Stabilization and power scaling of cladding pumped Er:Yb-codoped fiber amplifier via auxiliary signal at 1064 nm

Laser Zentrum Hannover e.V., Hollerithallee 8, D-30419 Hannover, Germany.
Optics Express (Impact Factor: 3.49). 09/2009; 17(20):18304-11. DOI: 10.1364/OE.17.018304
Source: PubMed


To the best of our knowledge we report for the first time on an Yb-sensitized Er-doped cladding pumped fiber amplifier which is simultaneously seeded by two single-frequency lasers operating at 1556 nm and 1064 nm, respectively. This mode of operation ensures stable amplifier operation by reducing the gain around 1 microm wavelength to the large signal gain value, while having no significant effect on the slope efficiency of the amplification process at 1556 nm when pumping at 976 nm. We were able to demonstrate stable output power of 8.7 W at 1556 nm with an amplifier gain of > 22 dB, a co-propagating pumping scheme and the power limitation only being set by the available amount of pump power.

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    • "Seeding the amplifier with a low power laser diode ensures simple tuning, modulation and output power control. The idea of dual-wavelength amplification in Er:Yb co-doped fibers was first demonstrated experimentally by Kuhn et al [10] [11] and investigated numerically by Han et al [12] [13]. The previous experiments carried out by our group have shown a great potential of commerciallyavailable Er:Yb co-doped DC fibers in amplification of 1 µm signals under high-power pumping [14] [15] [16]. "
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    ABSTRACT: We present a difference frequency generation based (DFG) mid-infrared (mid-IR) laser source using an all-polarization-maintaining-fiber (all-PM) amplifier capable of simultaneous amplification of 1064 nm and 1550 nm signals. The amplifier incorporates a single piece of a standard erbium:ytterbium (Er:Yb) co-doped double-clad (DC) active fiber and a limited number of off-the-shelf fiber-based components. Excited by a single 9 W multimode pump, the amplifier delivered over 12.1 dB and 17.8 dB gain at 1 µm and 1.55 µm, respectively. Due to an all-PM configuration, the amplifier was exceptionally convenient for DFG of mid-IR radiation in periodically polled lithium niobate (PPLN) crystal, yielding an output power of ~200 µW in a wide spectral range spanning from 3300 to 3470 nm.
    Laser Physics Letters 10/2014; 11(10):105103. DOI:10.1088/1612-2011/11/10/105103 · 2.46 Impact Factor
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    • "Besides, the simulation shows at low pump power, the 1064-nm signal has only a slight influence on the output power. These results qualitatively agree well with the experimental results of Kuhn et al. [19]. Actually, the possibility of the reabsorption of the 1064-nm signal has also been discussed and experimentally verified in that paper. "
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    ABSTRACT: The influence of the amplified spontaneous emission (ASE) on the performance of high-power, cladding-pumped Er-Yb codoped fiber amplifiers (EYDFAs) are investigated numerically. The results show that the counter-pump-propagating Yb-band ASE is the main reason that limits the efficiency of an EYDFA at high pump power. By introducing a co-pump-propagating Yb-band signal at proper wavelength, the counter-pump-propagating Yb-band ASE can be effectively suppressed and thus the available power of the EYDFA can be remarkably improved. This method is also helpful to improve the stability of high power EYDFAs.
    IEEE Journal of Quantum Electronics 12/2010; DOI:10.1109/JQE.2010.2052789 · 1.89 Impact Factor
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    ABSTRACT: A novel kind of all-solid photonic bandgap fiber (AS-PBGF) has been used in the master oscillator power amplifier structured Er/Yb-co-doped pulsed fiber amplifier to suppress the Yb band parasitic lasing for the power scaling and safety operation. To the best of our knowledge, this is the first time to report the use of AS-PBGF to suppress the Yb band parasitic lasing. The experimental results show that the Yb band parasitic lasing has been suppressed efficiently and the amplifier power has been raised dramatically with the utilization of AS-PBGF. An output power of 2.66 W was finally obtained without any unwanted parasitic lasing.
    Applied Physics B 02/2014; 114(4). DOI:10.1007/s00340-013-5564-5 · 1.86 Impact Factor
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