-------------------------------------------------------------------- COLLOQUIUM OF THE LABORATORY FOR COMPUTER DESIGN OF MATERIALS School of Computational Sciences (CSI 898-Sec 001) -------------------------------------------------------------------- NEGATIVE IONS WITH DIFFUSE EXCESS ELECTRONS KIT H. BOWEN, JR. Department of Chemistry, Johns Hopkins University, Baltimore, Maryland 21218, USA The extra electron in valence (conventional) anions resides in an orbital which is firmly grounded on the nuclear framework of the system, i.e., the extra electron is localized. Likewise, when such anions are solvated and become anion-molecule complexes, the extra electron usually remains localized with the anion. During photodetachment of the excess electron from such a cluster anion, this sub-anion acts as the chromophore, and the photoelectron spectrum reflects the characteristics of that anion, albeit stabilized and spectrally shifted to higher electron binding energy. In other cluster anions, however, the excess electrons are more delocalized,even though they remain closely associated with their nuclear frameworks. There is, however, still another class of molecular and cluster anions in which the excess electrons are neither localized nor closely associated with their nuclear frameworks, and these are anions with highly diffuse, excess electron distributions. Examples include dipole bound anions, quadrupole bound anions, double Rydberg anions, and some sizes of water cluster anions. While these species share the characteristic of having spatially diffuse excess electrons, they are otherwise bound by different, albeit idealized interactions. The excess electron in dipole bound anions is chiefly bound by the dipolar field of the corresponding neutral system, with the excess electron ballooning out into space at the positive end of the molecular or cluster system. Similarly, the excess electron in quadrupole bound anions is primarily bound by the quadrupolar field of the corresponding neutral system. Double Rydberg anions are the negative ions of Rydberg radicals. Each one can be thought of as a closed shell, cationic core which is enveloped by two Rydberg-like, highly diffuse electrons. Also, many water cluster anion systems appear to exhibit diffuse excess electron states of at least two types, with a third type being associated with internalizing electron states. In this talk, we will survey these different types of diffuse electron states, but we will focus on double Rydberg anions, in part because they are the least well-known diffuse, excess electron species. In particular, we will discuss the ammonia-based double Rydberg anions, (NnH3n+1)-, where n = 1- 7. Using anion photoelectron spectroscopy, we have measured electron affinities of these species, found examples of solvated double Rydberg anio ns, and accessed the first electronic states of several neutral Rydberg radicals by photodetaching electrons from their corresponding double Rydberg anions. Insight into the nature of these species was further aided by comparisons with the absorption measurements of Fuke on neutral Rydberg cluster-like radicals and by several theoretical studies, especially those of Ortiz. Monday , April 4, 2005 4:30 pm Room 206, Science & Tech. I, Fairfax Campus Refreshments will be served at 4:15 PM. ---------------------------------------------------------------------- Find the schedule at http://www.scs.gmu.edu/lcdm/seminar/schedule.html --------------------------------------------------------------------