Rydberg Ionization Spectroscopy

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Rydberg states

For more details on this topic, see Rydberg states.

For more details on this topic, see Rydberg molecules.

Atoms and molecules have ionization energy thresholds associated with the energy required to remove an electron from the ionic core. (The Rydberg formula describes the energy level series of a Rydberg atom.) Rydberg series describe the energy levels associated with almost removing an electron from the ionic core. Each Rydberg series converges on an ionization energy threshold associated with a particular ionic core configuration. These quantized Rydberg energy levels can be associated with the quasiclassical Bohr atomic picture. The closer you get to the ionization threshold energy, the more "near threshold Rydberg states" there are. As the electron is promoted to higher energy levels, the spacial excursion of the electron from the ionic core increases and the system is more like the Bohr model picture. (That is, the ionic core interaction with the Rydberg looks more like the interaction between the proton and the electron in the hydrogen atom. This can be refined by including a correction in the Rydberg formula associated with the presence of the ionic core called the quantum defect.) One way to visualize this system classically is to think of the electron as comet far removed from the solar system that represents the ionic core. The angular momentum of a comet determines if it has a highly elliptical orbit that is more likely to interact with the core of the system or a more nearly circular orbit that is much less likely to interact with core. This is also true for the orbital angular momentum of a Rydberg state electron interacting with an ionic core. The quantum defect correction term for the Rydberg series is associated with the

Techniques

Resonance Ionization Spectroscopy - RIS

The ionization threshold energy of atoms and small molecules are typically larger than the photon energies that are most easily available experimentally. However, it can be possible to span this ionization threshold energy if the photon energy is resonant with an intermediate electronically excited state. While it is often possible to observe the lower Rydberg levels in conventional spectroscopy of atoms and small molecules, Rydberg states are even more important in laser ionization experiments. Laser spectroscopic experiments often involve ionization through a photon energy resonance at an intermediate level, with an unbound final electron state and an ionic core. On resonance for phototransitions permitted by selection rules, the intensity of the laser in combination with the excited state lifetime makes ionization an expected outcome. This RIS approach and variations permit very sensitive detection of specific species.

Low Rydberg Levels and REMPI

For more details on this topic, see REMPI.

High photon intensity experiments can involve multiphoton processes with the absorption of integer multiples of the photon energy. In experiments that involve a multiphoton resonance, the intermediate is often a Rydberg state, and the final state is often an ion. The initial state of the system, photon energy, angular momentum and other selection rules can help in determining the nature of the intermediate state. This approach is exploited in Resonance Enhanced Multiphoton Ionization Spectroscopy (REMPI). An advantage of this spectroscopic technique is that the ions can be detected with almost complete efficiency and even resolved for their mass. It is also possible to gain additional information by performing experiments to look at the energy of the liberated photoelectron in these experiments. (Robert N. Compton [1] formerly of O.R.N.L. and Philip M. Johnson [2] pioneered the development of REMPI.)

Near Threshold Rydberg Levels

The same approach that produces an ionization even can be used to access the dense manifold of near Threshold Rydberg states with laser experiments. Often these experiments involve a laser operating at one wavelength to access the intermediate Rydberg state and a second wavelength laser to access the near Threshold Rydberg state region. Because of the photoabsorption selection rules, these Rydberg electrons are expected to be in a highly elliptical angular momentum states. It is the Rydberg electrons excited to nearly circular angular momentum states that are expected to have the longest lifetimes. The conversion between a highly elliptical and a nearly circular near Threshold Rydberg state might happen in several ways, including encountering small stray electric fields.

ZEKE

Zero Electron Kinetic Energy (ZEKE) was developed with the idea of collecting only the resonance ionization photoelectrons that have extremely low kinetic energy. The technique involves waiting for a period of time after a resonance ionization experiment and then pulsing an electric field to collect the lowest energy photoelectrons in a detector. Typically, ZEKE experiments usually use two different tunable lasers. One laser photon energy is tuned to be resonant with the energy of an intermediate state. (This may be resonant with an excited state at a multiphoton transition.) Another photon energy is tuned to be very close to the ionization threshold energy. The technique worked extremely well and demonstrated energy resolution that was significantly better than the laser bandwidth. It turns out that it was not the photoelectrons that were detected in ZEKE. The delay between the laser and the electric field pulse selected the longest lived and most circular Rydberg states closest to the energy of the ion core. The population distribution of surviving very long-lived near threshold Rydberg states is narrower than the laser energy bandwidth. The electric field pulse stark shifts the near Threshold Rydberg states and vibrational autoionization occurs. ZEKE has provided a significant advance in the study of the vibrational spectroscopy of molecular ions. (Klaus Müller-Dethlefs originated ZEKE spectroscopy.[3])

MATI

Mass Analyzed Threshold Ionization (MATI) was developed with idea of collecting the mass of the ions in a ZEKE experiment. MATI would have offered no advantage if low kinetic photoelectrons were detected. Because MATI also exploits vibrational autoionization of very near Threshold Rydberg states, it also can offer better resolution than the laser bandwidth in addition to allowing unambiguous determination of the mass of the ion. This information can be indispensable in understanding a variety of systems.

PIRI

Photo-Induced Rydberg Ionization (PIRI) was developed following REMPI experiments on electronic autoionization of low-lying Rydberg states of carbon dioxide. In REMPI photoelectron experiments, it was determined that a two-photon ionic core photoabsorption process (followed by prompt electronic autoionization) could dominate the direct single photon absorption in the ionization of some Rydberg states of carbon dioxide. These sorts of two excited electron systems had already been under study in the atomic physics, [4] but there the experiments involved very high order Rydberg states. PIRI works because electronic autoionization can dominate direct photoionization (photoionisation). The circularized near Threshold Rydberg state is more likely to undergo a core photoabsorption than to absorb a photon and directly ionize the Rydberg state. PIRI extends the near Threshold spectroscopic techniques to allow access to the electronic states (including dissociative molecular states and other hard to study systems) as well as the vibrational states of molecular ions.

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