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

Interferometry with atoms and molecules

Michael Chapman, Christopher R. Ekstrom, Jörg Schmiedmayer, Troy D. Hammond, Stefan Wehinger, David E. Pritchard

Published May 8, 1994• 1 citation
OpenAlex

Abstract

Three 0.2-μm period diffraction gratings were used to realize an interferometer for atoms and molecules1 that passes the interfering components of the deBroglie wave on opposite sides of a stretched metal foil positioned between two side plates. The foil was 10 cm long and 10 μ.m. thick, and a gas sample of density −2 × 1012 atoms/ cm3 could be introduced on one side of the foil only.

Related papers

Experiments with a separated-beam atom interferometer

David E. Pritchard, Christopher R. Ekstrom, Jörg Schmiedmayer +2 more

Three 0.2 micron period diffraction gratings were combined to realize an atom interferometer1 in which the interfering beams are distinctly separated in both position and momentum. A 10 cm long foil 10 microns thick was positioned symmetrically between two side electrodes, so that the atom wave in the two sides of the interferometer went on opposite sides of it. The fringe amplitude was 820 cps, which allows us to determine the phase to 15 milliradians in 1 minute.2

Annual Meeting Optical Society of America•Jan 1, 1993•7 citations

Matter-wave/atom interferometry

John F. Clauser, Shifang Li

Although interferometry's earliest and most familiar use is with photons, the discovery of matter-wave (deBroglie-wave) interference for electrons demanded the development of quantum mechanics. Since then, matter-wave interferometry has been performed with neutrons, Cooper electron-pairs, and most recently, with whole atoms and diatomic molecules. This talk describes our recent high-flux atom interferometry experiments using the generalized Talbot-vonLau effect. Our interferometer consists of a sequence of three planar vacuum-slit diffraction gratings, microfabricated from silicon nitride membranes. DeBroglie-wave interference fringes are sensed by measuring the transmission of potassium atoms on a hot- wire as a function of grating relative position. Different spatial Fourier components (up to sixth) in the diffraction pattern are resonant in the interferometer at different atomic velocities (i.e., at different wavelengths). When a laser cooled slow atomic beam is incident, various different diffraction patterns are observed as a function of atomic velocity. In an alternative `Heisenberg Microscope' configuration an incident thermal beam produces a velocity average over different fringe Fourier components. AC modulated weak laser light passing through the interferometer interacts selectively with atoms at a specific velocity. The associated fringe pattern is then ac modulated and revealed by its selective destruction.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Dec 12, 1994•0 citations

Atom interferometry

David E. Pritchard, Christopher R. Ekstrom, Jörg Schmiedmayer +2 more

We have constructed an atom interferometer using three 200 nm period transmission gratings. The two interfering portions of each atom’s wave pass on opposite sides of a stretched metal foil. A fringe amplitude of up to 900 cps is observed, which allows us to determine the phase to 15 milliradians in 1 minute. By applying different interactions to the two sides of the interferometer, we have determined the electric polarizability of the ground state of sodium, the coherence length of our beam, and the differential phase shifts and coherences of the different Zeeman ground states in a magnetic field. Some future prospects of separated beam experiments are discussed.

AIP conference proceedings•Jan 1, 1993•0 citations

Interferometry with atoms and molecules: a tutorial

David E. Pritchard, Michael Chapman, Christopher R. Ekstrom +6 more

Since the first interferometers for atoms and molecules were demonstrated in 1991, they have already been applied to measure atomic and molecular properties, to investigate fundamental aspects of quantum mechanics, and to measure inertial motion. This tutorial is designed to introduce those with a vague understanding of optical interferometers to atom interferometry. We outline the basic theory needed to calculate the observed phase shift, indicate how this phase shift is experimentally determined, and then describe how the phase shift is found in two particular cases: phase shifts caused by application of a uniform electric field to atoms on one side of the interferometer, and phase shift arising from the presence of a gaseous medium through which the atom wave on one side of the interferometer must propagate. We illustrate this presentation with a description of our three grating interferometer, including data taken with it.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•May 1, 1997•0 citations

An interferometer for atoms

David W. Keith, Christopher R. Ekstrom, Q. A. Turchette +1 more

We have demonstrated an interferometer for atoms. A three-grating geometry is used, in which the interfering beams are distinctly separated in both position and momentum. We used a highly collimated beam of sodium atoms with a de Broglie wavelength of 16 pm and high-quality 0.4-\ensuremath{\mu}m-period free-standing gratings which we fabricated using a novel method. The interference signal is 70 counts/s, which allows us to determine the phase to 0.1 rad in 1 min. Applications of atom interferometers are briefly discussed.

