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Technology Guide Principles – Applications – Trends - hhimawan

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2<br />

Laser<br />

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medicine<br />

<strong>Principles</strong><br />

Since they first appeared in 1960, lasers as a light<br />

source have established themselves in a growing<br />

number of applications in industry and in everyday<br />

life. Laser light differs from other light sources, such as<br />

light bulbs or neon lamps, by its very narrow spectral<br />

bandwith as well as its high temporal and spatial stability<br />

and consistency.<br />

“Laser” stands for Light Amplification by Stimulated<br />

Emission of Radiation, whereby radiation in this<br />

context refers to a stream of light particles (photons).<br />

Light amplification depends on the existence of a laseractive<br />

medium <strong>–</strong> a material in which a discrete amount<br />

of energy can be deposited (absorption) and subsequently<br />

released (emission) at an atomic level. Emission<br />

can be spontaneous, being either induced by the<br />

medium itself, or stimulated by other photons, as is the<br />

case for lasers. The newly generated photons have the<br />

same properties as those already existing, in terms of<br />

colour of light or wavelength.<br />

The wavelength of the generated photons can be<br />

modified according to the condition of the laser-active<br />

medium, which can be either a gas, a liquid or a crystal<br />

to which specific atoms have been added. This<br />

means that each laser can typically only emit photons<br />

within a small defined wavelength range. Since the<br />

wavelength not only represents the colour of the light<br />

particles but also their energy, photons of different<br />

wavelengths also possess different amounts of energy.<br />

Thus, light particles with a wavelength in the blue<br />

spectral range possess greater energy than photons<br />

with a wavelength in the red spectral range.<br />

pumping<br />

end mirror output mirror<br />

laser-active<br />

medium<br />

laser<br />

beam<br />

� Laser setup: The mirrors serve to generate a light field from<br />

identical photons by backcoupling already generated photons. To<br />

maintain the laser beam, energy must be deposed continuously<br />

in the laser­active medium by “pumping”.<br />

wavelength<br />

� Categorisation and characterisation of some laser types<br />

Aside from the energetically loaded laser-active<br />

medium <strong>–</strong> the crystal, liquid or gas <strong>–</strong> it is necessary to<br />

feed back the generated photons into the medium using<br />

a resonator, so that a resonant field of laser light<br />

comprising a large amount of identical photons builds<br />

up by further stimulated emission. Typically, the resonator<br />

consists of two oppositely positioned mirrors for<br />

each wavelength. One of the resonator mirrors is highly<br />

reflective to laser light. The other mirror allows part of<br />

the laser light to exit the resonator. Energy must be deposited<br />

continuously in the laser-active medium, in a<br />

process known as “pumping”. This ensures that sufficient<br />

stimulated emission is generated on a continuous<br />

basis to maintain constant laser operation. The pumping<br />

of the laser-active medium can be accomplished in<br />

several ways, such as generating an electrical field in<br />

the laser-active medium or by irradiating the medium<br />

with light.<br />

Lasers are categorised in different ways, i. e. according<br />

to their operating mode (continuous-wave or<br />

pulsed) or the type of the laser-active medium (solid<br />

state laser, gas laser, diode laser, etc.).<br />

Continuous-wave lasers are systems that emit laser<br />

light continuously. These systems are most easily char

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