Electronically excited states of water clusters of 7-azaindole: Structures, relative energies, and electronic nature of the excited statesThe geometry of the Fabry-Perot cavity makes it difficult to use for measuring the Stark effect. A ''Stark cage'' is described which generates an electric field suitable for this purpose. The cage is used to measure first and second order Stark splittings of several low-J transitions of the benzene-water dimer previously reported ͓Gutowsky, Emilsson, and Arunan, J. Chem. Phys. 99, 4883 ͑1993͔͒. The dipole moment is found to depend somewhat on rotational state, ranging from 1.65 to 2.00 Debye for both ground mϭ0 and first excited mϭ1 internal rotation states of the dimer. Additional mϭ1 transitions are reported, including the previously missing downshifted line of a kϭ0Ј doublet. Its presence and various Stark effects require reassignment of the mϭ1 spectrum. The results demonstrate that each J→Jϩ1 spectrum consists of three distinct components which arise from the H 2 O in an unusual way. In addition to the k-doublets, there are two progressions; a set of (Jϩ1) negative k's running from ϪJ to 0, and a set of (JϪ1) positive k's with somewhat smaller spacings, running from ϩ2 to ϩ(JϪ1). It is proposed that each of the three components is associated primarily with one of the three 1 01 , 1 11 , and 1 10 rotor states of the water. These ''patches'' are attributed to the potential energy surface ͑PES͒. Molecular mechanics for clusters ͑MMC͒ calculations indicate barriers of 300-600 cm Ϫ1 to internal rotation of the water about any of its inertial axes and nearly free rotation about an axis parallel to the benzene C 6 axis. This novel PES leads to unusual internal motions; asymmetric top rotations of the water about the benzene C 6 axis instead of the usual rotation about an inertial axis of the water.