“…Eu 2 + luminescence is usually due to 4f 6 5d-4f 7 interconfigurational transitions, which lead to a rather broad emission whose spectral position depends strongly on the chemical nature of the crystal. The maximum of the Eu 2 + 4f 6 5d-4f 7 [20,21]. In all the cases the emission bands are broad and the corresponding Stokes shifts are very large, ranging from $ 7500 cm À 1 for BaSiO 3 :Eu 2 + , Sr 2 LiSiO 4 F:Eu 2 + and up to 12,000 cm À 1 for Ba 2 Mg(BO 3 ) 2 :Eu 2 + .…”
Section: Discussionmentioning
confidence: 87%
“…Despite the emission maximum of Li 2 SrSiO 4 :Eu 2 + is in between those of Sr 2 LiSiO 4 F:Eu 2 + (535 nm), BaSiO 3 :Eu 2 + (550 nm) and Ba 2 LiB 5 O 10 :Eu 2 + (620 nm), this luminescence shows the characteristics of the Eu 2 + 4f 6 5d-4f 7 ( 8 S 7/2 ) emission. The red shift with the respect to the lowest excitation band is relatively small (3400 cm À 1 ), the decay time (t¼1.07 ms) is typical for 4f 6 5d-4f 7 transitions of Eu 2 + in inorganic compounds [21].…”
Section: Discussionmentioning
confidence: 93%
“…In all the cases the emission bands are broad and the corresponding Stokes shifts are very large, ranging from $ 7500 cm À 1 for BaSiO 3 :Eu 2 + , Sr 2 LiSiO 4 F:Eu 2 + and up to 12,000 cm À 1 for Ba 2 Mg(BO 3 ) 2 :Eu 2 + . Poort et al [20,21] and later Dorenbos [22] pointed out that these long-wavelength emissions are possibly not related to the 4f 6 5d-4f 7 transitions of Eu 2 + ions, but may be due to an absolutely different process, namely radiative decay of an impurity trapped exciton. This interpretation implies that excitation into the Eu 2 + 4f 7 -4f 6 5d bands leads to ionization of Eu 2 + ions and the formation of an exciton-like state, which consists of a bound electron hole pair with the hole localized on the Eu 3 + ion and the electron delocalized on the nearest-neighbor cations.…”
a b s t r a c tThe luminescent properties of Eu 2 + and Ce 3 + ions in Li 2 SrSiO 4 have been studied upon excitation in the 2-20 eV region. Based on the results of luminescent measurements, values of the crystal field splitting and the centroid shift of the Ce 3 + 5d configuration in Li 2 SrSiO 4 were found and compared with those of Ce 3 + ions in some other inorganic compounds. The Eu 2 + ions in Li 2 SrSiO 4 exhibit a broad band emission with a maximum at 576 nm, which is due to the 4f 6 5d-4f 7 transition. It was shown that the long-wavelength position of the Eu 2 + emission in Li 2 SrSiO 4 is caused by the large crystal-field splitting of the Eu 2 + 4f 6 5d configuration and relatively high degree of covalency of the Eu-O bond. The stabilization of Eu 2 + ions in Li 2 SrSiO 4 during the synthesis process requires a strong reducing agent. Two phenomenological approaches to explain the low stability of Eu 2 + in Li 2 SrSiO 4 are also discussed.
