data for a narrowband filter is shown at 0° AOI (angle of incidence) with average polarization

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