| 000 | 00000nam 2200000zi 4500 |
| 001 | 9.879508 |
| 003 | CaOODSP |
| 005 | 20240221113057 |
| 006 | m o d f |
| 007 | cr |n||||||||| |
| 008 | 190920t20182018quca ob f000 0 eng d |
| 040 | |aCaOODSP|beng|erda|cCaOODSP |
| 043 | |an-cn--- |
| 086 | 1 |aD68-10/074-2018E-PDF |
| 100 | 1 |aThéberge, Francis, |eauthor. |
| 245 | 10|aInfrared supercontinuum generated in concatenated InF3 and As2Se3 fibers / |cFrancis Théberge [and eight others]. |
| 264 | 1|a[Quebec (Quebec)] : |bDefence Research and Development Canada = Recherche et développement pour la défense Canada, |c2018. |
| 264 | 4|c©2018 |
| 300 | |a1 online resource (13 unnumbered pages) : |bfigures. |
| 336 | |atext|btxt|2rdacontent |
| 337 | |acomputer|bc|2rdamedia |
| 338 | |aonline resource|bcr|2rdacarrier |
| 490 | 1 |aExternal literature (P) ; |vDRDC-RDDC-2018-P074 |
| 500 | |a"Can unclassified." |
| 500 | |a"June 2018." |
| 500 | |a"Optics Express 13952, Vol. 26, No. 11. Date of publication from Ext publisher: May 2018." |
| 504 | |aIncludes bibliographical references. |
| 520 | |a"We report on infrared supercontinuum (SC) generation through subsequent nonlinear propagation in concatenated step-index fluoride and As2Se3 fiber. These fibers were pumped by an all-fiber laser source based on an erbium amplifier followed by a thuliumpower amplifier. ZBLAN and InF3 fibers were compared for the concatenated scheme. Thebroadest SC produced was achieved by optimizing the length of the InF3 fiber"--Abstract. |
| 692 | 07|2gccst|aScientific research |
| 710 | 1 |aDefence R&D Canada. |bValcartier Research Centre. |
| 830 | #0|aExternal literature (P) (Defence R&D Canada)|vDRDC-RDDC-2018-P074.|w(CaOODSP)9.854437 |
| 856 | 40|qPDF|s889 KB|uhttps://publications.gc.ca/collections/collection_2019/rddc-drdc/D68-10-074-2018-eng.pdf |