Study of formation and ionizing collision processes of highly excited Rydberg species

真司 植松

Andrey N. Klyucharev, A. V. Lazarenko

悟 山田

Xianzhao Peng, James E. Abbott, Wei Kong

Using a mass analyzed threshold ionization (MATI) spectrometer, the spectra of the monomer, dimer, and trimer of sodium were measured. Intense dimer signals both at the ionization threshold and at Rydberg resonances of the monomer were observed. Below the adiabatic threshold of the dimer, a trimer spectrum which showed vibrational progressions similar to those of the dimer was also recorded. In both cases, the high energy edge of the heavier cluster was shifted to a lower energy compared with that of the lighter cluster. The monomer time-of-flight spectrum at the Rydberg resonances was diffuse, while the time-of-flight spectrum of the dimer was sharp and intense. Based on the continuity of oscillator strength and further energetic analysis, we conclude that the dimer signal at the Rydberg resonances of the monomer originated from collisional association between a Rydberg state atom and a ground state atom. Similarly, the trimer signal was from the combination between a Rydberg state dimer and a ground state atom. The combined product from collision was in a Rydberg state that can be field ionized during MATI detection. This work offers direct experimental evidence for the formation of high Rydberg state species through collisional recombination.

James Veale

Alisa I. Walz‐Flannigan

We have observed the evolution of cold Rydberg gases and ultracold plasmas in an environment that allows for the control of interactions of the blackbody radiation temperature from 4K to 300K. The work in this thesis describes the influence of initial densities, populations, excitation state, evolution time and thermal background temperature on the evolution of cold Rydberg gases as well as directly excited ultracold plasmas. With some initial ionization, cold-Rydberg-atom gases easily develop a positive space charge that traps electrons for times on the order of tens of mus. This acts as a catalyst for electron-Rydberg atom collisions, increasing the collision probabilities by orders of magnitude and profoundly altering the final state of the Rydberg gas. Using state-selective field ionization, we have provided direct proof that these collisions cause changes in l-states, and we have seen the first experimental evidence that they also lead to inelastic n-changing collisions, as predicted by theory. We have also found evidence for Rydberg-Rydberg collisions, enabled by the attractive electric-dipole forces between atoms in high-l states and possibly by van-der-Waal's interactions at very high-n . Thermal interactions are seen to influence the formation of a plasma from a cold Rydberg gas. Plasmas form more easily in the presence of a 300K radiation field than at 4K, due to the contribution of thermal ionization to the plasma formation. The background temperature also appears to affect the electron temperature in both the directly excited plasma and the plasma spontaneously formed from a cold Rydberg gas. In Rydberg atom gases that have undergone partial ionization, electron temperatures were estimated using the dependence of n-changing collisions on the electron temperature.