2004
DOI: 10.1016/j.jcrysgro.2003.08.014
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Anomalous temperature dependence of photoluminescence from stoichiometric GD2O3−x film

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Cited by 7 publications
(4 citation statements)
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“…30 eV higher. The former displayed the characteristic shape of a spin−orbit doublet, and their BEs [BE(Gd 4d 5/2 ) = 142.1 eV; BE(Gd 4d 3/2 ) = 147.5 eV] and spacing (Δ = 5.4 eV) were in agreement with some previous works on Gd 2 O 3 , ,, despite the fact that higher BE values for Gd(III) oxide have also been reported. ,,, The satellite peak at BE = 170.3 eV was suggested to arise from exchange interactions …”
Section: Resultssupporting
confidence: 88%
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“…30 eV higher. The former displayed the characteristic shape of a spin−orbit doublet, and their BEs [BE(Gd 4d 5/2 ) = 142.1 eV; BE(Gd 4d 3/2 ) = 147.5 eV] and spacing (Δ = 5.4 eV) were in agreement with some previous works on Gd 2 O 3 , ,, despite the fact that higher BE values for Gd(III) oxide have also been reported. ,,, The satellite peak at BE = 170.3 eV was suggested to arise from exchange interactions …”
Section: Resultssupporting
confidence: 88%
“…In fact, for both Gd 2 O 3 and Dy 2 O 3 samples, the O1s band shape was characterized by two main components, highlighted in Figure for the sake of clarity. The most intense contribution, centered at BE = 531.7 eV, was attributed to the presence of −OH groups and carbonates/bicarbonates, due to the high reactivity of lanthanides toward CO 2 and H 2 O arising from atmospheric exposure. ,,,,, The presence of carbonate species was indeed confirmed by a high BE shoulder centered at 288.4 eV in the C1s peak. ,, Appreciable amounts of hydroxide and carbonate functionalities have indeed been previously observed for both Gd 2 O 3 and Dy 2 O 3 thin films deposited by different methods (MOCVD, e-beam evaporation). ,,,, The minor O 1s component at BE = 529.1 eV was related to oxygen in Gd(Dy) 2 O 3 , despite the fact that the pertaining literature is rather ambiguous on lattice oxygen BEs. ,,,,, …”
Section: Resultsmentioning
confidence: 55%
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“…In general, the PL intensity decreases with increasing temperature due to a reduction of excitonic transitions with temperature. The characteristic exhibited by the integrated intensity of the PL peak-a maximum at some measurement temperatures-has also appeared in other materials, such as porous silicon [16] , a-C:H film [17] , silicon nanocrystals in SiO 2 [18] and stoichiometric Gd 2 O 3−x film [19] . In this article, the integrated intensity of the peaks increases at first, reaches its maximum at about 50 K, and finally starts to diminish gradually.…”
Section: -2mentioning
confidence: 80%