access icon openaccess Q-switching and mode-locking pulse generation with graphene oxide paper-based saturable absorber

Q-switched and mode-locked erbium-doped fibre lasers (EDFLs) are demonstrated by using non-conductive graphene oxide (GO) paper as a saturable absorber (SA). A stable and self-starting Q-switched operation was achieved at 1534.4 nm by using a 0.8 m long erbium-doped fibre (EDF) as a gain medium. The pulse repetition rate changed from 14.3 to 31.5 kHz, whereas the corresponding pulse width decreased from 32.8 to 13.8 µs as the pump power increased from 22 to 50.5 mW. A narrow spacing dual-wavelength Q-switched EDFL could also be realised by including a photonics crystal fibre and a tunable Bragg filter in the setup. It can operate at a maximum repetition rate of 31 kHz, with a pulse duration of 7.04 µs and pulse energy of 2.8 nJ. Another GOSA was used to realise mode-locked EDFL in a different cavity consisting of a 1.6 m long EDF in conjunction with 1480 nm pumping. The laser generated a soliton pulse train with a repetition rate of 15.62 MHz and pulse width of 870 fs. It is observed that the proposed fibre lasers have a low pulsing threshold pump power as well as a low damage threshold.

Inspec keywords: Bragg gratings; Q-switching; optical pumping; optical filters; laser mode locking; photonic crystals; optical solitons; fibre lasers; graphene; holey fibres; erbium; paper; optical tuning; optical pulse generation; laser cavity resonators; optical saturable absorption

Other keywords: pulse repetition rate; wavelength 1534.4 nm to 1480 nm; soliton pulse train; threshold pump power; CO; tunable Bragg filter; energy 2.8 nJ; Q-switching; gain medium; erbium-doped fibre lasers; self-starting Q-switched operation; power 22 mW to 50.5 mW; mode-locking pulse generation; frequency 14.3 kHz to 31.5 kHz; distance 0.8 m to 1.6 m; cavity; pump power; saturable absorber; low damage threshold; photonics crystal fibre; nonconductive graphene oxide paper

Subjects: Laser beam modulation, pulsing and switching; mode locking and tuning; Laser resonators and cavities; Optical solitons; Gratings, echelles; Photonic bandgap materials; Optical saturation and related effects; Ultrafast optical techniques; Optical transient phenomena, self-induced transparency, optical saturation and related effects; Laser beam modulation, pulsing and switching; mode locking and tuning; Design of specific laser systems; Optical solitons; Fibre lasers and amplifiers; Optical coatings and filters; Fibre lasers and amplifiers; Spectral and other filters; Laser resonators and cavities

References

    1. 1)
      • 26. Jorio, A., Saito, R., Dresselhaus, G., Dresselhaus, M.S., Dresselhaus, G.: ‘Raman spectroscopy in graphene related systems’ (WILEY-VCH Verlag GmbH & Co. KGaA, Germany, 2011).
    2. 2)
    3. 3)
    4. 4)
    5. 5)
    6. 6)
    7. 7)
    8. 8)
    9. 9)
    10. 10)
    11. 11)
    12. 12)
    13. 13)
      • 30. Liu, J., Wu, S., Yang, Q., Song, Y., Wang, Z., Wang, P.: ‘163 nJ graphene mode-locked Yb-doped fiber laser’. CLEO:2011 – Laser Applications to Photonic Applications, OSA Technical Digest (CD), 2011, paper JWA23.
    14. 14)
    15. 15)
    16. 16)
    17. 17)
    18. 18)
    19. 19)
    20. 20)
    21. 21)
    22. 22)
    23. 23)
    24. 24)
    25. 25)
    26. 26)
    27. 27)
    28. 28)
    29. 29)
    30. 30)
http://iet.metastore.ingenta.com/content/journals/10.1049/joe.2014.0321
Loading

Related content

content/journals/10.1049/joe.2014.0321
pub_keyword,iet_inspecKeyword,pub_concept
6
6
Loading