1M. Chergul, V. Chandrasekharan, W. Bohmer, R. Haensel, H. Wilcke, and N. Schwentner, Chem. Phys. Lett. 105, 386 (1984). 2M. Huber, Helv. Phys. Acta, 37, 329 (1964).Author Institution: Chemical Physics Laboratory, SRI International; Chemical Physics Laboratory, SRI InternationalBy using the techniques of stimulated emission pumping combined with fluorescence dip spectroscopy it has been possible to characterize the getastable NO(L^{\prime}^{2}\Phi) state. The spectroscopic parameters are: Teβ=53740.81Β±0.20cmβ1Οeβ=999.36Β±0.18cmβ1Beβ=1.1189Β±0.0029cmβ1A=β42.480Β±0.032β0.310Β±0.035(v+1/2)cmβ1βreβ=1.4204Β±0.0037AΛΟeβxeβ=9.92Β±0.03cmβ1Ξ±eβ=0.019Β±0.0027cmβ1β The state is produced by initially populating NO(B^{\prime}^{2}_{\Delta_{5/2}}, v = 3, J= 7.5) with 157.630 on radiation from an F2β laser. While observing the Bβ²βX fluocescence emission, a Raman-shifted dye laser is tuned through the appropriate spectral regions (950-1300 nm), and intensity decreases are observed at the positions of the J = 6.5, 7.5, and 8.5 rotational levels of the 2Ξ¦ state (as well as other states). The first four vibrational levels have been detected in this manner, with the numbering being confirmed by the recent matrix isolation detection of v=0 by Chergui et al.1 Perturbations in the v=1 level of the B^{\prime}^{2}\Delta state, postulated by Huber2 as being due to the L^{\prime}^{2}\Phi state, are shown to involve the v=9 level. Supported by the National Science Foundatio