Slide 1
When using laser light sources, filters must have very sharp cutons and cutoffs since there will be many orders of magnitude more scattered laser light than fluorescence
Can specify wavelengths that filter must reject to certain tolerance (e.g., reject 488 nm light at 10-6 level: only 0.0001% of incident light at 488 nm gets through)
[RFM]
Slide 2
This lecture is intended to describe the nature and function of optical systems
It will describe how filters operate
When filters should be used
What problems and issues must be taken into consideration
Slide 3
Long pass filters transmit wavelengths above a cut-on wavelength
Short pass filters transmit wavelengths below a cut-off wavelength
Band pass filters transmit wavelengths in a narrow range around a specified wavelength
Band width can be specified
Neutral Density filter is a nondiscriminant intensity reducing filter
Absorption Filter is colored glass that absorbs unwanted light
Slide 4
Optics - Filter Properties
When a filter is placed at a 45o angle to a light source, light which would have been transmitted by that filter is still transmitted but light that would have been blocked is reflected (at a 90o angle)
Used this way, a filter is called a dichroic filter or dichroic mirror
[RFM]
Slide 5
Diffraction essentially describes a departure from theoretical geometric optics
Thus a sharp objet casts an alternating shadow of light and dark “patterns” because of interference
Diffraction is the component that limits resolution
3rd Ed. Shapiro p 83
Slide 6
Small amounts of incident light are reflected at the interface between two material of different RI
Thickness of the material will alter the constructive or destructive interference patterns - increasing or decreasing certain wavelengths
Optical filters can thus be created that “interfere” with the normal transmission of light
3rd Ed. Shapiro p 82
Slide 7
Interference filters: Dichroic, Dielectric, reflective filters…….reflect the unwanted wavelengths
Absorptive filters: Colour glass filters… absorb the unwanted wavelengths