Thermal properties of clusters and molecules - Experiments on evaporation, thermionic emission, and radiative cooling

摘要

This thesis presents experiments performed on clusters and molecules, where the three channels of unimolecular decay have beenstudied. Evaporation from protonated and negatively charged water cluster have yielded size dependent heat capacities, where thesmallest sizes with fewer than $21$ molecules show a heat capacity similar to bulk ice whereas clusters with molecules between $21$ and $300$ have a heat capacity in between that of ice and liquid water. The increase in heat capacity per added molecule in the cluster indicates that the intramolecular degrees of freedom are frozen atthe temperatures in the experiment (T$pprox!!!160$~K). Experiments on small mixed water-ammonia clusters resulted inrelative evaporation fractions for sizes between a total of three to eleven molecules, and $16$ molecules. The clusters were found to evaporate predominantly water molecules except for clusters containing six or more ammonia molecules. Relative evaporation ratesfor D$_2$O, HDO, and H$_2$O were measured for NH$_4^+$(H$_2$O)$_4$ with zero to six deuteriums interchanged with the hydrogens. The relative rates were found to be $1:0.71:0.56$.Absolute timedependent cooling rates for hot C$_{60}^-$ were obtained in an electrostatic storage ring with single photon absorption experiment. The cooling of the molecule could be divided into a thermionic emission part and a radiative part, where the crossover between the two occurred at $5$~ms, after which radiation was shown to be the dominant cooling channel. The spontaneous decayprofiles were used to extract decay parameters of the large organic anion zink phthalocyanine (ZnPc). Numerical simulations of the decay process show good agreement with measurements, using parametersderived from an analytical approximation also used for fullerenes. Photoabsorption experiments were performed on the much smaller C$_5^-$, showing the presence of strong radiative cooling. The cooling rate was determined by the dependence of the photoinduced neutralization yield vs. photon energy and laser firing time.