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Formation of broad continuous spectra through propagation of short high power pulses through nonlinear media, also known as supercontinuum generation, was first observed in 1970 and has since then been studied extensively in many different materials. The term supercontinuum does not cover a specific phenomenon but rather a plethora of nonlinear effect leading to considerable spectral broadening of optical pulses and thereby potentially octave-spanning output. The involved nonlinear effects depend on the dispersion in the material and count effects like self-phase modulation (SPM), Raman scattering, phase matching and solitons.
Supercontinuum light can be best described as ‘broad as a lamp, bright as a laser’. Incandescent and fluorescent lamps, such as those made from tungsten halogens or xenon, provide a very broad spectrum, typically 400 nm to 1,700 nm, but the intensity is limited to the quality of the filament or the efficiency of the gas excitation. Furthermore, as the light is not spatially coherent, coupling the light into the fi bre is a challenging affair, resulting in a low-power, low-brightness source with mediocre beam quality.
Lasers on the other hand have high spatial coherence and very high brightness, which enables optimum coupling to a fibre and outstanding single-mode beam quality. However, lasers are usually monochromatic, and thus if more than one wavelength is required extra lasers a specific wavelengths are required to cover a broad spectrum. A supercontinuum source bridges this gap, providing an ultrabroadband white-light spectrum but with singlemode beam characteristics and excellent pointing stability and the brightness of a laser. The figure below shows the broad emission spectrum that can be achieved.
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