• Light Amplification by Stimulated Emission of Radiation.
- when highly focussed energy is required (light or heat)
- when contact forces must be eliminated
- when a small geometry is required
- Produce collimated light - all of the light rays are (nearly) parallel. This means the light doesn’t diffuse quickly like normal light.
- Monochromatic - because the light is generated using specific gases, the frequency (wavelength) has a specific value. Normal white light tends to contain a wide mixture of different frequencies (a wide spectrum), but laser light is very specific.
- The light has significantly less power than a normal light bulb, but it is highly focussed, thus delivering a significantly higher light intensity.
• The principle behind lasers are
1. Excitation of light emission by electrical discharge.
2. Resonance - the laser chamber has reflecting ends separated by a multiple of half wavelengths one end is completely reflecting, and the other end is partially reflecting. The result is a reflection that leads to resonance.
• The height of the orbit the electron is in determines the wavelength of the photon. Larger atoms have higher orbits, therefore longer wavelengths (infrared). Smaller atoms have shorter falls, therefore shorter wavelengths (Ultraviolet).
• The electrons are caused to jump by a discharge of electrons with a potential charge in the range of KV.
• Various gases are used in Lasers. The contents of a laser can be a single gas, or a combination of gases.
- e.g. in a CO2 laser, CO2 is used to produce light with a 10.6 micrometer wavelength. Nitrogen is used to maintain electron populations in the upper valence shell of the CO2 molecules. Helium is used as an intracavity cooling agent.
• Lasers are very inefficient and build up excessive heat. If this heat becomes high enough it will effect the performance, and eventually damage the laser. To counteract this, heatsinks, water, and other forms of heat dissipation are used.
• The lasers often have sensors to shutdown when the temperatures become too high.
• Absorption is when energy causes an electron to accept enough energy to jump up one or more energy levels.
• Spontaneous emission is the drop of the electron to a lower energy orbit, and the release of the energy change as a photon.
• Absorption can be caused by energy sources, such as light, but it is also caused by the heat of an object. (as with incandescent lights)
• We can draw out a spectrum for frequencies emitted.
• Fluorescence is light of one color that causes emission of light of another color. (a shorter wavelength).
• In a laser the energy levels are increased to move more than 50% of the electrons (in the lasing material) to a higher energy state.
• The usual population inversion allows incoming photons to cause a new photon to be emitted without being absorbed itself. The two photons have,
**** This effect is also a 2 times amplification
1. The electrical/light discharges are used to cause electron population inversion and cause a few spontaneous emissions of photons.
2. The new photons travel in all directions, but some travel toward the mirrors, where they are reflected back and forth between the mirrors.
3. As the photons travel, they cause the generation of other photons travelling in the same direction.
4. This builds until the laser has a high intensity output.
5. The output beam escapes through one end of the laser that has a half silvered mirror.
• Various lasers are suited to different applications.
• Efficiency of lasers is often about 0.1% for gas, but CO2 can be as high as 18%.
Harry, J. E., Industrial Lasers and Their Applications, McGraw-Hill, London, 1974.
Hugel, H., Lasers in Manufacturing, Proceedings of the 5th, International Conference, Sept., 1988, Stuttgart, West Germany.
Ready, J. F., Lasers in Modern Industry, Society of Manufacturing Engineers, Dearborn Michigan, 1979.
Soares, O. D. D., and Perez-Amor, M., Applied Laser Tooling, Martinus Nijhoff Publishers, Lancaster UK, 1987.