Show simple item record

dc.contributor.authorKılınç, Muharrem
dc.contributor.authorDemirbaş, Ümit
dc.contributor.authorGonzalez-diaz, Juan B.
dc.contributor.authorThesinga, Jelto
dc.contributor.authorKellert, Martin
dc.contributor.authorPalmer, Guido
dc.contributor.authorKaertne, Franz X.
dc.contributor.authorPergament, Mikhail
dc.date.accessioned2024-04-15T08:24:38Z
dc.date.available2024-04-15T08:24:38Z
dc.date.issued2023
dc.identifier.citationKılınç, M., Demirbaş, Ü., Gonzalez-diaz, J. B., Thesinga, J., Kellert, M., Palmer, G., Kaertne, F. X. & Pergament, M. (2023). Thermal and population lensing of Yb:YLF at cryogenic temperature. Optical Materials Express, 13(11), 3200-3216.en_US
dc.identifier.issn2159-3930
dc.identifier.urihttp://hdl.handle.net/20.500.12566/2076
dc.description.abstractWe present what is, to our knowledge, the first detailed study of thermal and population lensing in cryogenically cooled Yb:YLF. Using a rod-shaped a-cut Yb:YLF crystal, the thermal lens strength is measured as a function of absorbed pump power for both E//a and E//c polarizations for pump power levels up to 600 W. Our experiments revealed that the thermal lensing behavior in Yb:YLF is quite asymmetric. For the E//a polarization, the thermal lens is rather strong and always converging for both horizonal and vertical axes. For the E//c configuration, thermal lensing is rather weak, and its sign could be different in different axis, and furthermore, the sign of thermal lensing is observed to be dependent on the absorbed pump power level. Simulations and detailed experimental measurements show that the observed peculiar behavior is a result of competition between the photo-elastic effect and thermo-optic effect: as their relative strength varies at different pump power levels. We have also measured the contribution of surface bulging into thermal lensing and found it to be relatively small in our crystals with un-doped end caps. Lastly, the population lensing is measured in Yb:YLF for the first time, and it is found to be quite weak as well, and the polarizability difference parameter of Yb:YLF is determined as (3 ± 1.5) x 10−34 m3.en_US
dc.description.sponsorshipNo sponsoren_US
dc.language.isoengen_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.titleThermal and population lensing of Yb:YLF at cryogenic temperatureen_US
dc.typeinfo:eu-repo/semantics/articleen_US
dc.relation.publicationcategoryInternational publicationen_US
dc.identifier.wosWOS:001104626900008
dc.identifier.scopus2-s2.0-85175608833
dc.contributor.orcid0000-0001-8420-8965 [Demirbaş, Ümit]
dc.contributor.abuauthorDemirbaş, Ümit
dc.contributor.yokid20328 [Demirbaş, Ümit]
dc.relation.journalOptical Materials Expressen_US
dc.contributor.ScopusAuthorID8840686700 [Demirbaş, Ümit]
dc.identifier.doi10.1364/OME.503085


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record