2009
DOI: 10.1016/j.jlumin.2009.03.009
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The role of hydrogen- and hydroxyl-doping in CsBr:Eu2+

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Cited by 2 publications
(2 citation statements)
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“…To investigate the exciton recombination dynamics of CsBr:Eu 2+ NCs, time‐resolved PL spectra were measured and the results are depicted in Figure d. The PL decay dynamics of CsBr:Eu 2+ NCs were monoexponential with lifetime of 342 ns, differing from the multiexponential characteristics of previously reported CsBr:Eu 2+ crystals, powders, and transparent ceramics . According to a report by Zorenko et al, a 342 ns lifetime corresponds to the radiative 4f 6 5d 1 ‐4f 7 transitions of Eu 2+ ion in Eu 2+ ‐V Cs isolated dipole centers .…”
Section: Resultsmentioning
confidence: 91%
“…To investigate the exciton recombination dynamics of CsBr:Eu 2+ NCs, time‐resolved PL spectra were measured and the results are depicted in Figure d. The PL decay dynamics of CsBr:Eu 2+ NCs were monoexponential with lifetime of 342 ns, differing from the multiexponential characteristics of previously reported CsBr:Eu 2+ crystals, powders, and transparent ceramics . According to a report by Zorenko et al, a 342 ns lifetime corresponds to the radiative 4f 6 5d 1 ‐4f 7 transitions of Eu 2+ ion in Eu 2+ ‐V Cs isolated dipole centers .…”
Section: Resultsmentioning
confidence: 91%
“…The emission spectra of NC-10 possess identical shape and position when excited by 272, 346, and 360 nm UV light, showing an excitation-independent nature (see Figure e). According to previous reports, these emission peaks can be assigned to the 4f 6 5d 1 –4f 7 transition of Eu 2+ in the Eu 2+ -V Cs dipole. , Two excitation peaks correspond to the splitting of 5d orbitals of Eu 2+ into the two components t 2g and e g , which is caused by the influence of the crystal field on the Eu 5d electrons. The peak located at 272 nm is attributed to the 4f 7 –4f 6 5d 1 (t 2g ) transitions, and to the 4f 7 –4f 6 5d 1 (e g ) transitions for the peak at 346 nm .…”
mentioning
confidence: 99%