2011
DOI: 10.1016/j.jallcom.2011.08.060
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Electronic structure and linear optical property of BaSi2N2O2 crystal

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Cited by 7 publications
(7 citation statements)
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“…Based on the experimental results, we can propose an energy level scheme for the afterglow emission in BaSi 2 O 2 N 2 :Eu 2+ . The band gap of BaSi 2 O 2 N 2 :Eu 2+ is 5.16 eV . The emission energies (2.5 eV) can be obtained from the elementary photoluminescence studies, and the trap energies (0.46 and 0.48 eV) are acquired from TL glow curves as described above.…”
Section: Resultsmentioning
confidence: 99%
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“…Based on the experimental results, we can propose an energy level scheme for the afterglow emission in BaSi 2 O 2 N 2 :Eu 2+ . The band gap of BaSi 2 O 2 N 2 :Eu 2+ is 5.16 eV . The emission energies (2.5 eV) can be obtained from the elementary photoluminescence studies, and the trap energies (0.46 and 0.48 eV) are acquired from TL glow curves as described above.…”
Section: Resultsmentioning
confidence: 99%
“…The band gap of BaSi 2 O 2 N 2 :Eu 2+ is 5.16 eV. 28 The emission energies (2.5 eV) can be obtained from the elementary photoluminescence studies, and the trap energies (0.46 and 0.48 eV) are acquired from TL glow curves as described above. In the case of BaSi 2 O 2 N 2 :Eu 2+ , trap is most efficient using UV radiation (k < 325 nm) while it can also be filled upon excitation with near-UV to blue light (360 nm < k < 500 nm), when exciting into the higher 5d excited states (H-5d) and the lower 5d excited states (L-5d), respectively.…”
Section: Resultsmentioning
confidence: 99%
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“…Furthermore, the observed narrow-band signature in SrMg 3 SiN 4 :Eu 2+ (fwhm of ∼43 nm) was also ascribed to the lone site occupied by the Eu emitter. , It is worth noting that the experimentally observed narrow-band emission is usually associated with a more symmetric coordination environment around the dopant, as seen in SrLiAl 3 N 4 , SrMg 3 SiN 4 , and BaSi 2 N 2 O 2 lattices with the cuboidal coordination. These symmetric coordination features can be identified by comparing the density of state of the nonequivalent nitrogen sites. ,, Conversely, nonequivalent substitution sites featuring an asymmetric coordination polyhedron are likely to generate broad-band emissions. The observation of two nonequivalent Y sites with different electronic structures in Y 3 Si 5 N 9 O phosphor is in accordance with the broadband emission recorded for the phosphors upon Ce 3+ doping .…”
Section: Design Criteria Of Lanthanide-activated Phosphorsmentioning
confidence: 99%
“…As a result of the larger chemical differences of the respective sites, the emission maxima and Stokes shifts are more distinct and thus lead to a relatively broad composite emission (FWHM ∼ 2,050-2,600 cm −1 ; refs 8,16,17,35). A comparison of the local Eu 2+ coordination geometry of SLA with Eu 2+ in BaSi 2 O 2 N 2 :Eu 2+ , a narrow-band green emitter (490 nm peak emission, FWHM ∼ 1,250 cm −1 ) with a surprisingly similar cuboidal coordination [36][37][38][39][40][41] , suggests that such a structural motif results in a small Stokes shift and thus in a narrow emission bandwidth, most likely due to hindered structure relaxation around the activator in its excited state 42 . Larger Stokes shifts and thus broader emission bands observed for Eu 2+ phosphors have been commonly associated with a more asymmetric dopantsite geometry 43 .…”
mentioning
confidence: 99%