1,720,970 research outputs found

    Three-level fiber DFB laser at 980 nm

    No full text
    A three-level fiber DFB-laser operating at 977nm is demonstrated for the first time using a 910nm pump diode. The fiber DFB laser shows 17.5mW output power under a launching power of 113mW

    977-nm all-fiber DFB laser

    No full text
    Three-level operation of a fiber distributed feedback (DFB) laser operating around 980nm is demonstrated for the first time. The ytterbium-doped DFB laser shows a maximum slope efficiency of 61% and output power of 38.2mW under a launched single-mode pump power of 150mW at 910nm. The efficiency of lasers with different coupling strengths and at different pump wavelengths is also investigated

    Relaxation oscillation noise suppression in fibre DFB lasers using a semiconductor optical amplifier

    No full text
    We report the experimental results of a simple, all optical technique to reduce the relative intensity noise peak of a fibre distributed feedback laser. A noise reduction of 30dB is achieved

    Intensity noise suppression in fibre DFB laser using gain saturated SOA

    No full text
    Experimental results of a simple, all-optical technique to reduce low-frequency intensity noise in an Er-Yb codoped fibre distributed feedback (DFB) laser are reported. This method utilises the gain dynamics of a saturated semiconductor optical amplifier (SOA) to produce a reduction of 30dB in the relaxation oscillation noise component of the fibre laser

    Keyed axis single-polarisation all-fibre DFB laser

    No full text
    A single-polarised D-shaped fibre DFB laser with keyed axis output is demonstrated. The laser shows an output power of 3.8 dBm and strong axis alignment when spliced to a polarisation maintaining fibre

    Erbium-ytterbium L-band fibre-DFB laser pumped at 1534nm

    No full text
    An L-band (1618nm) fibre-DFB laser pumped at 1534nm is demonstrated for the first time. It has a threshold of <10mW and up to 2mW of optical power in a single-polarisation with a line-width of ~8kHz

    Single-polarization all-fibre DFB laser with keyed axis output

    No full text
    A single-polarized fiber DFB laser with keyed axis output is demonstrated from a D-shaped fiber configuration. The laser shows an output power of 3.8dBm and strong axis alignment when spliced to a polarization maintaining fiber

    Compact high-power tunable three-level operation of double cladding Nd-doped fiber laser

    Full text link
    We present a compact high-power continuous-wave tunable neodymium-doped double cladding fiber laser operating on three-level 4F3/2 - 4I9/2 transition with a maximum output power up to 810 mW. At 926.7 nm, it has a maximum slope efficiency of 49.3% against absorbed 808-nm pump. By compressing the fiber Bragg grating, 15-nm tuning range is achieved

    All-fibre Bragg grating filters and lasers for future optical networks

    No full text
    Bragg gratings in optical fibre waveguides have now been around for 25 years and they were soon after being realised, identified as one of the most significant fibre-optic inventions with potentials in a wide variety of areas among telecommunications equivalent to that of the erbium doped fibre amplifier. Following their creation a plurality of in-fibre functions were thought possible with low or no insertion-loss. Although fabrication and control of vital grating parameters was limited in the early stages of their life, initially a number of filtering functions were identified for obvious demonstrations. It soon became apparent though that not just standard filtering manipulation was possible. Identifying the true potential of the devices has let to considerable effort being concentrated on their full exploitation implying building an infrastructure supported by theoretical design and manufacturing techniques around them. These techniques combined have let to a scenario where currently it is the imagination more than the actual design and manufacturing capabilities that imposes a limitation to what is being demonstrated and now they find applications in most of the modern telecommunications network. Cladding-pumped fibre technology has revolutionised fibre lasers over the last decade, increasing output power from less than 1 W with traditional core-pumping to well over 100 W. Even 1 kW of power has been reached in multi-mode designs, when several devices have been arranged in series or in parallel. For output powers below 100W, a few diode bars or multi-emitter laser diode assemblies are adequate pump sources. However, for powers beyond the 100 W level, diode stacks seem to be a better choice. The increasing availability of suitable diode stacks and the possibility of efficient fibre launch make them very attractive for pumping of high-power fibre-lasers. At the same time, while fibres proved very reliable at powers up to ~100 W, it is clear that further power-scaling to the kW level with diode stack pumping requires significant fibre optimisation in terms of fibre composition, pump coupling, and/or overall device layout. This is especially true when a single-mode output is required. We will in this presentation discuss and highlight some of the most recent advances in Bragg grating devices and applications in advanced components together with the most recent advances in the area of high power fibre lasers. In particular we will show examples of the latest in Bragg gratings for dispersion-control, short pulse-manipulation, advanced filtering applications together with some of our 1kW and speculate into what the future holds for Bragg gratings and high-power lasers and amplifiers

    A 16-channel OCDMA system (4 OCDMA x 4 WDM) based on 16-chip, 20 Gchip/s superstructure fibre Bragg gratings and DFB fibre laser transmitters

    No full text
    We demonstrate an all-fibre OCDMA system comprising 16 channels (4 OCDM x 4 WDM, 100 GHz grid) incorporating DFB fibre lasers as transmitters and 16-chip, 20 Gchip/s quaternary phase superstructured fibre Bragg gratings. Error free performance at 311 Mbit/s was obtained for all 16 channels for transmission distances of up to 50km of standard fibre without the need for dispersion compensation or nonlinear optical thresholding
    corecore