The common or garden incandescent lamp emits a continuous
spectrum - ie a wide range of wavelengths in the visible and near infra
red. Most street lights use sodium vapour at either high or low pressure.
The low pressure lamps emit a bright narrow spectrum of light at around
590nm. The high pressure types emit a continuous broad visible spectrum,
but with bright peaks between 550nm and 630nm. Mercury vapour lamps, used
in security lighting, emit a broad spectrum between 540nm and 630nm with
some content in the blue region.
These wavelengths are the 'enemy'. It very much depends
on the type of object you want to observe and the way you are observing
it (by eye, film or possibly CCD), but knowing where the pollution lies
and the required observation wavelengths, it is possible to design and make
a filter to reject the 'enemy'.
As an example, deep-sky emission nebulae glow most brightly at wavelengths
as follows,
- Oxygen III, or O-III, emitting at 495nm and 500nm
- Hydrogen alpha, or H-alpha, emitting at 656nm
- Hydrogen beta, or H-beta, emitting at 486nm
A filter which cuts out all wavelengths apart from these
will give good results when observing these types of bodies.
Such filters are made in a similar fashion to the way
mirrors are metallised. They rely on the wave nature of light and the interference
effects which can be generated in very thin solid layers of transparent
material. They are called interference filters, and find application in
all sorts of devices.
Probably the biggest application of these interference
filters is on spectacle lenses. A bare surface of glass has a 4.2% reflection
loss. This means that 8.4% of light is lost from two surfaces in a spectacle
lens. This loss gives rise to glare and a loss in brightness. It is possible
using interference filter technology to reduce the reflectance of a surface
to less than 0.5%, thus eliminating glare and associated problems.