25) Win@, R. K.; Peterson, v. J.; Fassei, v. A. APPl. sPectKJsc. 1979, 33, 206.Laser-excited atomlc Huotescence in a graphne furnace gives detection IbnHs for Pb, Cu, Mn, Sn, AI, In, LI, and Pt, in the pkogram to sub-picagram range. The linear dynamk range for these elements varles from 3 to 7 orders of magnnude. A graphlte rod, a plain graphite cup, and a slotted graphite cup are compared as the cuvette In the fluorescence system.Detection lhnlts for a pyrolytic coating, a tantalum foil liner, and a tantalum carbide coating of the graphlte cuvette are compared. A hydrogen-argon atmosphere, a low-pressure atmosphere, and an argon atmosphere are compared as the atmosphere s u r r o w the graphite cuvette. Lastly, Cu and Yn are determined In several standard reference materials.Laser-excited atomic fluorescence using a graphite furnace has been shown to give very low detection limits (1-9). Bolshov et al. (5) achieved excellent detection limits for Pb, Fe, Na, Pt, Ir, Eu, Cu, Ag, Co, and Mn, using a Nd:YAGpumped dye laser system. These results ranged from 1.5 fg for P b to 300 pg for Eu. Tilch et al. (7) utilized a nitrogenpumped dye laser system to obtain similar detection limits for some of the same elements as well as a few others. Probably the most impressive reaulb have been the femtogram detection limits for Pb. Besides Bolshov and Tilch (5, 7) Human et al. (6) also obtained a detection limit in the femtogram range for Pb.Pulsed lasers offer several advantages for atomic fluorescence such as wide tunability and high peak powers. However, these lasers are less than optimum when using electrothermal atomization because of the low repetition rate (e.g., 20 Hz) of the lasers. The pulsed laser must be synchronized so that there is a laser pulse during the time when atoms are present in the laser path. This problem can be overcome somewhat by using a computer to synchronize the laser pulse with the formation of atoms during the atomization stage or by confining the atomic vapor within a tube atomizer to increase the residence time. An alternative is to operate the pump laser at higher frequencies if possible, e.g., by use of a copper vapor laser pumped dye laser system a t ca. 6 kHz. The atomizer requires a special design for atomic fluorescence since the fluorescence is viewed at 90' to the laser beam. A graphite cup (5, 7), a Massmann cup (IO), a graphite tube with holes cut in the sides (9), and a graphite rod ( I , 6), are several designs that have been tried. The simplicity of the graphite rod makes it attractive for use with volatile elements. On the other hand, the graphite cup offers an improvement over the graphite rod because the sample is in a semienclosed 0003-2700/86/0358-2598$01.50/0 environment, which gives more of a "furnace" effect. However, the atoms still must emerge from the furnace into the cooler atmosphere before being excited by the laser. As the atoms vaporize out of the hot furnace they have more of a chance to react with interferents, such as 02. In principle, the best atomizers are those...