PACS 71.35.Aa, 71.55.Ht, 78.55.Hx For the first time the characteristics of the main emission of Al 2 (WO 4 ) 3 are reported. In order to distinguish the excitonic and electron-hole processes in Al 2 (WO 4 ) 3 we measured the creation spectrum of photostimulated luminescence under irradiation by synchrotron light and compared it to the excitation spectrum of the main emission. It is shown that the onset of the excitation spectrum of the main 2.7 eV emission of Al 2 (WO 4 ) 3 is at 5 eV, while the threshold of the creation of electron-hole pairs is measured to be 8.7 to 9.5 eV at 8 K. The latter value is in good agreement with the band-gap value of α-Al 2 O 3 (9.4 eV). This supports the suggestion that free electrons and holes are created in tungstates due to electronic transitions from oxygen to cation states situated several eV above the bottom of the conduction band.
IntroductionWe have shown earlier [1] that in a sequence of tungstate crystals, the creation of electron-hole (e-h) pairs occurs at energies 1-2 eV above the fundamental absorption edge. This feature has not been observed for other crystals like, e.g., simple oxides. In such tungstates, only excitons, selftrapped on the oxyanionic complex, are created under excitation in the lower part of the conduction band. These tungstate crystals are characterized by a high light yield at room temperature. We suggest that the high probability of self-trapping and low mobility of excitons, which prevent energy transport to crystal defects with the subsequent non-radiative decay of the excitons, are responsible for the high light yield of tungstates. There are two possible explanations for the creation of e-h pairs in the crystals studied: i) ionisation due to excitation of the upper oxyanionic states and ii) excitation of cation states whose relative position in the conduction band strongly depends on the host cation. The good agreement between the threshold energy of e-h pair creation in a certain metal tungstate and the band-gap width in the corresponding metal oxide, observed for several tungstate crystals [1], seems to support the latter suggestion. To prove the important role of cationic states in the formation of free electrons and holes in oxyanionic crystals, we have chosen to study and synthesize a tungstate material Al 2 (WO 4 ) 3 with a cation, whose oxide has one of the largest band-gaps known among oxide crystals (9.4 eV for α-Al 2 O 3 [2]).Aluminium tungstate has an orthorhombic structure and belongs to the Pnca space group [3]. This little-known compound attracted attention of researchers as a trivalent cation ionic conductor [4][5][6] and when doped with trivalent ions, e.g. Cr 3+ [7] and Yb 3+ [8], as a laser host material. The optical properties of pure aluminium tungstate have not been reported earlier.