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

AIP conference proceedings

Coherent Atom Optics with fast metastable rare gas atoms

Jules Grucker, J. Baudon, J.‐C. Karam, F. Perales, Valerij Bočvarski, G. Vassilev, M. Ducloy

Published Jan 1, 2006• 1 citation
Publisher

Abstract

Coherent atom optics experiments making use of an ultra‐narrow beam of fast metastable atoms generated by metastability exchange are reported. The transverse coherence of the beam (coherence radius of 1.7 μm for He*, 1.2 μm for Ne*, 0.87 μm for Ar*) is demonstrated via the atomic diffraction by a non‐magnetic 2μm‐period reflection grating. The combination of the non‐scalar van der Waals (vdW) interaction with the Zeeman interaction generated by a static magnetic field gives rise to “vdW‐Zeeman” transitions among Zeeman sub‐levels. Exo‐energetic transitions of this type are observed with Ne*(3P2) atoms traversing a copper micro‐slit grating. They can be used as a tunable beam splitter in an inelastic Fresnel bi‐prism atom interferometer.

DOI
10.1063/1.2406011

Related papers

A slowed coherent atomic beam as a new source for atomic interferometry

M. Hamamda, G. Dutier, Valerij Bočvarski +4 more

The paper presents an experiment based on an efficient coupling between atomic Zeeman states (for atoms with internal angular momentum) allowed by the quadrupolar component of the surface- induced van der Waals (vdW) interaction. This exo-energetic "vdW - Zeeman" transition provides a tuneable (magnetic field intensity dependent) beam splitter that was theoretically illustrated by the simplest possible interferometer: an atomic counterpart of Fresnel biprism. The velocity - adjustable atomic beam is here coming across two opposite surfaces (single slit of a nano-grating). For a transverse coherent radius large enough, the atom wave packet is strongly inelastically diffracted by the two opposite surfaces at some distances from the slit to yield non localised interference fringes. The calculation has been done for Ar metastable atoms with a grating of 100 nm period and different velocities of the atoms (560 to 10 m/s). Via the interference pattern (Schlieren image), this device should give access to such novel information as the oscillating part of the complex vdW - interaction transition amplitude. This simplest configuration is not sensitive to inertial effect. As a next step, a loop - closing transmission grating was added to realize a new type of compact interferometer.

Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)•Jun 1, 2009•0 citations

Atom diffraction with a ‘natural’ metastable atom nozzle beam

J.‐C. Karam, N Wipf, Jules Grucker +7 more

The resonant metastability-exchange process is used to obtain a metastable atom beam with intrinsic properties close to those of a ground-state atom nozzle beam (small angular aperture, narrow velocity distribution). The estimated effective source diameter (15 µm) is small enough to provide at a distance of 597 mm a transverse coherence radius of about 873 nm for argon, 1236 nm for neon and 1660 nm for helium. It is demonstrated both by experiment and numerical calculations with He*, Ne* and Ar* metastable atoms, that this beam gives rise to diffraction effects on the transmitted angular pattern of a silicon-nitride nano-slit grating (period 100 nm). Observed patterns are in good agreement with previous measurements with He* and Ne* metastable atoms. For argon, a calculation taking into account the angular aperture of the beam (0.35 mrad) and the effect of the van der Waals interaction—the van der Waals constant C 3 = 1.83 +0.1 −0.15 au being derived from spectroscopic data—leads to a good agreement with experiment.

Journal of Physics B Atomic Molecular and Optical Physics•Jul 18, 2005•21 citations

Coherent Atom Optics With Fast Metastable Beams: Metastable Helium Diffraction By 1D and 2D Magnetized Reflection Gratings

Jules Grucker, J. Baudon, J.‐C. Karam +3 more

1D and 2D reflection gratings (Permalloy stripes or dots deposited on silicon), immersed in an external homogeneous static magnetic field, are used to study 1D and 2D diffraction of fast metastable helium atoms He* (23S1). Both the grazing incidence used here and the repulsive potential (for sub‐level m = −1) generated by the magnetisation reduce the quenching effect. This periodically structured potential is responsible for the diffraction in the incidence plane as well as for the diffraction in the perpendicular plane.

AIP conference proceedings•Jan 1, 2007•0 citations

Production of a slow, monoenergetic metastable neon beam for atom diffraction studies

Andrew Palmer, Joshua P. Beardmore, Timothy John Hourigan +2 more

We present characterization results from a series of atom-optical elements designed to produce a slow, monochromatic metastable neon atomic beam source.These elements include a two dimensional optical collimator, a Zeeman slower and a hexapole magnetic bender.The beam will be diffracted from various gratings for studies of the van der Waals forces governing atom-surface interactions.

•Jan 1, 2006•0 citations

Van der Waals - Zeeman transitions of slow metastable argon atoms Ar*(3P2)

M. Hamamda, Thierry Taillandier-Loize, F. Perales +4 more

Metastable argon atoms Ar*(3P2), produced by electron bombardment of a nozzle beam of ground state Ar atoms, are slowed down from their initial thermal velocity of 560 m/s down to a few tens of m/s, using a standard Zeeman slower. In this decelerator, a repulsive force is induced by a counter-propagating σ+- polarized laser beam, locked in frequency on the3P2-3D3closed transition (λ= 811.5 nm) and then detuned by 340 MHz. A special profile of longitudinal magnetic field is adjusted in order to maintain atoms in resonance with light all over the device, by compensating the variable Doppler shift by the convenient Zeeman shift. Low velocities, e.g. 55 m/s, are accessible but due to spontaneous emission randomly distributed recoil momentums enlarge both angular and velocity distributions of the beam. Nevertheless, by placing off axis collimating slits and grating, it is in principle possible to observe transmission and/or diffraction phenomena specific of low velocities.

Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)•May 1, 2011•0 citations

Young’s double-slit experiment with atoms: A simple atom interferometer

O. Carnal, J. Mlynek

An atomic interferometer based on a Young's-type double-slit arrangement has been demonstrated. A supersonic beam of metastable helium atoms passes through a 2-\ensuremath{\mu}m-wide slit in a thin gold foil. This transversely coherent beam impinges on a second microfabricated transmission structure, consisting of two 1-\ensuremath{\mu}m-wide slits at a lateral distance of 8 \ensuremath{\mu}m. This double slit defines two possible paths on which the atoms can reach the detector slit. The good visibility of the observed fringes should make it possible to measure differential phase shifts in the interferometer of 1/3 rad in less than 10 min.

Physical Review Letters•May 27, 1991•627 citations
Coherent atom optics experiments making use of an ultra‐narrow beam of fast metastable atoms generated by metastability exchange are reported. The transverse coherence of the beam (coherence radius of 1.7 μm for He*, 1.2 μm for Ne*, 0.87 μm for Ar*) is demonstrated via the atomic diffraction by a non‐magnetic 2μm‐period reflection grating. The combination of the non‐scalar van der Waals (vdW) interaction with the Zeeman interaction generated by a static magnetic field gives rise to “vdW‐Zeeman” transitions among Zeeman sub‐levels. Exo‐energetic transitions of this type are observed with Ne*(3P2) atoms traversing a copper micro‐slit grating. They can be used as a tunable beam splitter in an inelastic Fresnel bi‐prism atom interferometer.
The paper presents an experiment based on an efficient coupling between atomic Zeeman states (for atoms with internal angular momentum) allowed by the quadrupolar component of the surface- induced van der Waals (vdW) interaction. This exo-energetic "vdW - Zeeman" transition provides a tuneable (magnetic field intensity dependent) beam splitter that was theoretically illustrated by the simplest possible interferometer: an atomic counterpart of Fresnel biprism. The velocity - adjustable atomic beam is here coming across two opposite surfaces (single slit of a nano-grating). For a transverse coherent radius large enough, the atom wave packet is strongly inelastically diffracted by the two opposite surfaces at some distances from the slit to yield non localised interference fringes. The calculation has been done for Ar metastable atoms with a grating of 100 nm period and different velocities of the atoms (560 to 10 m/s). Via the interference pattern (Schlieren image), this device should give access to such novel information as the oscillating part of the complex vdW - interaction transition amplitude. This simplest configuration is not sensitive to inertial effect. As a next step, a loop - closing transmission grating was added to realize a new type of compact interferometer.
The resonant metastability-exchange process is used to obtain a metastable atom beam with intrinsic properties close to those of a ground-state atom nozzle beam (small angular aperture, narrow velocity distribution). The estimated effective source diameter (15 µm) is small enough to provide at a distance of 597 mm a transverse coherence radius of about 873 nm for argon, 1236 nm for neon and 1660 nm for helium. It is demonstrated both by experiment and numerical calculations with He*, Ne* and Ar* metastable atoms, that this beam gives rise to diffraction effects on the transmitted angular pattern of a silicon-nitride nano-slit grating (period 100 nm). Observed patterns are in good agreement with previous measurements with He* and Ne* metastable atoms. For argon, a calculation taking into account the angular aperture of the beam (0.35 mrad) and the effect of the van der Waals interaction—the van der Waals constant C 3 = 1.83 +0.1 −0.15 au being derived from spectroscopic data—leads to a good agreement with experiment.
1D and 2D reflection gratings (Permalloy stripes or dots deposited on silicon), immersed in an external homogeneous static magnetic field, are used to study 1D and 2D diffraction of fast metastable helium atoms He* (23S1). Both the grazing incidence used here and the repulsive potential (for sub‐level m = −1) generated by the magnetisation reduce the quenching effect. This periodically structured potential is responsible for the diffraction in the incidence plane as well as for the diffraction in the perpendicular plane.
Metastable argon atoms Ar*(3P2), produced by electron bombardment of a nozzle beam of ground state Ar atoms, are slowed down from their initial thermal velocity of 560 m/s down to a few tens of m/s, using a standard Zeeman slower. In this decelerator, a repulsive force is induced by a counter-propagating σ+- polarized laser beam, locked in frequency on the3P2-3D3closed transition (λ= 811.5 nm) and then detuned by 340 MHz. A special profile of longitudinal magnetic field is adjusted in order to maintain atoms in resonance with light all over the device, by compensating the variable Doppler shift by the convenient Zeeman shift. Low velocities, e.g. 55 m/s, are accessible but due to spontaneous emission randomly distributed recoil momentums enlarge both angular and velocity distributions of the beam. Nevertheless, by placing off axis collimating slits and grating, it is in principle possible to observe transmission and/or diffraction phenomena specific of low velocities.
An atomic interferometer based on a Young's-type double-slit arrangement has been demonstrated. A supersonic beam of metastable helium atoms passes through a 2-\ensuremath{\mu}m-wide slit in a thin gold foil. This transversely coherent beam impinges on a second microfabricated transmission structure, consisting of two 1-\ensuremath{\mu}m-wide slits at a lateral distance of 8 \ensuremath{\mu}m. This double slit defines two possible paths on which the atoms can reach the detector slit. The good visibility of the observed fringes should make it possible to measure differential phase shifts in the interferometer of 1/3 rad in less than 10 min.