O atoms in the P-3(2), P-3(1), and P-3(0) states were detected by vacu
um-ultraviolet laser-induced fluorescence (VUV LIF) technique. The O(P
-3(2)), O(P-3(1)), and O(P-3(0)) atoms were produced by the collisiona
l reaction between the O atoms in the D-1 excited state and collision
partner N-2. O atoms in the D-1 excited state were obtained hy photodi
ssociation of N2O at 1930-nm laser light. As O(P-3(2)). O(P-3(1)), and
O(P-3(0)) species have their first transition in the VUV region, the
probe laser was used to excite O(2p(3)P(J=2.1.0)) atoms to the O(3s(3)
S(0)) state at 130.212 nm for j = 2, 130.481 nm for j = 1, and 130.597
nm for j = 0. A four-wave difference frequency mixing (2 omega(1) - o
mega(2)) process using Kr as nonlinear media was employed to generate
130-nm probe laser light.