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

arXiv:0704.2299 · Physical Review Letters

One-Dimensional Rydberg Gas in a Magnetoelectric Trap

Michael Mayle, Bernd Hezel, Igor Lesanovsky, Peter Schmelcher

Published Sep 14, 2007• 19 citations
arXivHTMLPDF

Abstract

We study the quantum properties of Rydberg atoms in a magnetic Ioffe-Pritchard trap which is superimposed by a homogeneous electric field. Trapped Rydberg atoms can be created in long-lived electronic states exhibiting a permanent electric dipole moment of several hundred Debye. The resulting dipole-dipole interaction in conjunction with the radial confinement is demonstrated to give rise to an effectively one-dimensional ultracold Rydberg gas with a macroscopic interparticle distance. We derive analytical expressions for the electric dipole moment and the required linear density of Rydberg atoms.

DOI
10.1103/physrevlett.99.113004

Related papers

Interaction-induced stabilization of ultracold Rydberg atoms in a Ioffe-Pritchard trap

Bernd Hezel

Interaction-induced stabilization of ultracold Rydberg atoms in a Ioffe-Pritchard trap — Subject of this thesis is a theoretical investigation of the quantum properties of highly excited atoms in an inhomogeneous magnetic field configuration. It is demonstrated how the large size of the Rydberg atoms alters the coupling to strong magnetic gradients. We find that Rydberg atoms can be tightly trapped in long-lived electronic states. This confinement permits the creation of a one-dimensional Rydberg gas stabilized against auto-ionization by a dipolar repulsion between the atoms, which is generated imposing a homogeneous electric field. This strongly anisotropic interaction is also responsible for a well controllable equilibrium configuration of two Rydberg atoms in the trap whose distance can be changed by tuning the electric field.

•Jan 1, 2010•0 citations

Interaction-induced stabilization of circular Rydberg atoms

Bernd Hezel, Michael Mayle, Peter Schmelcher

We discuss a candidate solution for the controlled trapping and manipulation of two individual Rydberg atoms by means of a magnetic Ioffe-Pritchard trap that is superimposed by a constant electric field. In such a trap Rydberg atoms experience a permanent electric dipole moment that can be of the order of several hundred debye. The interplay of electric dipolar repulsion and three-dimensional magnetic confinement leads to a well controllable equilibrium configuration with tunable trap frequency and atomic distance. We thoroughly investigate the trapping potentials and analyze the interaction-induced stabilization of two such trapped Rydberg atoms. Possible limitations and collapse scenarios are discussed.

arXiv:1106.6275•Physical Review A•Dec 2, 2011•2 citations

Ultracold Rydberg atoms in a Ioffe-Pritchard trap

Bernd Hezel, Igor Lesanovsky, Peter Schmelcher

We discuss the properties of ultracold Rydberg atoms in a Ioffe-Pritchard magnetic field configuration. The derived two-body Hamiltonian unveils how the large size of Rydberg atoms affects their coupling to the inhomogeneous magnetic field. The properties of the compound electronic and center of mass quantum states are thoroughly analyzed. We find very tight confinement of the center of mass motion in two dimensions to be achievable while barely changing the electronic structure compared to the field free case. This paves the way for generating a one-dimensional ultracold Rydberg gas.

arXiv:0705.1299•Physical Review A•Nov 26, 2007•14 citations

Magnetic trapping of ultracold Rydberg atoms in low angular momentum states

Michael Mayle, Igor Lesanovsky, Peter Schmelcher

We theoretically investigate the quantum properties of $nS$, $nP$, and $nD$ Rydberg atoms in a magnetic Ioffe-Pritchard trap. In particular, it is demonstrated that the two-body character of Rydberg atoms significantly alters the trapping properties opposed to pointlike particles with identical magnetic moment. Approximate analytical expressions describing the resulting Rydberg trapping potentials are derived and their validity is confirmed for experimentally relevant field strengths by comparisons to numerical solutions of the underlying Schr\"odinger equation. In addition to the electronic properties, the center-of-mass dynamics of trapped Rydberg atoms is studied. In particular, we analyze the influence of a short-time Rydberg excitation, as required by certain quantum-information protocols, on the center-of-mass dynamics of trapped ground-state atoms. A corresponding heating rate is derived and the implications for the purity of the density matrix of an encoded qubit are investigated.

arXiv:0906.0946•Physical Review A•Nov 12, 2009•17 citations

Controlling Ultracold Rydberg Atoms in the Quantum Regime

Bernd Hezel, Igor Lesanovsky, Peter Schmelcher

We discuss the properties of Rydberg atoms in a magnetic Ioffe-Pritchard trap being commonly used in ultracold atomic physics experiments. The Hamiltonian is derived, and it is demonstrated how tight traps alter the coupling of the atom to the magnetic field. We solve the underlying Schrödinger equation of the system within a given n manifold and show that for a sufficiently large Ioffe field strength the 2n;{2}-dimensional system of coupled Schrödinger equations decays into several decoupled multicomponent equations governing the center of mass motion. An analysis of the fully quantized center of mass and electronic states is undertaken. In particular, we discuss the situation of tight center of mass confinement outlining the procedure to generate a low-dimensional ultracold Rydberg gas.

