In contrast to Yb 3+ which is a well-investigated optically active ion, the spectroscopic properties of its divalent counterpart Yb 2+ in glasses are hardly investigated, although Yb 2+ might have a notable influence on the luminescence properties of Yb 3+ -doped glasses even at low Yb 2+ concentrations because of its strong f-d transitions. In this paper, we report on the preparation and spectroscopic properties of Yb 2+ -doped aluminosilicate glasses that were produced using the normal meltquench technique. The glass composition is 20CaOÁ20Al 2 O 3 Á60SiO 2 (mol%). To achieve a sufficient amount of Yb 2+ in the samples, different methods were applied to influence the red-ox equilibrium during glass melting: firstly, under argon atmosphere and additional argon bubbling, and secondly by the addition of metallic aluminum powder to the batch. The strongly reduced samples show a greenish to brownish yellow coloring which could be attributed to the strong absorption of Yb 2+ ions in the UV to blue spectral range. The absolute Yb 2+ concentration in the glass and the molar extinction coefficient of Yb 2+ was obtained by spectroscopic measurements. If irradiated with UV light, the Yb 2+ -doped samples show a broad fluorescence emission in the wavelength range from 450 to 700 nm with a peak at around 515 nm.silicate, optical glasses, aluminosilicate glasses, ytterbium II, photoluminescence
| INTRODUCTIONIn contrast to the well-studied Yb 3+ ions, investigations of its lower oxidation state Yb 2+ are hardly reported for melt-quenched glasses. However, Yb 2+ might occur besides the widely used Yb 3+ , and hence information on its optical properties and its red-ox behavior are quite essential. The optically active ion Yb 3+ is used in highpower laser materials, laser fibers and scintillator materials but also as sensitizer for energy transfer and up-conversion processes. 1-3 Recently, the Yb 3+ ion was proposed to improve the solar cell efficiency by utilizing the quantum cutting effect, as it emits close to the efficiency maximum of silicon-based solar cells at around 1000 nm. 4-6 To collect large parts of the solar spectrum, broad band f-d absorption in the UV to blue spectral region is needed. This can for example be achieved by the addition of by Ce 3+ and Eu 2+ . Additionally, the absorption and emission wavelengths of these ions can be tuned to fit the spectral requirements for quantum cutting in connection with Yb 3+ . 7,8 However, the problem in Eu 2+ /Yb 3+ and Ce 3+ / Yb 3+ co-doped materials is the formation of Eu 3+ /Yb 2+ or Ce 4+ /Yb 2+ charge transfer states, which both quench the Eu 2+ or Ce 3+ emissions which is needed for the quantum cutting process. 9,10 To determine whether these charge transfer states are formed, a good knowledge on the spectral properties of Yb 2+ in the host material is required. On the other hand, also the Yb 2+ /Yb 3+ ion pair has been proposed for quantum cutting, since Yb 2+ -as Ce 3+ and Eu 2+ -shows broad and strong absorption in the UV to visible range because of f-d transiti...