Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physical Review Letters

Diabatic Field Ionization of Highly Excited Sodium Atoms

THOMAS H. JEYS, Greg W. Foltz, K. A. Smith, Edward J. Beiting, F. G. Kellert, F. B. Dunning, R. F. Stebbings

Published Feb 11, 1980• 140 citations
Publisher

Abstract

Data demonstrating that, contrary to earlier results, laser-excited sodium Rydberg atoms may pass from low-electric field strengths to ionizing electric field strengths along two quite distinct paths is presented. One path involves predominantly adiabatic passage while the other path involves predominantly diabatic passage. Data are presented along with a model that supports this conclusion.

DOI
10.1103/physrevlett.44.390

Related papers

ELECTRIC FIELD IONIZATION OF SODIUM RYDBERG ATOMS

THOMAS H. JEYS

The outer electron of a Rydberg atom is so weakly bound to the atomic core that a relatively small electric field may cause the electron to be stripped from the atom. The field strength at which this ionization happens is strongly dependent on the state of the Rydberg atom. Pulsed electric field ionization serves, therefore, not only as a means by which a Rydberg atom may be efficiently detected, but also a means by which the state of the Rydberg atom may be analyzed.\nThe first observation of predominantly diabatic passage to field ionization of a non-hydrogenic Rydberg atom has resulted in an improved understanding of the adiabatic and diabatic ionization processes. The magnitudes of the various field ionization features have been measured and found to agree with theory, and by detailed analysis, it is now possible to label the various field ionization signal features with the appropriate (VBAR)m(,l)(VBAR) quantum numbers. A much better understanding of the laser excitation process, the Rydberg state production, and the response of the excited state to an increasing electric field has enabled measurement of some Rydberg fine-structure intervals, through observation of field ionization quantum beats.

•Jan 1, 1982•0 citations

Field ionization of highly excited states of sodium

Thomas F. Gallagher, L. M. Humphrey, William E. Cooke +2 more

We have observed the selective ionization of the degenerate $|{m}_{j}|$ levels of $s$, $p$, and $d$ states of sodium in the range of $n$ from 15 to 20 and have shown that atoms produced in these low-field (\ensuremath{\sim} 10 V/cm) states pass adiabatically from low-field $|{m}_{j}|$ to intermediate-field $|{m}_{l}|$ states. Experiments on the Stark manifold states in intermediate fields (\ensuremath{\sim} 1 kV/cm) and high fields (\ensuremath{\sim} 4 kV/cm) show that the $|{m}_{l}|=0 \mathrm{and} 1$ states pass adiabatically from intermediate- to high-field states and that the passage of the $|{m}_{l}|=2$ states is very nearly adiabatic. These findings suggest a general approach for predicting the threshold fields for ionization of atomic Rydberg states.

Physical Review A•Sep 1, 1977•186 citations

Electric field ionization of highly excited sodium nd atoms

THOMAS H. JEYS, G. B. McMillian, K. A. Smith +2 more

Selective field ionization (SFI) is frequently used to detect atoms in high Rydberg states and to analyze Rydberg population distributions. In order to realize the full potential of this technique, however, a detailed understanding of the behavior of Rydberg atoms during passage from low to ionizing fields is required. The factors influencing this passage are discussed quantitatively and are illustrated by means of detailed SFI data obtained for $\mathrm{Na}34d$ atoms.

Physical Review A•Jul 1, 1982•32 citations

Adiabetic electric field ionization of Sodium Rydberg atoms

G. B. McMillian

Utilizing the technique of high resolution selective field ionization it is possible to observe ionization structure as narrow as 2 V/cm for Na(nS,nD) atoms. Field ionization structure this narrow is characteristic of atoms evolving predominantly adiabatically in a rapidly increasing electric field. By increasing the slew rate of the applied field it is possible to induce departures from the adiabatic path at specific avoided level crossings. These departures result in multiple ionization thresholds which may be explained by arguments based on a simple quantum mechanical model of adiabatic field ionization.

•Jan 1, 1982•0 citations

Study of Rydberg-atom l -changing collisions using selective field ionization

F. G. Kellert, THOMAS H. JEYS, G. B. McMillian +3 more

The excited products of collisions between xenon atoms and $\mathrm{Na}(\mathrm{nd})$ atoms with $n=37$ and $n=42$ have been investigated by use of selective field ionization (SFI). It is observed that, at an ionizing-field slew rate of \ensuremath{\sim} ${10}^{9}$ V/cm sec, most of the collision products follow predominantly diabatic paths to ionization which occurs at field strengths consistent with those predicted by quantum mechanical tunneling calculations. Detailed analysis of the SFI data indicates that the collision products have a wide (possibly complete) range of values of $l$ and ${m}_{j}$, although it is not clear whether the observed distribution results from single or multiple collisions. No evidence of $n$-changing collisions was seen. Similar data for collisions involving $\mathrm{Xe}(\mathrm{nf})$ atoms are briefly discussed.

Physical Review A•Mar 1, 1981•53 citations

ELECTRIC FIELD IONIZATION OF HIGHLY EXCITED RUBIDIUM ATOMS (COLLISIONS, RYDBERG)

G. B. McMillian

A frequency stabilized ring dye laser, with a linewidth of (TURN)250 kHz, has been utilized to selectively excite Rb(N('2)S, N('2)D) states in the range N = 20 - 100 by a two photon process. The highly excited atoms were detected by the technique of electric field ionization. Excited states with (VBAR)M(,L)(VBAR) < 3 have been observed to ionize along predominantly adiabatic paths and states with (VBAR)M(,L)(VBAR) (GREATERTHEQ) 3 have been observed to ionize along predominantly diabatic paths for the range of N investigated. The electric field dependence of the ionization threshold has been determined to be in good agreement with that calculated from a simple model based on the energies and ionization rates of hydrogen.\nCollisions between highly excited rubidium atoms and neutral xenon atoms, which result in a change in the N and L of the excited state of the rubidium atom, have been investigated. The N of the final state has been shown to be limited to those states which lie closest in energy to the initial state, in good agreement with theory. The distribution of L of the final states has been shown to be completely statistical or biased towards production of high L. The distribution of final L is definitely not biased toward production of states with low values of L.

