English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

Resonance Raman (RR) peaks of and stretching modes and their higher harmonicshave been observed superimposed on photoluminescence (PL) spectrum of thinfilms. Commercial fluorine doped thin films deposited by sputtering on glassand thin films deposited on Si by laser ablation have been studied. Thedispersions of CO and OH stretching RR modes are ~ 600 cm-1/eV and 800 cm-1respectively. The dispersion of the third harmonic of CO stretching mode is ~2000 cm-1/eV. Similar dispersion of RR peak of stretching modes and higherharmonics superimposed on PL spectra has been observed in Mo1-xFexO2 thin filmsand SiO2 bulk glass. Large dispersion of RR peaks seems to be a common propertyof oxides with impurities of and .

Dispersion of Resonant Raman Peaks of CO and OH in SnO2, Mo1-x FexO2 Thin Films and SiO2 bulk glass