“…Eu 2 + luminescence is usually due to 4f 6 5d-4f 7 interconfigurational transitions, which lead to a rather broad emission whose spectral position depends strongly on the chemical nature of the crystal. The maximum of the Eu 2 + 4f 6 5d-4f 7 [20,21]. In all the cases the emission bands are broad and the corresponding Stokes shifts are very large, ranging from $ 7500 cm À 1 for BaSiO 3 :Eu 2 + , Sr 2 LiSiO 4 F:Eu 2 + and up to 12,000 cm À 1 for Ba 2 Mg(BO 3 ) 2 :Eu 2 + .…”
Section: Discussionmentioning
confidence: 87%
“…Despite the emission maximum of Li 2 SrSiO 4 :Eu 2 + is in between those of Sr 2 LiSiO 4 F:Eu 2 + (535 nm), BaSiO 3 :Eu 2 + (550 nm) and Ba 2 LiB 5 O 10 :Eu 2 + (620 nm), this luminescence shows the characteristics of the Eu 2 + 4f 6 5d-4f 7 ( 8 S 7/2 ) emission. The red shift with the respect to the lowest excitation band is relatively small (3400 cm À 1 ), the decay time (t¼1.07 ms) is typical for 4f 6 5d-4f 7 transitions of Eu 2 + in inorganic compounds [21].…”
Section: Discussionmentioning
confidence: 93%
“…In all the cases the emission bands are broad and the corresponding Stokes shifts are very large, ranging from $ 7500 cm À 1 for BaSiO 3 :Eu 2 + , Sr 2 LiSiO 4 F:Eu 2 + and up to 12,000 cm À 1 for Ba 2 Mg(BO 3 ) 2 :Eu 2 + . Poort et al [20,21] and later Dorenbos [22] pointed out that these long-wavelength emissions are possibly not related to the 4f 6 5d-4f 7 transitions of Eu 2 + ions, but may be due to an absolutely different process, namely radiative decay of an impurity trapped exciton. This interpretation implies that excitation into the Eu 2 + 4f 7 -4f 6 5d bands leads to ionization of Eu 2 + ions and the formation of an exciton-like state, which consists of a bound electron hole pair with the hole localized on the Eu 3 + ion and the electron delocalized on the nearest-neighbor cations.…”
a b s t r a c tThe luminescent properties of Eu 2 + and Ce 3 + ions in Li 2 SrSiO 4 have been studied upon excitation in the 2-20 eV region. Based on the results of luminescent measurements, values of the crystal field splitting and the centroid shift of the Ce 3 + 5d configuration in Li 2 SrSiO 4 were found and compared with those of Ce 3 + ions in some other inorganic compounds. The Eu 2 + ions in Li 2 SrSiO 4 exhibit a broad band emission with a maximum at 576 nm, which is due to the 4f 6 5d-4f 7 transition. It was shown that the long-wavelength position of the Eu 2 + emission in Li 2 SrSiO 4 is caused by the large crystal-field splitting of the Eu 2 + 4f 6 5d configuration and relatively high degree of covalency of the Eu-O bond. The stabilization of Eu 2 + ions in Li 2 SrSiO 4 during the synthesis process requires a strong reducing agent. Two phenomenological approaches to explain the low stability of Eu 2 + in Li 2 SrSiO 4 are also discussed.
“…An evident increase in luminescence decay time with an increase in monitored luminescence wavelength supports this conclusion. 37 In addition, the decay curves of β-SiAlON:Eu (529) and β-SiAlON:Eu (540) were also measured at RT ( Figure S10 and Table S3). The obtained lifetimes show the same trend as that measured at 10 K. The decay time of the sharp lines as well as broad band for both samples are in the 0.6-1.2 μs range, which means that the observed luminescence is related to parity-allowed transitions from the excitated states of electronic configuration 4f electronic configuration create the seven electronic levels: 7 F0-7 F6, analogous to the Eu 3+ which does not interact with the lattice ions since they are screened by 5s 2 5p 6 electrons.…”
Narrow-band green-emitting phosphor β-SiAlON:Eu has been widely used in advanced wide-gamut backlighting devices. However, the origins for unusual sharp lines in photoluminescence emission at room temperature and tunable narrow-bandemission tailored by reducing Al-O in β-SiAlON:Eu are still unclear. Here, the presence of sharp-line fine structure in the emission spectra of β-SiAlON:Eu is mainly due to purely electronic transitions (zero phonon lines) and their vibronic repetitions resulted from the multi-microenvironment around Eu 2+ ions that has been revealed by relative emission intensity of sharp line depends on excitation wavelength and monotonously increasing decay time. The specific features of the Eu 2+ occupying interstitial sites indicate that the effect of crystal field strength can be neglected. Therefore the enhanced rigidity and higher ordering structure of β-SiAlON:Eu with decreasing the substitution of Si-N by Al-O become the main factors in decreasing electron-lattice coupling and reducing inhomogeneous broadening, favouring the blue-shift and narrow of the emission band, the enhanced thermal stability, as well as the charge state of Eu 2+ . Our results provide new insights for explaining the reason for narrow-band-emission in β-SiAlON:Eu, which will deliver an impetus for the exploration of phosphors with narrow band and ordering structure.
“…48 The l 3 dependence of the decay time yields a value of about 0.8 ms for the 445 nm emission. The shorter decay time observed, 0.4 ms, indicates that energy transfer takes place, shortening the decay time.…”
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