arXiv:physics/0610194•Physical Review Letters•Nov 29, 2006•24 citations

Rydberg atoms in magnetic quadrupole traps

Igor Lesanovsky, Jörg Schmiedmayer, Peter Schmelcher

We investigate the electronic structure and properties of Rydberg atoms exposed to a magnetic quadrupole field. It is shown that the spatial as well as generalized time-reversal symmetries lead to a two-fold degeneracy of the electronic states in the presence of the external field. A delicate interplay between the Coulomb and magnetic interactions in the inhomogeneous field leads to an unusual weak field splitting of the energy levels as well as complex spatial patterns of the corresponding spin polarization density of individual Rydberg states. Remarkably, the magnetic quadrupole field induces a permanent electric-dipole moment of the atom.

arXiv:physics/0312045•Europhysics Letters (EPL)•Feb 1, 2004•16 citations
We study the quantum properties of Rydberg atoms in a magnetic Ioffe-Pritchard trap which is superimposed by a homogeneous electric field. Trapped Rydberg atoms can be created in long-lived electronic states exhibiting a permanent electric dipole moment of several hundred Debye. The resulting dipole-dipole interaction in conjunction with the radial confinement is demonstrated to give rise to an effectively one-dimensional ultracold Rydberg gas with a macroscopic interparticle distance. We derive analytical expressions for the electric dipole moment and the required linear density of Rydberg atoms.
Interaction-induced stabilization of ultracold Rydberg atoms in a Ioffe-Pritchard trap — Subject of this thesis is a theoretical investigation of the quantum properties of highly excited atoms in an inhomogeneous magnetic field configuration. It is demonstrated how the large size of the Rydberg atoms alters the coupling to strong magnetic gradients. We find that Rydberg atoms can be tightly trapped in long-lived electronic states. This confinement permits the creation of a one-dimensional Rydberg gas stabilized against auto-ionization by a dipolar repulsion between the atoms, which is generated imposing a homogeneous electric field. This strongly anisotropic interaction is also responsible for a well controllable equilibrium configuration of two Rydberg atoms in the trap whose distance can be changed by tuning the electric field.
We discuss a candidate solution for the controlled trapping and manipulation of two individual Rydberg atoms by means of a magnetic Ioffe-Pritchard trap that is superimposed by a constant electric field. In such a trap Rydberg atoms experience a permanent electric dipole moment that can be of the order of several hundred debye. The interplay of electric dipolar repulsion and three-dimensional magnetic confinement leads to a well controllable equilibrium configuration with tunable trap frequency and atomic distance. We thoroughly investigate the trapping potentials and analyze the interaction-induced stabilization of two such trapped Rydberg atoms. Possible limitations and collapse scenarios are discussed.
We discuss the properties of ultracold Rydberg atoms in a Ioffe-Pritchard magnetic field configuration. The derived two-body Hamiltonian unveils how the large size of Rydberg atoms affects their coupling to the inhomogeneous magnetic field. The properties of the compound electronic and center of mass quantum states are thoroughly analyzed. We find very tight confinement of the center of mass motion in two dimensions to be achievable while barely changing the electronic structure compared to the field free case. This paves the way for generating a one-dimensional ultracold Rydberg gas.
We theoretically investigate the quantum properties of nSnSnS, nPnPnP, and nDnDnD Rydberg atoms in a magnetic Ioffe-Pritchard trap. In particular, it is demonstrated that the two-body character of Rydberg atoms significantly alters the trapping properties opposed to pointlike particles with identical magnetic moment. Approximate analytical expressions describing the resulting Rydberg trapping potentials are derived and their validity is confirmed for experimentally relevant field strengths by comparisons to numerical solutions of the underlying Schr\"odinger equation. In addition to the electronic properties, the center-of-mass dynamics of trapped Rydberg atoms is studied. In particular, we analyze the influence of a short-time Rydberg excitation, as required by certain quantum-information protocols, on the center-of-mass dynamics of trapped ground-state atoms. A corresponding heating rate is derived and the implications for the purity of the density matrix of an encoded qubit are investigated.
We discuss the properties of Rydberg atoms in a magnetic Ioffe-Pritchard trap being commonly used in ultracold atomic physics experiments. The Hamiltonian is derived, and it is demonstrated how tight traps alter the coupling of the atom to the magnetic field. We solve the underlying Schrödinger equation of the system within a given n manifold and show that for a sufficiently large Ioffe field strength the 2n;{2}-dimensional system of coupled Schrödinger equations decays into several decoupled multicomponent equations governing the center of mass motion. An analysis of the fully quantized center of mass and electronic states is undertaken. In particular, we discuss the situation of tight center of mass confinement outlining the procedure to generate a low-dimensional ultracold Rydberg gas.
We investigate the electronic structure and properties of Rydberg atoms exposed to a magnetic quadrupole field. It is shown that the spatial as well as generalized time-reversal symmetries lead to a two-fold degeneracy of the electronic states in the presence of the external field. A delicate interplay between the Coulomb and magnetic interactions in the inhomogeneous field leads to an unusual weak field splitting of the energy levels as well as complex spatial patterns of the corresponding spin polarization density of individual Rydberg states. Remarkably, the magnetic quadrupole field induces a permanent electric-dipole moment of the atom.