In this work we report infrared to visible upconversion luminescence in the low phonon-energy host material KPb 2 Cl 5 doped with Er 3ϩ ions under 4 I 9/2 excitation. The upconversion mechanisms are investigated by using steady-state and time-resolved laser spectroscopy. When the excitation wavelength is resonant with the 4 I 9/2 level (Ϸ800 nm), the upconverted emission originates from the levels 2 H 9/2 and 4 S 3/2 . These upconverted emissions occur via energy-transfer upconversion processes. However, under nonresonant excitation at lower energies than 4 I 9/2 , the main emission results from the level 2 H 9/2 . This latter upconverted emission can be attributed to excited-state absorption of the pump radiation. The proposed upconversion mechanisms responsible for the different emissions from the levels 2 H 9/2 and 4 S 3/2 are supported by both the time evolution of the upconversion luminescence after pulsed infrared excitation and the upconversion luminescence excitation spectra. Rate equation analysis has been used to identify and characterize the energy-transfer processes responsible for the observed fluorescence behavior.
We report internal laser cooling in Yb(3+) -doped KPb(2)Cl(5) . From the quantum efficiency values measured in the heating and cooling regions by use of the photothermal deflection technique, we have obtained a room-temperature cooling efficiency of 0.2% in a sample doped with ~5x10(19)ions/cm(3) . Excitation spectra obtained under high irradiation fluences show an excess of fluorescence with regard to those obtained at low fluences, which agrees with the prediction of a model based on photon-ion-phonon interaction.
In this work we report infrared-to-visible upconversion luminescence in the low-phonon-energy host material KPb 2 Cl 5 codoped with Pr 3ϩ and Yb 3ϩ ions. An orange luminescence from the 1 D 2 level, and less intense blue, green, and red emissions from the 3 P 0,1 levels of Pr 3ϩ have been observed under resonant excitation in the 1 G 4 level of Pr 3ϩ . As regards to Yb 3ϩ , when the 2 F 5/2 level is resonantly excited, the visible emissions are also present but the blue, green, and red emissions from 3 P 0,1 levels are enhanced if compared with the orange luminescence from level 1 D 2 . On the other hand, excitation at the high-energy wing of the 2 F 5/2 level originates emission only from 3 P 0,1 levels. The upconverted fluorescence from the 1 D 2 and 3 P 0,1 levels occurs by energy transfer upconversion and/or excited-state absorption processes depending on the excitation wavelength. The possible mechanisms which lead these processes are discussed.
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