Superluminescent Diodes (SLD)

A superluminescent light emitting diode is, similar to a laser diode, based on an electrically driven pn-junction that, when biased in forward direction, becomes optically active and generates amplified spontaneous emission over a wide range of wavelengths. The peak wavelength and the intensity of the SLD depend on the active material composition and on the injection current level. SLDs are designed to have high single pass amplification for the spontaneous emission generated along the waveguide but, unlike laser diodes, insufficient feedback to achieve lasing action. This is obtained very successfully through the joint action of a tilted waveguide and anti-reflection coated facets.

SLDs are optical sources with a rather wide optical bandwidth. In that they differ from both lasers, that have a very narrow spectrum, and white light sources, that exhibit a much larger spectral width. This characteristic mainly reflects itself in a low temporal coherence of the source (which is the limited capability of the emitted light wave to maintain the phase over time). SLDs may however exhibit a high degree of spatial coherence, meaning that they can be efficiently coupled into single-mode optical fibers. Some applications take advantage of the low temporal coherence of SLDs sources to achieve high spatial resolution in imaging techniques. The coherence length is a quantity frequently used to characterize the temporal coherence of the light source. It is related to the path difference between the two arms of an optical interferometer over which the light wave is still capable to generate an interference pattern.

On the one hand SLDs are semiconductor devices that are optimized to generate a large amount of amplified spontaneous emission (ASE). In order to do that, they incorporate high-power gain sections in which seeding spontaneous emission is amplified with high gain factors of 30 dB or more. On the other hand SLDs lack optical feedback, so that no laser action can occur. Optical feedback resulting from back-reflections of light from optical components such as e.g. connectors into the cavity is suppressed by means of tilting the facets relative to the waveguide, and can be suppressed further with anti-reflection coatings. The formation of resonator modes and thus pronounced structures in the optical spectrum and/or to spectral narrowing are avoided.

Typical parameters of fiber-coupled SLDs

Part numberMean
wavelength
Bandwith
FWHM
Output
power
Maximum
wavelength
Spectrum
dip
Ripples
RMS1
PEROperating
current
nmnmmWnmdBdBdBmA
SLD-1000-100-YY-25 100010025955, 103010.0220600
SLD-1030-120-YY-15103012015970, 105040.0220550
SLD-1030-20-YY-15010302013010300.0420800
SLD-1050-90-YY-351050903510500.220700
SLD-1060-20-YY-15010652513010600.0520800
SLD-1060-20-YY-30010602030010600.3201600
SLD-1064-20-YY-350106420350116418750
SLD-1080-30-YY-10010803010010800.0520800
SLD-1130-20-YY-301130273011250.0320300
SLD-1140-85-YY-111408511110, 117040.0520400
SLD-1190-90-YY-111909011160, 122550.0220300
SLD-1250-110-YY-5125011051210, 128060.0520800
SLD-1280-50-YY-1128050112800.0220400

1 – @ ASE maximum, RMS in 1 nm range, 10pm resolution

Any customized wavelength from the 780-1330 nm range is possible. Please, contact us for the details.