Energy transfer rates between Nd(II1) and Yb(II1) in glasses of the basic composition 36 PbFz:24 ZnFz:35 CaFs:2 AlF3:3 YF3:4 LaFs were calculated from donor decay curves, and applied for construction of acceptor luminescence curves. The transfer rates are time dependent and the energy loss by Nd(II1
Concentration dependence of energy transfer between chromium (III) and neodymium (III) in lithium-lanthanum-phosphate glasses
β Scribed by R. Reisfeld; A. Kisilev
- Publisher
- Elsevier Science
- Year
- 1985
- Tongue
- English
- Weight
- 499 KB
- Volume
- 115
- Category
- Article
- ISSN
- 0009-2614
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β¦ Synopsis
Energy-transfer efficiencies between C?+ and Nd3+ various concentrations of Cr3+ and Nd'+. were measured in lithium-lanthanum-phosphate glasses doped by The transfer efficiencies obtained by decrease of donor lifetimes revealed different bekvior from those calculated directly from the increase of Nd3+ Iuminescence. Optimum conditions are determined for lumineseenee devices based on these materials. 1. Intmduction Lithium-lanthanum-phosphate glasses doped by Nd3+ were reported to have reasonable cross section for laser emission [l] _ Later it was suggested that Nd laser can be pumped via Cr3+ in Nd(Al,Cr)3(PO& crystals [Z] and several silicate glasses [3]. It was also shown that efficient energy transfer takes place between Cr3+ and Nd3+m LLJ? glass [4] _ However, the lifetime of Cr3* from which the transfer rates can be determined was not measured because ofthe low intensity ofCr3+ lmnlnescence. It was also indicated that in LLP glass with high Nd concentration the interaction between Cr3+ and Nd3* is more effective than the non-radiative losses in Cr3+. It was also realized that high Nd concentrations are accompanied by back energy transfer from Nd3+ to Cr3+ [5]. Wirig et al. [6] have observed cw laslng in LLP glasses doped by Cr3* and Nd3+ and cormluded that the presence of Cr3+'does not lower significantly the slope efficiency of Nd3+ as compared to Nd3+ only doped glasses. These authors concluded that presence of C!r3* can extend-the pumping range of the lasers. In order to evaluate the advantages and disadvantages of co-doping Nd3* with Cr3* for glass lasers and ' EnriqueBerman Professor of Solar Energy.
π SIMILAR VOLUMES
Energy transfer from C?' to Nd3+ in mullite glasses and glass-ceramics was investigated at 10 and 300 K. Nd3+ and Cr)+ emissions were observed using time-resolved laser spectroscopy Ln the spectral range 640 to 880 nm, and the energy-transfer mechanism was determined. Further information on the dyna
LaF3 In which manganese may replace all the zinc, and neodymium some lanthanum, Is studkd by dynamic and static methods. Both methods arrive at the same results Indicating Iinear dependence of transfer probability on &nor concentration. These results also demonstrate energy storage in the manganese-
Energy-transfer processes between C?+ and Nd3+ multisites in YAG have been studied. 4A2+4T2 zero-phonon and 4A2+2T1 transitions of Cr3+ were observed by high-resolution dye laser excitation spectroscopy.
Energy transfer (ET) between Cc3++ Tm3+ and Ce3++ Tb3+ in p h osphate glass was measured in the temperature range 7-300 K. The efficiency of ET between Ce3' and Tm3+ is independent of temperature, while temperature increasr; is observed in the Ce3+-Tb3+ pair. This is explained by the increase with t