Multireference averaged quadratic coupled cluster (MRAQCC) (4,5)/cc-pVTZ calculations predict that bond pseudorotation (BPR) in the first excited singlet state of the cyclopentadienyl cation (CPC) proceeds with a barrier of just 0.35 kcal/mol, where five dienylic forms present the minima and five allylic forms the transition states of the pseudorotation process.Vibrational and entropic corrections revert the order of stabilities and lead to a G(298) of just 0.05 kcal/mol indicating that BPR is unhindered at room temperature. The description of the CPC ring in terms of curvilinear deformation coordinates (seven for C 5 , seven for X 5 , and three coupling coordinates) make it possible to explore both the six-dimensional (6D) Jahn-Teller and the 8D pseudo-Jahn-Teller space and assess the importance of Jahn-Teller and pseudo-Jahn-Teller deformations of the CPC ring. The latter dominate the ring deformations along the BPR path. The only somewhat larger Jahn-Teller contribution results from a E 1 -symmetrical CCH bending motion. For the perhalogenated CPCs, the dominance of the pseudo-Jahn-Teller effect increases, however, the total deformation of the D 5h -symmetrical ring decreases and thereby also the stabilization of the 1 A 1 forms along the BPR path. This leads to a reduction of the BPR barriers to just 0.14 kcal/mol for C 5 I + 5 . For all pentahalogeno CPCs, the dienylic form is more stable both at the energy and free energy level. The use of curvilinear deformation coordinates facilitates the understanding of the electronic features of cyclic (pseudo-) Jahn-Teller systems. Fig. 1) and the relevance of its three (n = 1, 2, 3) elementary BPR processes (see Fig. 2) for electronic structure and dynamic behavior is analyzed. The three BPR motions lead in some combination to the actual BPR of CPC shown in Fig. 3, and we will quantitatively determine their contributions.
2-5,CPC has been the target of several experimental investigations, [6][7][8][9] which because of its peculiar electronic structure and chemical behavior triggered extended computational studies. [9][10][11][12][13][14] CPC was identified in the mass spectrum [15,16] and its solvolytic generation was reported by Tidwell and coworkers, [17] who also summarized the early synthetic work on CPC. The ground state of CPC was identified to be a triplet with D 5hsymmetry (X 3 A 2 ) and the adiabatic singlet-triplet splitting was determined to be 4.38 kcal/mol. [9] Special focus was laid on the description of the first excited singlet state of 1, which according to electronic structure theory should be an antiaromatic D 5hsymmetrical 1 E 2 state with 4π electrons (1c, Fig. 1). A possible Jahn-Teller distortion of this state was discussed at an early stage where a summary of the early theoretical work on CPC can be found in the book by Bersuker. [3] Recently, a detailed pulsed-field-ionization zero-kinetic-energy (PFI-ZEKE) photoelectron spectroscopy study of C 5 H + 5 and C 5 D + 5