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Spectroscopic Properties Of Ho3+ Doped And Ho3+/Pr3+ Co-doped Y2O3 Transparent Ceramics

Posted on:2024-09-28Degree:MasterType:Thesis
Country:ChinaCandidate:J Y ZangFull Text:PDF
GTID:2531307052496564Subject:Electronic information
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The 3μm Mid-infrared lasers are widely used in gas detection,laser medicine,materials manufacturing,military,etc,with important application context and great scope for demand,and have become a hot research direction of research and development for national defense and civilians.Holmium ion(Ho3+)doped luminescent materials have received increasing attention because of their potential to achieve infrared luminescence near 2.85μm.However,the luminescence of Ho3+-doped luminescent materials near 2.85μm is produced by a radiative transition between the5I65I7 energy levels.However,the energy levels are in a"self-terminating"state in the normal state,with a short lifetime for the upper laser energy level 5I6 and a long lifetime for the lower laser energy level 5I7,resulting in the bottleneck type of population in the upper energy level with little and the lower energy level with a large number.These characteristics make the electrons in the 5I6 energy level relax to the 5I7 energy level mainly by transferring energy to the lattice phonons through the non-radiation transition,with the chance of radiative leap being very small.The key to achieving 2.85μm mid-infrared luminescence is to open the self-closing state between the 5I6 and 5I7 levels to make the non-radiative transition into a radiative transition,which requires low phonon energy of the matrix material.so that the upper energy level 5I6 of the laser gets a longer lifetime,allowing more electrons to gather on it and better particle number inversion between the upper and lower energy levels 5I6 and 5I7 of the laser.The sesquioxide usually has relatively low phonon energy and serves as a potential matrix material for rare earth ions.Among the three half-oxides(Sc2O3、Y2O3 and Lu2O3),Y2O3 has the lowest phonon energy,generally 597 cm-1,while Y2O3 used in this paper has lower phonon energy of 563 cm-1.Therefore,it is of certain significance and value to study the spectral properties of Ho3+in low phonon energy Y2O3.In addition,we select praseodymium ions(Pr3+)that can be coupled with Ho3+levels to reduce the lifetime of the lower laser level 5I7 and promote the inversion of particle numbers at 5I6 and 5I7levels,so as to reduce the pump threshold of the gain material to improve the laser efficiency.Based on the above considerations,the spectral properties of Ho:Y2O3 and Ho/Pr:Y2O3 transparent ceramics with low phonon energy have been systematically studied in this research.The following achievements and progress have been made:1.Cooperate to prepare transparent ceramic samples with different concentrations of Ho:Y2O3 by vacuum sintering and hot isostatic pressing.The maximum phonon energy is only 563 cm-1 by the FTIR test,with lower maximum phonon energy than normal Y2O3 transparent ceramics and lower phonon energy than other common oxide transparent ceramics,which is more conducive to the improvement of the energy level5I6 lifetime on the laser.By the XRD test shows that Ho3+will not change the structure of Y2O3,which ensures the excellent performance of ceramics and the efficient transition emission of Ho3+.2.Our Y2O3 transparent ceramics were found to achieve fluorescence at 2850 nm when doped with Ho3+ions alone at sufficiently low phonon energies for pumping at640 nm instead of 1100 nm.Fluorescence lifetime tests show that the upper energy level of the Ho3+laser has a lifetime of 0.90 ms,which is a significant increase compared to common Ho:YAP crystals(0.39 ms,subsection 3.3.7)due to the low phonon energy,while the lower energy level has little increase in lifetime,suggesting that the 5I6 energy level of Ho3+can gather more electrons,facilitating particle number reversal between the upper and lower energy levels of the laser.This suggests that the 5I6 energy level of Ho3+can concentrate more electrons,which is conducive to particle number reversal between the upper and lower energy levels and achieving~2.85μm laser output.3.According to the Judd-Ofelt(J-O)theory,the research models the spectral parameters of Ho3+transition process in the sample,such as vibrator intensity,J-O parameter,spontaneous radiation transition probability,radiation lifetime,fluorescence branching ratio and so on.The calculated J-O parameters areΩ2=2.38×10-20 cm24=1.92×10-20 cm26=1.04×10-20 cm2.Compared with general matrix materials with a smallerΩ2 and a larger mass factor,it is proved that Ho3+has a higher ionic property in Ho:Y2O3,which makes the inversion of particle number easier to realize,Therefore,it proves that our Ho:Y2O3 transparent ceramic has the possibility of realizing~2.85μm laser output.4.By testing and comparing the spectral properties of Ho3+/Pr3+co-doped Y2O3samples and Ho3+single-doped samples,it is found that the fluorescence of the Ho3+/Pr3+co-doped Y2O3 sample at 2094 nm was very weak compared to the Ho3+single-doped Y2O3 sample and the lifetime of the energy level under the laser decreased significantly from 8.65 ms for the Ho3+single-doped Y2O3 to 0.67 ms for the Ho3+/Pr3+co-doped Y2O3,the lifetime of the upper laser energy level did not change significantly to 0.72 ms,indicating that(1)the energy transfer between Ho3+:5I7→Pr3+:3F2 with a transfer efficiency of 92.26%(Eq.5-1 in the text)was generated between Ho3+and Pr3+;(2)the Ho3+/Pr3+co-doped Y2O3(2)the number of 5I7 energy levels in Ho3+is greatly reduced,and the bottleneck electron distribution between the upper and lower energy levels of the laser is significantly improved or even disappears;(3)the upper energy level lifetime of the laser is slightly longer than the lower energy level lifetime,and the particle number reversal between the upper and lower energy levels is achieved.All this suggests that the doping of rare earth ions Pr3+effectively increases the potential of Ho/Pr:Y2O3 transparent ceramics to achieve~2.85μm mid-infrared laser output.
Keywords/Search Tags:Holmium, Transparent ceramics, Holmium/praseodymium co-doping, Low phonon energy, Judd-Ofelt theory, Spectroscopic properties
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