2017
DOI: 10.1039/c6ce02611g
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Morphology control of uniform CaMoO4microarchitectures and development of white light emitting phosphors by Ln doping (Ln = Dy3+, Eu3+)

Abstract: CrystEngComm publishes novel findings in the field of crystal engineering, including properties, target crystals and materials, crystal growth, nanocrystals and computational studies. Articles reporting results which could be routinely predicted or result from the application of standard procedures or techniques are unlikely to prove acceptable. For publication in CrystEngComm a paper must report work of high quality and originality. Communications must report chemistry of sufficient importance and impact to j… Show more

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Cited by 39 publications
(23 citation statements)
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“…This result may imply that the Eu 3+ ions are located in the site without inversion symmetry. A similar phenomenon has been observed in many CaMoO 4 :Eu 3+ samples, as reported in the literature [9,28,30]. One possible explanation for this discrepancy is given by considering the polarizability effect of the MoO 4 units on the EuO 8 units [28].…”
Section: Effect Of Hot Water Treatmentsupporting
confidence: 50%
“…This result may imply that the Eu 3+ ions are located in the site without inversion symmetry. A similar phenomenon has been observed in many CaMoO 4 :Eu 3+ samples, as reported in the literature [9,28,30]. One possible explanation for this discrepancy is given by considering the polarizability effect of the MoO 4 units on the EuO 8 units [28].…”
Section: Effect Of Hot Water Treatmentsupporting
confidence: 50%
“…The excellent luminescent properties together with the high chemical and thermal stability of the CaMoO4:Eu 3+ phosphor has attracted a lot of attention in the last decade. Photoluminescence properties of CaMoO4:Eu 3+ have been extensively studied in bulk samples, 5,6,7,8 microparticles 3,9,10,11 and different types of nanoparticles. 12,13,14,15 However, very little attention has been paid to the substitution mechanism and crystal structure of Eu 3+ :CaMoO4 phosphors.…”
Section: Introductionmentioning
confidence: 99%
“…The decay curves obtained for the I(t) = I 01 exp(-t/τ 1 ) + I 02 exp(-t/τ 2 ) (1) where I(t) is the luminescence intensity, t is the time after excitation, and τ i (i = 1, 2) is the decay time of the i-component, with initial intensity I 01 . Such biexponential behavior has been previously observed for this system [35,37] and other lanthanidebased nanophosphors [38] and accounts for the contribution of the Eu 3+ ions located close to the surface of the nanoparticles (short time component) whose luminescence is influenced by OH species or surface defects that act as luminescence quench- [38] The fitting parameters are presented in Table 4, which shows that the short-time component is a minority in all cases and that the lifetime values tend to decrease as the Eu doping level increases. This variation is also manifested by the average lifetime values, <τ>, calculated from Equation (2): (2) where t f represents the time required for the luminescence signal to reach the background.…”
Section: Luminescence Propertiesmentioning
confidence: 71%