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

Rydberg states interacting in crossed electric and magnetic fields

S. D. Hogan

Published Jan 1, 2006• 0 citations
OpenAlex

Related papers

Ultra-long-range Rydberg molecules in electric and crossed electric and magnetic fields

Peter Schmelcher, Markus Kurz

Bulletin of the American Physical Society•Jun 5, 2013•0 citations

Rydberg Electrons in Crossed Electric and Magnetic Fields

Jan von Milczewski, T. Uzer

APS•May 1, 1996•0 citations

Rydberg atoms in crossed external magnetic and electric fields: Experimental observation of an outer potential minimum

M. Fauth, HERBERT WALTHER, E. Werner

Zeitschrift für Physik D Atoms Molecules and Clusters•Sep 1, 1987•31 citations

The Atomic Rydberg Spectrum in Crossed Electric and Magnetic Fields: Experimental Evidence of a New Quantization Law

Francis Jean Penent, Dominique Delande, F. Biraben +2 more

Springer series in optical sciences/SPringer series in optical sciences•Jan 1, 1983•0 citations

Rydberg atoms in crossed electric and magnetic fields. Experimental evidence for the Pauli quantization

Francis Jean Penent, Dominique Delande, F. Biraben +1 more

Optics Communications•Mar 1, 1984•35 citations

Rydberg states of helium in electric and magnetic fields of arbitrary relative orientation

Ondřej Tkáč, Matija Žeško, Josef A. Agner +2 more

A spectroscopic study of Rydberg states of helium (n = 30 and 45) in magnetic, electric and combined magnetic and electric fields with arbitrary relative orientations of the field vectors is presented. The emphasis is on two special cases where (i) the diamagnetic term is negligible and both paramagnetic Zeeman and Stark effects are linear (n = 30, B ≤ 120 mT and F = 0-78 V cm⁻¹), and (ii) the diamagnetic term is dominant and the Stark effect is linear (n = 45, B = 277 mT and F = 0-8 V cm⁻¹). Both cases correspond to regimes where the interactions induced by the electric and magnetic fields are much weaker than the Coulomb interaction, but much stronger than the spin-orbit interaction. The experimental spectra are compared to spectra calculated by determining the eigenvalues of the Hamiltonian matrix describing helium Rydberg states in the external fields. The spectra and the calculated energy-level diagrams in external fields reveal avoided crossings between levels of different m ₗ values and pronounced m ₁-mixing effects at all angles between the electric- and magnetic-field vectors other than 0. These observations are discussed in the context of the development of a method to generate dense samples of cold atoms and molecules in a magnetic trap following Rydberg-Stark deceleration.

•Apr 1, 2016•5 citations
A spectroscopic study of Rydberg states of helium (n = 30 and 45) in magnetic, electric and combined magnetic and electric fields with arbitrary relative orientations of the field vectors is presented. The emphasis is on two special cases where (i) the diamagnetic term is negligible and both paramagnetic Zeeman and Stark effects are linear (n = 30, B ≤ 120 mT and F = 0-78 V cm⁻¹), and (ii) the diamagnetic term is dominant and the Stark effect is linear (n = 45, B = 277 mT and F = 0-8 V cm⁻¹). Both cases correspond to regimes where the interactions induced by the electric and magnetic fields are much weaker than the Coulomb interaction, but much stronger than the spin-orbit interaction. The experimental spectra are compared to spectra calculated by determining the eigenvalues of the Hamiltonian matrix describing helium Rydberg states in the external fields. The spectra and the calculated energy-level diagrams in external fields reveal avoided crossings between levels of different m ₗ values and pronounced m ₁-mixing effects at all angles between the electric- and magnetic-field vectors other than 0. These observations are discussed in the context of the development of a method to generate dense samples of cold atoms and molecules in a magnetic trap following Rydberg-Stark deceleration.