TY - JOUR
T1 - The effects of energy transfer on the Er 3+ 1.54 μm luminescence in nanostructured Y 2O 3 thin films with heterogeneously distributed Yb 3+ and Er 3+ codopants
AU - Hoang, J.
AU - Schwartz, Robert N.
AU - Wang, Kang L.
AU - Chang, J. P.
N1 - Funding Information:
The authors acknowledge the financial support from National Science Foundation under NSF CBET-0522534. This work was carried out in part at the Stanford Synchrotron Radiation Laboratory, a national user facility operated by Stanford University on behalf of the U.S. Department of Energy, Office of Basic Energy Sciences. J. Hoang acknowledges the Dissertation Year Fellowship support from UCLA Graduate Division. J. Hoang also acknowledges Calvin Pham and Ryan Hoekstra for their contribution to the experiments and PL measurements, respectively.
PY - 2012/9/15
Y1 - 2012/9/15
N2 - We report the effects of heterogeneous Yb 3+ and Er 3+ codoping in Y 2O 3 thin films on the 1535 nm luminescence. Yb 3+:Er 3+:Y 2O 3 thin films were deposited using sequential radical enhanced atomic layer deposition. The Yb 3+ energy transfer was investigated for indirect and direct excitation of the Yb 2+F 7/2 state using 488 nm and 976 nm sources, respectively, and the trends were described in terms of Forster and Dexters resonant energy transfer theory and a macroscopic rate equation formalism. The addition of 11 at. Yb resulted in an increase in the effective Er 3+ photoluminescence (PL) yield at 1535 nm by a factor of 14 and 42 under 488 nm and 976 nm excitations, respectively. As the Er 2O 3 local thickness was increased to greater than 1.1 Å, PL quenching occurred due to strong local Er 3+ ↔ Er 3+ excitation migration leading to impurity quenching centers. In contrast, an increase in the local Yb 2O 3 thickness generally resulted in an increase in the effective Er 3+ PL yield, except when the Er 2O 3 and Yb 2O 3 layers were separated by more than 2.3 Å or were adjacent, where weak Yb 3+ ↔Er 3+ coupling or strong Yb 3+ ↔ Yb 3+ interlayer migration occurred, respectively. Finally, it is suggested that enhanced luminescence at steady state was observed under 488 nm excitation as a result of Er 3+ → Yb 3+ energy back transfer coupled with strong Yb 3+ Yb 3+ energy migration.
AB - We report the effects of heterogeneous Yb 3+ and Er 3+ codoping in Y 2O 3 thin films on the 1535 nm luminescence. Yb 3+:Er 3+:Y 2O 3 thin films were deposited using sequential radical enhanced atomic layer deposition. The Yb 3+ energy transfer was investigated for indirect and direct excitation of the Yb 2+F 7/2 state using 488 nm and 976 nm sources, respectively, and the trends were described in terms of Forster and Dexters resonant energy transfer theory and a macroscopic rate equation formalism. The addition of 11 at. Yb resulted in an increase in the effective Er 3+ photoluminescence (PL) yield at 1535 nm by a factor of 14 and 42 under 488 nm and 976 nm excitations, respectively. As the Er 2O 3 local thickness was increased to greater than 1.1 Å, PL quenching occurred due to strong local Er 3+ ↔ Er 3+ excitation migration leading to impurity quenching centers. In contrast, an increase in the local Yb 2O 3 thickness generally resulted in an increase in the effective Er 3+ PL yield, except when the Er 2O 3 and Yb 2O 3 layers were separated by more than 2.3 Å or were adjacent, where weak Yb 3+ ↔Er 3+ coupling or strong Yb 3+ ↔ Yb 3+ interlayer migration occurred, respectively. Finally, it is suggested that enhanced luminescence at steady state was observed under 488 nm excitation as a result of Er 3+ → Yb 3+ energy back transfer coupled with strong Yb 3+ Yb 3+ energy migration.
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U2 - 10.1063/1.4752754
DO - 10.1063/1.4752754
M3 - Article
AN - SCOPUS:84867039034
VL - 112
JO - Journal of Applied Physics
JF - Journal of Applied Physics
SN - 0021-8979
IS - 6
M1 - 063117
ER -