15min:
THE LOWEST 3(n, pi*) STATE OF 2-CYCLOPENTEN-1-ONE: CAVITY RINGDOWN ABSORPTION SPECTRUM AND RING-BENDING POTENTIAL ENERGY FUNCTION.

NATHAN R. PILLSBURY, STEPHEN DRUCKER, Department of Chemistry, University of Wisconsin-Eau Claire, Eau Claire, WI 54702; JAEBUM CHOO, Department of Chemistry, Hanyang University, Ansan 425-791, Korea; JAAN LAANE, Department of Chemistry, Texas A & M University, College Station, TX 77843.

The room-temperature cavity ringdown absorption spectra of 2-cyclopenten-1-one (2CP) and deuterated derivatives were recorded near 385 nm. The very weak ( epsilon < 1 M-1 cm-1) band system in this region is due to the T leftarrow S0 electronic transition, where T is the lowest-energy 3(n, pi*) state. The origin band was observed at 25,963.6 cm-1 for the undeuterated molecule and at 25,959.4 and 25,956.2 cm-1, respectively, for 2CP-5-d1 and 2CP-5,5-d2. For the -d0 isotopomer, about 50 vibronic transitions have been assigned in a region from -500 to +500 cm-1 relative to the origin band. Nearly every corresponding assignment was made in the -d2 spectrum. Several excited-state fundamentals have been determined for the d0/d2 isotopomers, including ring-twisting ( nu29'=238.9/227.8 cm-1), out-of-plane carbonyl deformation ( nu28'=431.8/420.3 cm-1), and in-plane carbonyl deformation ( nu19'=346.3/330.2 cm-1). The ring-bending ( nu30') levels for the T state were determined to be at 36.5, 118.9, 213.7, 324.5, and 446.4 cm-1 for the undeuterated molecule. These drop to 29.7, 101.9, 184.8, 280.5, and 385.6 cm-1 for the -d2 molecule. A potential energy function of the form V = ax4 + bx2 was fit to the ring-bending levels for each isotopic species. The fitting procedure utilized a kinetic energy expansion that was calculated based on the structure obtained for the T state from ab initio calculations.The barrier to planarity, determined from the best-fitting potential energy functions for the -d0, -d1, and -d2 species, ranges from 42.0 to 43.5 cm-1. In the T state, electron repulsion resulting from the spin flip favors nonplanarity. The S0 and S1 states have planar structures that are stabilized by conjugation.