Ligand Effects on ESR and Optical Properties of Gold Atoms in γ Irradiated Organic Solid Solutions at 77 K

• Published in: The journal of physical chemistry. B Vol. 109; no. 40; pp. 18942 - 18948
• Main Authors: Hase, Yoko Miyatake, Ito, Yoshitaka, Tajima, Yusuke
• Format: Journal Article
• Language: English
• Published: United States American Chemical Society 13.10.2005
• Subjects: Electron Spin Resonance Spectroscopy - methods; Ethanol - chemistry; Ethanol - radiation effects; Furans - chemistry; Furans - radiation effects; Gamma Rays; Gold - chemistry; Gold - radiation effects; Hydrochloric Acid - chemistry; Ligands; Magnetics; Optics and Photonics; Sensitivity and Specificity; Temperature
• ISSN: 1520-6106; 1520-5207
• DOI: 10.1021/jp053738h

Ligand effects on ESR and optical properties of Au0 atoms produced at 77 K in γ irradiated solid solutions of AuCl/MTHF and AuCl/EtOH with and without HCl were investigated. Four groups of ESR lines were observed at 73 K more clearly around the magnetic fields at about 250, 280, 340, and 400 mT for both γ irradiated MTHF and EtOH solid solutions with HCl than those without HCl. The values of a and g J calculated by Breit−Rabi analysis showed a remarkable dependence on the solvent polarity. It was confirmed that the signals were the hyperfine quartet corresponding to the transitions between the Zeeman levels of Au0 atoms with nuclear spin of 3/2 in the ground state, 2S1/ 2. It was also confirmed that Au0 atoms produced after γ irradiation were located in the nuclear environment of isotropic interaction with surrounding ligand molecules. Delocalization of the unpaired spin density of Au0 onto ligands is found to be as large as one in the case of Cu0 atoms. Our previous hypothesis of the occurrence of configuration mixing of d valence orbital into the wave function of the atom in its 2S1/2 was strongly supported. The dependence of the ESR, optical absorption, and the steady-state emission and excitation characteristics on solvent polarity was cleared in this study. We observed two kinds of emissions i.e., a band at 385 nm and a set of emission bands at 456, 482, 484, and 520 nm. These correspond to two bands out of the six kinds of emissions observed previously. The bands were attributed to exciplex (Au0·Ln···Au+)* and the excited Au0 atoms trapped in a large cavity, respectively. The negative counterion of Au+ of the gold compound plays an important role for the formation of the exciplexes.