2014
DOI: 10.1016/j.jlumin.2013.11.041
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Pressure evolution of luminescence in Sr Ba1−(NbO2)3:Pr3+ (x=1/2 and 1/3)

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Cited by 11 publications
(15 citation statements)
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“…An alternative way to induce irreversible modifications in the local field surrounding the RE 3+ ions is by densification of the glass structure under high pressure, promoting irreversible changes in the interatomic distances and bonding angles. The effect of high pressure on the luminescence properties of vitreous and crystalline systems doped with RE 3+ ions has been investigated in situ using the diamond anvil cell (DAC). It is worth noting that the effect of high pressure on the structure of the GeO 2 glass was, also, extensively investigated. , In this context, the objective of this work is to study the structural and spectroscopic properties of the GeO 2 –PbO glass doped with Sm 3+ ions before and after densification at 7.7 GPa in a large volume high pressure apparatus.…”
Section: Introductionmentioning
confidence: 99%
“…An alternative way to induce irreversible modifications in the local field surrounding the RE 3+ ions is by densification of the glass structure under high pressure, promoting irreversible changes in the interatomic distances and bonding angles. The effect of high pressure on the luminescence properties of vitreous and crystalline systems doped with RE 3+ ions has been investigated in situ using the diamond anvil cell (DAC). It is worth noting that the effect of high pressure on the structure of the GeO 2 glass was, also, extensively investigated. , In this context, the objective of this work is to study the structural and spectroscopic properties of the GeO 2 –PbO glass doped with Sm 3+ ions before and after densification at 7.7 GPa in a large volume high pressure apparatus.…”
Section: Introductionmentioning
confidence: 99%
“…This method has been used to estimate the location of the ground states of Tb 3+ and Pr 3+ with respect to conduction band in many materials. [14][15][16][17][18][19][20][21][22][23][24] We have chosen Y 2 O 2 S doped with Eu 3+ and Y 2 O 2 S doped with Tb 3+ to demonstrate how high-pressure spectroscopy can be used to determine the energetic structures of dielectric hosts doped with Ln 3+ and Ln 2+ .…”
Section: Introductionmentioning
confidence: 99%
“…[11][12][13][14][15] In the case of Pr 3+ or Tb 3+ doped samples, the emission dynamics are influenced by the formation of an intermediate charge transfer state (or the impurity trapped exciton state) that interferes with the 4f excited states of the dopants by creating new relaxation channels that lead to the quenching of otherwise emitting levels. [14][15][16][17][18][19][20][21][22][23][24][25][26][27][28] The ionization transition creates the Ln 4+ ion (Ln = Tb, Pr) and an electron in the conduction band (e cb ). After ionization, the Coulomb attraction between Ln 4+ and e cb allows the system to exist in the bound state, which defines an impurity trapped exciton (ITE) state (also referred to the praseodymium/terbium trapped exciton (PTE/TTE) state) in the past literature.…”
Section: Introductionmentioning
confidence: 99%