Integration of β-NaYF4 Upconversion Nanoparticles into Polymers for Polymer Optical Fiber Applications
- Авторлар: Neumann L.1, Jakobs F.1, Spelthann S.2, Zaremba D.1, Radunz S.3, Resch-Genger U.3, Evert R.1, Kielhorn J.1, Kowalsky W.1, Johannes H.1
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Мекемелер:
- Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
- Leibniz Universität Hannover, Institut für Quantenoptik
- Bundesanstalt für Materialforschung und–prüfung
- Шығарылым: Том 125, № 5 (2018)
- Беттер: 711-715
- Бөлім: Nanophotonics
- URL: https://ogarev-online.ru/0030-400X/article/view/165848
- DOI: https://doi.org/10.1134/S0030400X18110206
- ID: 165848
Дәйексөз келтіру
Аннотация
Producing active polymer optical fibers (POFs) is a key step towards new applications such as fluorescent fiber solar concentrators (FFSCs), sensors, contactless coupling devices, or fiber integrated light sources and lasers. Therefore, integration of fluorescent nanoparticles into the polymer matrix is necessary and becomes accessible via in situ polymerization. For optical applications, the polymer has to fulfill various requirements such as chemical and physical stability, optical transparency in the application-relevant spectral region as well as a good synthetic accessibility. A common material for these is poly(methyl methacrylate) (PMMA). The β-phase NaYF4:Yb3+,Er3+ upconversion nanoparticles (UCNP) were synthesized from the rare earth salts via thermal decomposition method in high-boiling point solvent 1-octadecene and capping agent oleic acid. Current results show hazy samples of the polymer with integrated nanoparticles made from monomer solution of methyl methacrylate. However, further optical tuning such as increasing the transparency of the bulk samples by changing the monomer solution to non-polar n-butyl methacrylate (nButMA) or cyclohexyl methacrylate (CHMA) or further optimization of the UCNP shell could lead to more suitable polymer bulk samples.
Авторлар туралы
L. Neumann
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
F. Jakobs
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
S. Spelthann
Leibniz Universität Hannover, Institut für Quantenoptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Hannover, 30167
D. Zaremba
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
S. Radunz
Bundesanstalt für Materialforschung und–prüfung
Email: h2.johannes@ihf.tu-bs.de
Германия, Berlin, 12489
U. Resch-Genger
Bundesanstalt für Materialforschung und–prüfung
Email: h2.johannes@ihf.tu-bs.de
Германия, Berlin, 12489
R. Evert
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
J. Kielhorn
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
W. Kowalsky
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
H.-H. Johannes
Technische Universität Braunschweig, Institut für Hochfrequenztechnik, Labor für Elektrooptik
Хат алмасуға жауапты Автор.
Email: h2.johannes@ihf.tu-bs.de
Германия, Braunschweig, 38106
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