2016
DOI: 10.1016/j.jlumin.2016.08.034
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Fano׳s antiresonance and crystal-field study of Cr3+ in metaphosphate glasses

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Cited by 21 publications
(8 citation statements)
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“…The strongly oscillating conductance spectra are originated from the interference between the reflected wave from Fano defects and that propagating along the nanoribbon. Such Fano resonant and antiresonant spectra have been observed in optical, [ 30 ] plasmonic, [ 31 ] and transport [ 32 ] experiments.…”
Section: Discussionmentioning
confidence: 81%
“…The strongly oscillating conductance spectra are originated from the interference between the reflected wave from Fano defects and that propagating along the nanoribbon. Such Fano resonant and antiresonant spectra have been observed in optical, [ 30 ] plasmonic, [ 31 ] and transport [ 32 ] experiments.…”
Section: Discussionmentioning
confidence: 81%
“…Each 4 A 2 → 4 T 2 excitation band has a dip structure at approximately 700 nm owing to the Fano antiresonance phenomenon. 41) Although the peak wavelengths of excitation bands did not change with Cr concentration, the FWHMs tended to increase with increasing Cr concentration. Similar trends in the dependence of the shifting PL peak and broadening of the PLE bandwidth on the luminescent center concentration have often been reported for phosphor materials with multiple luminescent sites.…”
Section: Pl Propertiesmentioning
confidence: 89%
“…The 4 A 2 → 4 T 2 excitation band has the dip structure at 688 nm caused by Fano antiresonance due to the interaction between intra-t 2 3 levels ( 2 E and 2 T 1 ) and t e 2 level ( 4 T 2 ). 42) The Cr 4+ and Cr 6+ absorption bands were not recognized in the PLE spectra. Thus, the energy transfer from these chromium ions to Cr 3+ does not occur.…”
Section: Optical and Pl Propertiesmentioning
confidence: 97%