2022
DOI: 10.2139/ssrn.4118370
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The Photoluminescence of a Blue Phosphor Eu2+ Doped Silicate Lutetium Strontium with Triple Sites

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Cited by 1 publication
(2 citation statements)
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“…The FWHM of the luminescent band increases with increasing temperature. Boltzmann distribution is often used to explain this phenomenon 15,45 : FWHM(T)badbreak=8Ln2goodbreak×hνsgoodbreak×prefixcothhν2kT$$\begin{equation}{\mathrm{FWHM}}(T) = \sqrt {8Ln2} \times h\nu \sqrt s \times \sqrt {\coth \frac{{h\nu }}{{2kT}}} \end{equation}$$where k is Boltzmann constant; S is the Huang‐Rhys parameter; hv is the electronic transitions vibrate phonon energy, and it is the same for 5d and 4f of Eu 2+ . As the temperature rises, the interaction of electrons and phonons is dominant.…”
Section: Resultsmentioning
confidence: 99%
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“…The FWHM of the luminescent band increases with increasing temperature. Boltzmann distribution is often used to explain this phenomenon 15,45 : FWHM(T)badbreak=8Ln2goodbreak×hνsgoodbreak×prefixcothhν2kT$$\begin{equation}{\mathrm{FWHM}}(T) = \sqrt {8Ln2} \times h\nu \sqrt s \times \sqrt {\coth \frac{{h\nu }}{{2kT}}} \end{equation}$$where k is Boltzmann constant; S is the Huang‐Rhys parameter; hv is the electronic transitions vibrate phonon energy, and it is the same for 5d and 4f of Eu 2+ . As the temperature rises, the interaction of electrons and phonons is dominant.…”
Section: Resultsmentioning
confidence: 99%
“…The FWHM of the luminescent band increases with increasing temperature. Boltzmann distribution is often used to explain this phenomenon 15,45 :…”
Section: Luminescence Application Abilitiesmentioning
confidence: 99%