The vanadate crystals YVO4, GdVO4 and LuVO4 are good host materials for diode-pumped neodymium-doped lasers because they have large absorption and emission cross sections, have broad bandwidths and naturally lase in a single polarization.Experiments with ytterbium-doped YVO4 and GdVO4 also have yielded positive laser results, and now scientists at Max Born Institut für Nichtlineare Optik und Kurzzeitspektroskopie in Berlin and at Shandong University in Jinan, China, have reported equally positive results with Yb:LuVO4.The investigators grew their Yb:LuVO4 by the Czochralski technique from a melt with 1.5 percent ytterbium doping. Because the ionic radius of ytterbium is very close to that of the lutetium it replaces in the crystal lattice, the ytterbium concentration in the crystal was 1.56 ±0.01 atomic percent, nearly identical to the concentration of the melt.They measured the spectroscopic properties of Yb:LuVO4 and then observed laser oscillation in the material under pumping with a Ti:sapphire laser and a diode laser. They found, spectroscopically, the spontaneous lifetime was 256 µs, roughly the same as ytterbium in the other vanadate hosts. The absorption and emission cross sections were strongly polarization-dependent, as in all vanadates. Surprisingly, a trend observed in neodymium-doped vanadates, namely that the cross sections increase going from GdVO4 to YVO4 to LuVO4, appears not to be present in the ytterbium-doped vanadates.For the Ti:sapphire-pumped laser experiments, the scientists placed a 2-mm-thick, uncoated piece of Yb:LuVO4 in a three-mirror resonator at Brewster’s angle. The 985-nm pump light entered the resonator through the folding mirror and was focused to an ~22-µm Gaussian waist at the crystal. From an absorbed pump power of 1.5 W, the laser generated 360 mW at 1041 nm (Figure 1). At this point, the laser’s optical efficiency was 24 percent and its slope efficiency, 47 percent.4 Laser Produces More Than 1 W" hspace="6" src="https://www.photonics.com/images/Web/Articles/2006/1/1/TechLaser1.gif" width="240" align="left" vspace="6" border="0" />Figure 1. Under Ti:sapphire pumping, the Yb:LuVO4 laser achieved 360 mW at a slope efficiency of 47 percent. T = transmission of output coupler. Images ©OSA.The results are similar to those obtained by others with Yb:GdVO4 and Yb:YVO4, but the threshold for Yb:LuO4 observed in this case was somewhat higher. The investigators attribute this to higher-than-optimal ytterbium doping in their sample.For the diode-pumping experiments, they used the same 2-mm-thick sample but placed it in a two-mirror, hemispherical resonator. They focused the 981-nm pump light through the flat mirror to an ~40-μm spot on the crystal. The highest output was 1.05 W, obtained with a 2.1 percent output coupler (Figure 2). The laser’s optical efficiency was 15.4 percent, and the slope efficiency was 20.7 percent. 4 Laser Produces More Than 1 W" hspace="6" src="https://www.photonics.com/images/Web/Articles/2006/1/1/TechLaser2.gif" width="240" align="right" vspace="6" border="0" />Figure 2. When pumped with a 981-nm diode laser, the Yb:LuVO4 laser generated 1.05 W with a slope efficiency of 20.7 percent. T = transmission of output coupler; η = slope efficiency; and λ = output wavelength.The 2-mm piece of Yb:LuVO4 employed in the laser experiments was mounted on a copper holder but otherwise was uncooled. Nonetheless, no saturation or rollover was evident at the upper reaches of the input/output curves. The scientists expect that significantly higher power could be obtained by actively cooling the laser crystal, by antireflection-coating it and by matching the pump light more closely to the laser crystal’s absorption peak.