Resonant Dispersion Effect on Actively Mode-Locked Nd:Glass Laser

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dc.contributor.authorLu, Wei
dc.contributor.authorYan, Li
dc.contributor.authorMenyuk, Curtis
dc.date.accessioned2025-06-17T14:45:52Z
dc.date.available2025-06-17T14:45:52Z
dc.date.issued2001-05-06
dc.descriptionConference on Lasers and Electro-Optics 2001, Baltimore, Maryland United States, 6–10 May 2001
dc.description.abstractActively mode-locked Nd:glass lasers can potentially generate very short pulses since they have broad lasing bandwidths (~5 nm for Nd:silicate) even in the free-running state. However, the modulator is too weak to mode-lock fully such broad bandwidth without compensation of the group velocity dispersion (GVD).
dc.description.urihttps://opg.optica.org/abstract.cfm?uri=CLEO-2001-CMK6
dc.format.extent2 pages
dc.genreconference papers and proceedings
dc.identifierdoi:10.13016/m2kzs8-fclq
dc.identifier.citationLu, Wei, Li Yan, and Curtis R. Menyuk. "Resonant Dispersion Effect on Actively Mode-Locked Nd:Glass Laser" In Conference on Lasers and Electro-Optics (2001), Paper CMK6, CMK6. Optica Publishing Group, 2001. https://opg.optica.org/abstract.cfm?uri=CLEO-2001-CMK6.
dc.identifier.urihttp://hdl.handle.net/11603/38958
dc.language.isoen_US
dc.publisherOptica
dc.relation.isAvailableAtThe University of Maryland, Baltimore County (UMBC)
dc.relation.ispartofUMBC Faculty Collection
dc.relation.ispartofUMBC Computer Science and Electrical Engineering Department
dc.rightsThis item is likely protected under Title 17 of the U.S. Copyright Law. Unless on a Creative Commons license, for uses protected by Copyright Law, contact the copyright holder or the author.
dc.subjectNumerical simulation
dc.subjectTi:sapphire lasers
dc.subjectUMBC Optical Fiber Communications Laboratory
dc.subjectUMBC High Performance Computing Facility (HPCF)
dc.subjectFemtosecond pulses
dc.subjectDispersion
dc.subjectLasers
dc.subjectPhase modulation
dc.titleResonant Dispersion Effect on Actively Mode-Locked Nd:Glass Laser
dc.typeText
dcterms.creatorhttps://orcid.org/0000-0003-0269-8433

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