• Photonics Research
  • Vol. 2, Issue 4, B70 (2014)
Gael Kervella1, Jeremy Maxin2, Mickael Faugeron1, Perrine Berger2, Hadrien Lanctuit2, Gregoire Pillet2, Loic Morvan2、*, Frederic van Dijk1, and and Daniel Dolfi2
Author Affiliations
  • 1III-V Lab, a Joint Laboratory of Alcatel Lucent Bell Labs, Thales Research & Technology, and CEA-LETI, Campus Polytechnique, 1, Av. A. Fresnel, 91767 Palaiseau, France
  • 2Thales Research and Technology, Campus Polytechnique, 1, Av. A. Fresnel, 91767 Palaiseau, France
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    DOI: 10.1364/PRJ.2.000B70 Cite this Article Set citation alerts
    Gael Kervella, Jeremy Maxin, Mickael Faugeron, Perrine Berger, Hadrien Lanctuit, Gregoire Pillet, Loic Morvan, Frederic van Dijk, and Daniel Dolfi. Laser sources for microwave to millimeter-wave applications [Invited][J]. Photonics Research, 2014, 2(4): B70 Copy Citation Text show less

    Abstract

    We present several laser sources dedicated to advanced microwave photonic applications. A quantum-dash mode-locked laser delivering a high-power, ultra-stable pulse train is first described. We measure a linewidth below 300 kHz at a 4.3 GHz repetition rate for an output power above 300 mW and a pulse duration of 1.1 ps after compression, making this source ideal for microwave signal sampling applications. A widely tunable (5–110 GHz), monolithic millimeter-wave transceiver based on the integration of two semiconductor distributed feedback lasers, four amplifiers, and two high-speed uni-traveling carrier photodiodes is then presented, together with its application to the wireless transmission of data at 200 Mb∕s. A frequency-agile laser source dedicated to microwave signal processing is then described. It delivers arbitrary frequency sweeps over 20 GHz with high precision and high speed (above 400 GHz∕ms). Finally, we report on a low-noise (below 1 kHz linewidth), solid-state, dual-frequency laser source. It allows independent tuning of the two frequencies in the perspective of the implementation of a tunable optoelectronic oscillator based on a high-Q optical resonator.
    f=c(λ2λ1)λ2λ1.(1)

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    Elaser(t)=Alasersin(2πflasert+2π0tδflaser(t)dt+φlaser(t)),(2)

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    verror=Aerrorsin(2πflaserτ+φlaser(t)φlaser(tτ)),(3)

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    vref=Arefsin(2πfAOt+φref(t)),(4)

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    φref(t)=2πtτtδflaser(t)dt2πτδflaser(t),(5)

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    Gael Kervella, Jeremy Maxin, Mickael Faugeron, Perrine Berger, Hadrien Lanctuit, Gregoire Pillet, Loic Morvan, Frederic van Dijk, and Daniel Dolfi. Laser sources for microwave to millimeter-wave applications [Invited][J]. Photonics Research, 2014, 2(4): B70
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