1996
DOI: 10.1063/1.361801
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Excited-state absorption of Tm3+-doped single crystals at photon-avalanche wavelengths

Abstract: Excited-state absorption (ESA) spectra calibrated in units of cross sections are reported in the case of Tm3+-doped YAG, YAP, and Y2O3 single crystals around wavelengths at which photon-avalanche absorptions were observed recently. The peak ESA cross sections are compared with those obtained theoretically by using the Judd–Ofelt approach.

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Cited by 21 publications
(18 citation statements)
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“…4. One part of the electronic population of the 3 F 2 + 3 F 3 levels then decayed non-radiatively to the 3 H 4 level, as observed in other hosts [3][4][5], and another part absorbed another photon pump up to the 1 D 2 level. The decay from the 3 H 4 to 3 H 6 , 3 F 4 and 3 H 5 levels generated emissions at 801 nm, 1.48 mm and 2.3 mm, respectively.…”
Section: Resultsmentioning
confidence: 91%
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“…4. One part of the electronic population of the 3 F 2 + 3 F 3 levels then decayed non-radiatively to the 3 H 4 level, as observed in other hosts [3][4][5], and another part absorbed another photon pump up to the 1 D 2 level. The decay from the 3 H 4 to 3 H 6 , 3 F 4 and 3 H 5 levels generated emissions at 801 nm, 1.48 mm and 2.3 mm, respectively.…”
Section: Resultsmentioning
confidence: 91%
“…We found in the literature that in other thuliumdoped materials, the population of the 1 D 2 and 1 G 4 levels was only achieved by ESA [3][4][5]15]. However, ESA processes in KGW pumping at 688 nm were not possible because the energy difference between the 3 H 4 and 1 D 2 levels (14876 cm À1 ) and the 3 F 4 and 1 G 4 levels (15125 cm À1 ) is greater than the energy of a photon pump (14535 cm À1 ).…”
Section: Resultsmentioning
confidence: 96%
See 1 more Smart Citation
“…Often referred to as a pump-probe technique [1], ESA measurements have been extensively studied in the past [1][2][3][4][5][6]. Either pump or probe beams can be operated in pulsed or continuous wave (cw) mode.…”
Section: Introductionmentioning
confidence: 99%
“…Uma cascata dos dois amplificadores é utilizada para se obter o espectro diferencial de transmissão o qual resulta em medidas de AEE, absorção de estado fundamental (AEF) e também emissão estimulada (EE). No caso pulsado, 6,[19][20][21] o qual não será abordado aqui, é possível estudar simultâneamente as transições AEE a partir de estados com diferentes valores de tempo de vida. No entanto, este método oferece menor sensibilidade e pior razão sinal ruído do que o método contínuo, o qual pode ser eficientemente aplicado para medidas de AEE a partir de níveis com valores de tempo de vida longo, como os que são aqui discutidos.…”
Section: Introductionunclassified