High-power tunable low-noise coherent source at 1.06µm based on a surface-emitting semiconductor laser

Exploiting III-V semiconductor technologies, vertical external-cavity surface-emitting laser (VECSEL) technology has been identified for years as a good candidate to develop lasers with high power, large coherence and broad tunability. Combined with fiber amplification technology, tunable single-fre...

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Veröffentlicht in:Applied optics (2004) 2018
Hauptverfasser: Chomet, Baptiste, Zhao, Jian, Ferrieres, Laurence, Myara, Mikhaël, Guiraud, Germain, Beaudoin, Gregoire, Lecocq, Vincent, Sagnes, Isabelle, Traynor, Nicholas, Santarelli, Giorgio, Denet, Stephane, Garnache, Arnaud
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Sprache:eng
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Zusammenfassung:Exploiting III-V semiconductor technologies, vertical external-cavity surface-emitting laser (VECSEL) technology has been identified for years as a good candidate to develop lasers with high power, large coherence and broad tunability. Combined with fiber amplification technology, tunable single-frequency lasers can be flexibly boosted to a power level of several tens of watts. Here, we demonstrate a high power, single frequency and broadly tunable laser based on VECSEL technology. This device emits in the near-infrared around 1.06 µm and exhibits high output power (>100 mW) with a low-divergence diffraction-limited TEM00 beam. It also features a narrow free-running linewidth of < 400 kHz, with high spectral purity (SMSR >55 dB), and continuous broadband tunability greater than 250 GHz (< 15 V piezo voltage, 6 kHz cutoff frequency) with a total tunable range up to 3 THz. In addition, a compact design without any movable intracavity elements offers a robust single-frequency regime. Through fiber amplification, a tunable single-frequency laser is achieved at an output power of 50 W covering the wavelength range from 1057 nm to 1066 nm. Excess intensity noise brought on by the amplification stage is in good agreement with a theoretical model. A low relative intensity noise (RIN) value of-145 dBc/Hz is obtained at 1 MHz and we reach the shot-noise limit above 200 MHz.
ISSN:1559-128X
2155-3165
DOI:10.1364/AO.57.005224