Kinetics of Cr3+ to Cr4+ ion valence transformations and intra-lattice cation exchange of Cr4+ in Cr,Ca:YAG ceramics used as laser gain and passive Q-switching media (original) (raw)

2019, The Journal of Chemical Physics

This paper focuses on the kinetics of Cr 4+ formation in Cr,Ca:YAG ceramics prepared by solid-state reaction sintering. The kinetics of Cr 4+ formation was studied by annealing of Cr,Ca:YAG ceramics in ambient air under different temperatures at different times, resulting in the transformation of Cr 3+ to Cr 4+. The activation energy (Ea) of Cr 3+ oxidation determined by the Jander model was 2.7 ± 0.2 eV, which is in good correlation with the activation energy of innergrain oxygen diffusion in the YAG lattice. It is concluded that Cr 3+ to Cr 4+ transformation in YAG ceramics is limited by oxygen diffusion through the grain body. It was established that in Cr,Ca:YAG ceramics, the intralattice cation exchange, in which the Cr 4+ ions exchange positions with the Al 3+ ions, switching from "A" to "D" sites, is faster than Cr 3+ to Cr 4+ oxidation. In the temperature range of 900-1300 ○ C, the reaction enthalpy of Al 3+ /Cr 4+ ion exchange between octahedral "A" and tetrahedral "D" lattice sites is close to zero, and this exchange ratio is thermodynamically driven by entropy.

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Dynamics of chromium ion valence transformations in Cr,Ca:YAG crystals used as laser gain and passive Q-switching media

Optical Materials, 2003

Thermal treatment of YAG crystals co-doped with Cr 4þ and Ca 2þ exhibits reversible oxidation-reduction reactions of the chromium ions, which depend on both temperature and ambient atmosphere. Dynamics of these reactions were studied by the spectral absorption and fluorescence characteristics of Cr,Ca:YAG crystals following different thermal treatment procedures. The absorption spectra were resolved into different peaks, of modified Lorentzian line-shape. Full reduction of Cr 4þ into Cr 3þ is obtained by prolonged heating under vacuum, or in an ambient atmosphere of Ar:5 vol.% H 2 mixture at $1000°C. Saturated oxidation is obtained by prolonged heating at elevated temperatures in free air. The oxygen diffusion coefficient is estimated as (1.85 AE 0.2) Â 10 À6 cm 2 /s at 850°C, with an activation-energy of (1.7 AE 0.07) eV. Only a small fraction of Cr 3þ ion concentration transforms into Cr 4þ. The latter may reside in either octahedral or tetrahedral sites, each exhibiting a different absorption spectrum. Transition from octahedral sites to tetrahedral ones is thermally activated, although no unique thermal activation energy may be assigned to the process. Knowing the process parameters now allows one to optimize oxidization procedures administered to Cr,Ca:YAG crystal devices that are used as laser gain media or as saturable absorbers.

Efficient energy transfer between Ce3+/Cr3+ and Nd3+ ions in transparent Nd/Ce/Cr:YAG ceramics

Optical Materials, 2011

This paper reports the spectroscopic and laser characteristics of transparent ceramics of YAG:Nd codoped with Ce and Cr. The ceramics were prepared by advanced ceramic techniques and showed more than 85% of transparency. Diode pumped laser oscillation performed at different output coupler transmissions (T) showed that a maximum slope efficiency of 16% was achieved for T = 3%. The cross energy transfer mechanism under violet laser diode pumping has been analyzed and the possible energy transfer mechanisms have been proposed using the various energy levels of the dopant ions. The emission lifetimes of the dopant ions at two different concentrations have also been found.