•Jan 1, 1985•0 citations
Data demonstrating that, contrary to earlier results, laser-excited sodium Rydberg atoms may pass from low-electric field strengths to ionizing electric field strengths along two quite distinct paths is presented. One path involves predominantly adiabatic passage while the other path involves predominantly diabatic passage. Data are presented along with a model that supports this conclusion.
The outer electron of a Rydberg atom is so weakly bound to the atomic core that a relatively small electric field may cause the electron to be stripped from the atom. The field strength at which this ionization happens is strongly dependent on the state of the Rydberg atom. Pulsed electric field ionization serves, therefore, not only as a means by which a Rydberg atom may be efficiently detected, but also a means by which the state of the Rydberg atom may be analyzed.\nThe first observation of predominantly diabatic passage to field ionization of a non-hydrogenic Rydberg atom has resulted in an improved understanding of the adiabatic and diabatic ionization processes. The magnitudes of the various field ionization features have been measured and found to agree with theory, and by detailed analysis, it is now possible to label the various field ionization signal features with the appropriate (VBAR)m(,l)(VBAR) quantum numbers. A much better understanding of the laser excitation process, the Rydberg state production, and the response of the excited state to an increasing electric field has enabled measurement of some Rydberg fine-structure intervals, through observation of field ionization quantum beats.
We have observed the selective ionization of the degenerate ∣mj∣|{m}_{j}|∣mj​∣ levels of sss, ppp, and ddd states of sodium in the range of nnn from 15 to 20 and have shown that atoms produced in these low-field (\ensuremath{\sim} 10 V/cm) states pass adiabatically from low-field ∣mj∣|{m}_{j}|∣mj​∣ to intermediate-field ∣ml∣|{m}_{l}|∣ml​∣ states. Experiments on the Stark manifold states in intermediate fields (\ensuremath{\sim} 1 kV/cm) and high fields (\ensuremath{\sim} 4 kV/cm) show that the ∣ml∣=0and1|{m}_{l}|=0 \mathrm{and} 1∣ml​∣=0and1 states pass adiabatically from intermediate- to high-field states and that the passage of the ∣ml∣=2|{m}_{l}|=2∣ml​∣=2 states is very nearly adiabatic. These findings suggest a general approach for predicting the threshold fields for ionization of atomic Rydberg states.
Selective field ionization (SFI) is frequently used to detect atoms in high Rydberg states and to analyze Rydberg population distributions. In order to realize the full potential of this technique, however, a detailed understanding of the behavior of Rydberg atoms during passage from low to ionizing fields is required. The factors influencing this passage are discussed quantitatively and are illustrated by means of detailed SFI data obtained for Na34d\mathrm{Na}34dNa34d atoms.
Utilizing the technique of high resolution selective field ionization it is possible to observe ionization structure as narrow as 2 V/cm for Na(nS,nD) atoms. Field ionization structure this narrow is characteristic of atoms evolving predominantly adiabatically in a rapidly increasing electric field. By increasing the slew rate of the applied field it is possible to induce departures from the adiabatic path at specific avoided level crossings. These departures result in multiple ionization thresholds which may be explained by arguments based on a simple quantum mechanical model of adiabatic field ionization.
The excited products of collisions between xenon atoms and Na(nd)\mathrm{Na}(\mathrm{nd})Na(nd) atoms with n=37n=37n=37 and n=42n=42n=42 have been investigated by use of selective field ionization (SFI). It is observed that, at an ionizing-field slew rate of \ensuremath{\sim} 109{10}^{9}109 V/cm sec, most of the collision products follow predominantly diabatic paths to ionization which occurs at field strengths consistent with those predicted by quantum mechanical tunneling calculations. Detailed analysis of the SFI data indicates that the collision products have a wide (possibly complete) range of values of lll and mj{m}_{j}mj​, although it is not clear whether the observed distribution results from single or multiple collisions. No evidence of nnn-changing collisions was seen. Similar data for collisions involving Xe(nf)\mathrm{Xe}(\mathrm{nf})Xe(nf) atoms are briefly discussed.
A frequency stabilized ring dye laser, with a linewidth of (TURN)250 kHz, has been utilized to selectively excite Rb(N('2)S, N('2)D) states in the range N = 20 - 100 by a two photon process. The highly excited atoms were detected by the technique of electric field ionization. Excited states with (VBAR)M(,L)(VBAR) < 3 have been observed to ionize along predominantly adiabatic paths and states with (VBAR)M(,L)(VBAR) (GREATERTHEQ) 3 have been observed to ionize along predominantly diabatic paths for the range of N investigated. The electric field dependence of the ionization threshold has been determined to be in good agreement with that calculated from a simple model based on the energies and ionization rates of hydrogen.\nCollisions between highly excited rubidium atoms and neutral xenon atoms, which result in a change in the N and L of the excited state of the rubidium atom, have been investigated. The N of the final state has been shown to be limited to those states which lie closest in energy to the initial state, in good agreement with theory. The distribution of L of the final states has been shown to be completely statistical or biased towards production of high L. The distribution of final L is definitely not biased toward production of states with low values of L.