Passive harmonic mode-locking in Tm–Ho doped fiber laser with MoS2–ZnO saturable absorber deposited on the arc-shaped fiber

buir.contributor.authorOrtaç, Bülent
buir.contributor.orcidOrtaç, Bülent|0000-0002-1104-7459
dc.citation.epage10
dc.citation.spage1
dc.citation.volumeNumber154
dc.contributor.authorAhmad, H.
dc.contributor.authorArina, M. R. N.
dc.contributor.authorSamion, M. Z.
dc.contributor.authorOrtaç, Bülent
dc.contributor.authorYusoff, N.
dc.date.accessioned2025-02-21T13:16:43Z
dc.date.available2025-02-21T13:16:43Z
dc.date.issued2024-07-10
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)
dc.description.abstractThis work reports a harmonic mode-locked Tm-Ho doped fiber laser (THDFL) using newly fabricated MoS 2 -ZnO as a saturable absorber (SA). It generates harmonic mode-locking (HML) operation with a center wavelength of 1911.4 nm and a 3-dB bandwidth of 3.02 nm. The fundamental repetition rate and pulse width were 14.1 MHz and 2.05 ps, respectively. Based on the radio frequency (RF) spectrum, the observed signal-to-noise (SNR) of the fundamental HML pulse was 67.22 dB. Increasing the pump power with fine-tuning of the polarisation controller (PC), higher order HML pulses were also observed using the MoS 2 -ZnO SA. The highest stable HML frequency was 300 MHz, observed at the 21st HML. The central wavelength and 3-dB bandwidth of the HML pulse were 1915.2 nm and 2.29 nm, respectively. The 21st HML pulses demonstrated a SNR of 40.09 dB. No supermode noise was observed in the RF spectrum, indicating that the 21st HML pulses were relatively stable. With industry demand, this high repetition rate HML with MoS 2 -ZnO SA opens new avenues for comprehension and manipulation of electronic phenomena, paving the way for future innovations in ultrafast lasers.
dc.description.provenanceSubmitted by Mutluhan Gürel (mutluhan.gurel@bilkent.edu.tr) on 2025-02-21T13:16:43Z No. of bitstreams: 1 Passive_harmonic_mode-locking_in_Tm–Ho_doped_fiber_laser_with_MoS2–ZnO_saturable_absorber_deposited_on_the_arc-shaped_fiber.pdf: 7485753 bytes, checksum: da474deea64f6b8efa97a483489bc749 (MD5)en
dc.description.provenanceMade available in DSpace on 2025-02-21T13:16:43Z (GMT). No. of bitstreams: 1 Passive_harmonic_mode-locking_in_Tm–Ho_doped_fiber_laser_with_MoS2–ZnO_saturable_absorber_deposited_on_the_arc-shaped_fiber.pdf: 7485753 bytes, checksum: da474deea64f6b8efa97a483489bc749 (MD5) Previous issue date: 2024-07-10en
dc.embargo.release2026-07-10
dc.identifier.doi10.1016/j.optmat.2024.115797
dc.identifier.issn0925-3467
dc.identifier.issn1873-1252
dc.identifier.urihttps://hdl.handle.net/11693/116580
dc.language.isoEnglish
dc.publisherElsevier BV * North-Holland
dc.relation.isversionofhttps://doi.org/10.1016/j.optmat.2024.115797
dc.rightsCC BY-NC-ND 4.0 (Attribution-NonCommercial-NoDerivatives 4.0 International Deed)
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/
dc.source.titleOptical Materials
dc.subjectHarmonic mode-locking
dc.subjectTm-Ho doped fiber laser
dc.subjectMoS2-ZnO composite
dc.subjectUltrafast-laser
dc.titlePassive harmonic mode-locking in Tm–Ho doped fiber laser with MoS2–ZnO saturable absorber deposited on the arc-shaped fiber
dc.typeArticle

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