Interference Filters
and Other Devices
(gratings treated elsewhere)
edited 2/6/01
chem 454
Optical Interference occurs when two light beams are superimposed
- light of different wavelengths will not participate in interference
- of course a beam with many wavelegths can have interference at each wavelength
- it's easier to analyze intereference devices by focusing on monochromatic light
- The simplest interference occurs as light passes through a thin film or thin coating
- about 10% of the light normally reflects from the face of the coating
- of the 90% transmitted, about 10% will be reflected at the interface at the bottom of the thnk film
- thse two reflected beams will travel in the same direction
- these two beams become superimposed
- the second component has had to travel further
- as a result it is out of phase with the first reflected light
- If the two beams are in phase they will undergo constructive interference
- the two waves will add, forming a wave of amplitude larger than either componenet
- the result is a brighter image (more reflection) than either wave by itself
- in fact, since Intensity is proportional to the square of the amplitude, the signal could be twice as intense as the sum of the two separate beams.
- this condition occurs if the second path exceeds the first by a multiple of the wavelength of the light
- this requires the film thickness to be half the wavelength (since light travels down and then back through the film)
- (actually, this involves the wavelength in the medium. THis will, in turn, depend on the refractive index of the medium)
- If the two beams are 180 degrees out of phase we get complete destructive interference
- if the two components are of equal amplitude, the produce a sine wave of amplitude zero (no light)
- the result is no reflection (and by default 100% transmission)
- this occurs if the film thickness is half the wavelength of light
- If the two beams are out of phase (but not 180 degrees) we will get partial interference and an intermediate result.
Applications
-
Optial Coatings: camera and binocular lenses are often coated with a quarter wave thckness of a material like MgF2 or SiO2
- this reduces the reflection at each lens surface
- it increases the light transmission
- it also eliminates stray light (strong lights might otherwise show up as a series of bright spots elsewhere in the image)
- you can often see this when driving at light if you wear glasses or in photographs taken looking into the sun.
- of course this is most effective at one wavelength, typically set at the middle of the visible range. It is still helpul (although less effective) throughout the spectrum.
-
Interference filters are often made with multiple coatings to enhance the effect
- a transmission filter can be ddesigned to transmit only a very narrow spectral region (perhaps 0.5 -1.5 nm)
- some filters are desgined to transmit all but a specfici wavelength of light (e.g., to block one line from a Hg vapor lamp.)
- some operate as wavelength specific reflection devices
- actually the same filter can act as a narrow pass filter in transmission and a band rekjection filter by reflection.
- If you titl the filter, you effectively change the path length by 1/cosine of the angle.
- this shifts the wavelength range of the device slightly (a useful trick)
- You can also buy wedge coating of varying thickness-- the wavelength transmitted chages throughout the device
-
Dichroic Mirrors are basically designed to have extremely efficient reflection
- they are built as described above
- they can often reflect over 99.999% of the light
- again, they work best at a sprecific wavelength
- they are esental for many lasers
-
Dichroic Paints and Inks
- If you make a film with multiple thin layers it has the properties above
- if reflects light better at one waavelength region
- if you break the film into tiny flackes you can add it to an ink or paint
- if will be deposited and generally alighn itself flat on the surface
- there will be some variation in angle and hence shome shifts in color
- you may see surface sparkle with a few slightly different colros
- the color shifts as you tint the object or as you walk past it
- some automobiles use such paints for greater visual effect
- the denomiation (large 20 or 10 in lower right) on new US currancy is printed in a dichroic ink to fight couterfitting
- the color shifts from green to black as you view a legitimate bill
- a photocopy is made at a fixed angle and its number will not show this effect
The Fabry-Perot Etalon
- This is basically a thin film with a highly reflective coating on the top and bottom surface
- We now focus our attention on two beams
- light passing through the top reflection surface, amking its way into the film
- the part of that light that reflects twice off the bottom and top reflective coatings
- When those two beams are in phase we get constructive interference and enhanced intensity
- actually, the beam (trapped between the reflectors) does this repeatedly
- this is comparable to many thin layers in sequence
- only light of a specific wavelength will avoid destructive interference
- the Etalon transmits light of a specific wavelength only (very narrow band)
- We can choose the wavelength by the spacing of the reflective coatings
- some devices actually have an air gap between two mirrors
- others are of fixed thickness and therfore fixed wavelength
- There is now a tunable solid state filter based on the Fabry Perot Etalon
- a thin layer of material is coated front and back with a reflective layer
- the material is one that changes its refraactive index if an electrical field is applied
- remember, the wavelength of light shifts with refractive index
- frequency stays constant, but speed shifts (hence wavelength changes)
- changing the voltage changes the wavelength of the device
- this permits simple control of wavelength with an electrical signal
- this also permits fabrication of very tiny devices if desired
- (it's much harder to make tiny devices that must rely on moving components to change wavelength)
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