Superluminescent Sources
Author: the photonics expert Dr. Rüdiger Paschotta
Acronym: SFS
Definition: optical sources based on superluminescence
Categories: photonic devices, non-laser light sources
DOI: 10.61835/dh2 Cite the article: BibTex plain textHTML Link to this page LinkedIn
Superluminescent sources (also called ASE sources) are broadband light sources (white light sources) based on superluminescence. (They are sometimes erroneously called superfluorescent sources, which would be based on the substantially different phenomenon of superfluorescence.) Essentially, a superluminescent source contains a laser gain medium which is excited in order to emit and then amplify luminescent light.
A superluminescent source has a very low temporal coherence, resulting from the large emission bandwidth (compared with that of, e.g., a laser). That greatly reduces the tendency for laser speckle, as are often observed with laser beams, e.g. from laser diodes. On the other hand, the spatial coherence is usually very high: the output of a superluminescent source can be very well focused (similar to a laser beam) and is thus suitable for obtaining by far higher optical intensities than with an incandescent lamp, for example. This combination of low temporal and high spatial coherence makes such devices interesting for applications such as optical coherence tomography (OCT) (e.g. in the medical sector), device characterization (e.g. in optical fiber communications), gyroscopes, and fiber-optic sensors. See the article on superluminescent diodes for more details on applications.
The main kinds of superluminescent sources are superluminescent diodes (SLDs) and fiber amplifiers. Fiber-based sources can provide much higher output powers, whereas SLDs are much more compact and also cheaper. In both cases, the emission bandwidth is at least several nanometers and often tens of nanometers, sometimes even well above 100 nm.
For all high-gain ASE sources, it is very important carefully to suppress any optical feedback, e.g. via reflections from fiber ends because this can lead to parasitic lasing. (Using a Faraday isolator may not be sufficient.) For fiber-based devices, Rayleigh scattering from within the fiber may introduce the final performance limitations.
More to Learn
Encyclopedia articles:
- superluminescence
- amplified spontaneous emission
- superluminescent diodes
- white light sources
- coherence
Suppliers
The RP Photonics Buyer's Guide contains 39 suppliers for superluminescent sources. Among them:
Spectra Quest Lab
Spectra Quest Lab offers ASE light sources in the 950-nm and 1040-nm bands. They have a very low gain ripple of typically 0.03 dB (RMS) and relatively flat spectral characteristics with a 3 dB bandwidth above 50 nm; PM fiber-coupled output power is 100 mW (typ.) and have come as turnkey bench-top packages. A current modulation port with 1 MHz bandwidth is provided for high-speed modulation.
Quantifi Photonics
Quantifi Photonics' SLED 1000 Series is a super-luminescent LED light source with high output power, large bandwidth and low spectral ripple. They are available in various wavelengths in compact benchtop or PXI form factors and ideal for test procedures in telecom and datacom applications.
AdValue Photonics
AdValue Photonics offers 2-μm ASE sources: the AP-ASE-2000 with over 170 nm bandwidth and 20 mW output power, and the AP-ASE-2100 with over 100 nm and 10 mW output power. Both come as a turn-key benchtop package.
Frankfurt Laser Company
Frankfurt Laser Company offers a wide range of superluminescent diodes with center emission wavelengths between 680 nm to 2400 nm. Our portfolio also includes high-power versions with output powers of tens of watts.
DK Photonics
DK Photonics offers fiber-based broadband ASE sources emitting in the telecom wavelength bands C and/or L or around 1060 nm.
Bibliography
[1] | M. J. F. Digonnet, “Theory of superfluorescent fiber lasers”, IEEE J. Lightwave Technol. 4 (11), 1631 (1986); https://doi.org/10.1109/JLT.1986.1074661 |
[2] | P. F. Wysocki et al., “Broadband fiber sources for gyros”, Proc. SPIE 1585, 371 (1992); https://doi.org/10.1117/12.135068 |
[3] | P. F. Wysocki et al., “Characteristics of erbium-doped superfluorescent fiber sources for interferometric sensor applications”, IEEE J. Lightwave Technol. 12 (3), 550 (1994); https://doi.org/10.1109/50.285318 |
[4] | R. Paschotta et al., “Efficient superfluorescent light sources with broad bandwidth”, J. Sel. Top. Quantum Electron. 3 (4), 1097 (1997); https://doi.org/10.1109/2944.649547 |
[5] | P. Wang and W. A. Clarkson, “High-power, single-mode, linearly polarized, ytterbium-doped fiber superfluorescent source”, Opt. Lett. 32 (17), 2605 (2007); https://doi.org/10.1364/OL.32.002605 |
[6] | G. Smith et al., “High-power near-diffraction-limited solid-state amplified spontaneous emission laser devices”, Opt. Lett. 32 (13), 1911 (2007); https://doi.org/10.1364/OL.32.001911 |
[7] | D. Y. Shen et al., “Broadband Tm-doped superfluorescent fiber source with 11 W single-ended output power”, Opt. Express 16 (15), 11021 (2008); https://doi.org/10.1364/OE.16.011021 |
[8] | M. Blazek et al., “Unifying intensity noise and second-order coherence properties of amplified spontaneous emission sources”, Opt. Lett. 36 (17), 3455 (2011); https://doi.org/10.1364/OL.36.003455 |
[9] | R. Paschotta, case study on a fiber-based ASE source |
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