Optical characteristics of Cr3+ and Nd3+ codoped Y3Al5O12 ceramics

Optics & Laser Technology

The optical characteristics of Cr 3 þ and Nd 3 þ codoped Y 3 Al 5 O 12 (YAG) ceramics are measured. These measurements are done using two pumping sources, a 808 nm laser diode (LD) and a Xe short-arc lamp, to simulate solar radiation. The specimens used are 0:1%Cr 3 þ =1:0%Nd 3 þ and 3:0%Cr 3 þ =1:0%Nd 3 þ (atomic%) codoped YAG ceramics. A Nd:YAG crystal doped with 1:0%Nd 3 þ is used as a reference. The saturation intensities of the Cr/Nd:YAG ceramics pumped by the LD are the same as that of the Nd:YAG crystal, while they are higher when they are pumped by the Xe lamp. The saturation intensities are 3:23 7 0:18 kW=cm 2 for the 0:1% Cr-doped ceramic and 4:30 7 0:24 kW=cm 2 for the 3.0%Cr-doped ceramic. The small signal gains of the 0.1%Cr-doped and 3.0%Cr-doped ceramics are measured and found to be 1.8 times and 7.0 times higher than that of Nd:YAG for the same intensity of solar pumping, respectively. The quantum efficiency of energy transfer from Cr 3 þ to Nd 3 þ is estimated to be 0:88 7 0:09 for the 0.1%Cr-doped ceramic and 0:67 7 0:08 for the 3.0%Cr-doped ceramic.

Performance of YAG: Cr4+ laser crystal

Optical Materials, 1994

The results of investigations of emission, saturable absorption and lasing properties of YAG:Cr4~crystal are summarized and analyzed. A spectroscopic and thermodynamic model of the dopant centera four-fold coordinated Cr4~ion, a new activator ofmaterials for solid state quantum electronicsis developed. The polarization dependencies of emission, saturable absorption and lasing properties of YAG:Cr4~crystal are shown to be accounted for by the tetragonal symmetry ofthe new dopant center. The authors analyze the transition probabilities between the energy levels, working in the Cr4' active center.

Distribution of oxidation states of Cr ions in Ca or Ca/Mg co-doped Cr:Y3Al5O12 single-crystal fibers with nitrogen or oxygen annealing environments

Journal of Crystal Growth, 2008

The valence states of Cr ions in Ca or Ca/Mg co-doped Cr:Y 3 Al 5 O 12 (YAG) single-crystal fibers are studied. The fibers were grown using the laser-heated pedestal growth method, followed by annealing treatments up to 1500 1C. The concentrations of the Cr 3+ and Cr 4+ ions in octahedral and tetrahedral sites in oxygen or nitrogen environments were characterized. Above 700 1C, migration of Cr 4+ between octahedral and tetrahedral sites takes place; its relative stabilization energy was estimated. For Ca,Cr:YAG annealed in an oxygen or nitrogen environment, it was 0.25 and 0.3 eV, respectively. For Mg,Ca,Cr:YAG annealed in oxygen or nitrogen, it was 0.47 and 0.49 eV, respectively. For the Ca,Cr:YAG crystal fiber (Ca/Cr ¼ 113.1%) with oxygen annealing, about 35% and 2.5% of Ca ions took part in charge compensation for Cr 4+ in the octahedral and tetrahedral sites, respectively. The density of oxygen vacancies depends on the concentration of Ca ions. The estimated ratios of the unreacted oxygen vacancies to total oxygen vacancies were about 63% and 88% for oxygen and nitrogen annealing, respectively. The main limitation on the concentration of Cr 4+ in the tetrahedral site of YAG is the presence of unreacted oxygen vacancies.

Chromium recharging processes in the Y<formula><inf><roman>3</roman></inf></formula>Al<formula><inf><roman>5</roman></inf></formula>O<formula><inf><roman>12</roman></inf></formula>:Mg,Cr single crystal under the reducing and oxidizing annealing influence

International Conference on Solid State Crystals 2000: Growth, Characterization, and Applications of Single Crystals, 2001

The influence of reducing and oxidizing annealing on optical absorption spectra of the yttrium aluminium garnet (YAG) single crystal co-doped with Mg and Cr is investigated using step-by-step isothermal and isochronous thermal treatment in H 2 or air flow. The changes in the spectra were analyzed using decomposition on elementary absorption bands of Gaussian shape. The separeted absorption bands attributed to the Cr 4 ÷ ions occupying octahedral and tetrahedral sites in garnet lattice demonstrate different behaviour. The analysis allowes to distinguish the electronic recharging process Cr 4 +Oct] _ &+[Oc] taking place in the octahedral sites of garnet lattice and having lower activation energy from the chromium migration process Cr 4 +[,it<-• Cr 4 ÷[oti happening at higher temperatures or longer exposure. Estimations show that approximately 0.2% of total number of chromium ions occupied tetrahedral sites forming phototropic centers in the YAG: Mg, Cr crystal.

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