Physical Review Letters•May 27, 1991•582 citations

Atom Interferometry Progress

David E. Pritchard, Christopher R. Ekstrom, David W. Keith +2 more

Abstract : An atom interferometer is constructed in which the atom waves are physically separated prior to being recombined. Fabricated transmission gratings are used as optical elements for the matter waves. Atom interferometers should be useful in studies of atomic properties, tests of basic quantum physics, for metrology, as rotation sensors, and perhaps ultimately as devices to make ultra- small structures using atom holograms. During the last year our atom interferometer has evolved from a rough plan to an essentially complete device. At present all the major components of the interferometer have been built, and tested at least once. The system will be given its first real try in the next year. Our interferometer consists of three 0.2 microns - period diffraction gratings equally spaced approx. 0.65 m apart in our atomic beam machine. The maximum separation of the beams will be approx. 60 microns. The first two gratings separate and redirect the atomic beam forming a standing wave interference pattern in the atomic flux at the third grating, which acts like a mask to sample this pattern. A principle technical obstacle is the mechanical vibrations of our machine which will blur the interference pattern.

mit•Apr 19, 1990•0 citations
Three 0.2-μm period diffraction gratings were used to realize an interferometer for atoms and molecules1 that passes the interfering components of the deBroglie wave on opposite sides of a stretched metal foil positioned between two side plates. The foil was 10 cm long and 10 μ.m. thick, and a gas sample of density −2 × 1012 atoms/ cm3 could be introduced on one side of the foil only.
Although interferometry's earliest and most familiar use is with photons, the discovery of matter-wave (deBroglie-wave) interference for electrons demanded the development of quantum mechanics. Since then, matter-wave interferometry has been performed with neutrons, Cooper electron-pairs, and most recently, with whole atoms and diatomic molecules. This talk describes our recent high-flux atom interferometry experiments using the generalized Talbot-vonLau effect. Our interferometer consists of a sequence of three planar vacuum-slit diffraction gratings, microfabricated from silicon nitride membranes. DeBroglie-wave interference fringes are sensed by measuring the transmission of potassium atoms on a hot- wire as a function of grating relative position. Different spatial Fourier components (up to sixth) in the diffraction pattern are resonant in the interferometer at different atomic velocities (i.e., at different wavelengths). When a laser cooled slow atomic beam is incident, various different diffraction patterns are observed as a function of atomic velocity. In an alternative `Heisenberg Microscope' configuration an incident thermal beam produces a velocity average over different fringe Fourier components. AC modulated weak laser light passing through the interferometer interacts selectively with atoms at a specific velocity. The associated fringe pattern is then ac modulated and revealed by its selective destruction.
We have constructed an atom interferometer using three 200 nm period transmission gratings. The two interfering portions of each atom’s wave pass on opposite sides of a stretched metal foil. A fringe amplitude of up to 900 cps is observed, which allows us to determine the phase to 15 milliradians in 1 minute. By applying different interactions to the two sides of the interferometer, we have determined the electric polarizability of the ground state of sodium, the coherence length of our beam, and the differential phase shifts and coherences of the different Zeeman ground states in a magnetic field. Some future prospects of separated beam experiments are discussed.
Since the first interferometers for atoms and molecules were demonstrated in 1991, they have already been applied to measure atomic and molecular properties, to investigate fundamental aspects of quantum mechanics, and to measure inertial motion. This tutorial is designed to introduce those with a vague understanding of optical interferometers to atom interferometry. We outline the basic theory needed to calculate the observed phase shift, indicate how this phase shift is experimentally determined, and then describe how the phase shift is found in two particular cases: phase shifts caused by application of a uniform electric field to atoms on one side of the interferometer, and phase shift arising from the presence of a gaseous medium through which the atom wave on one side of the interferometer must propagate. We illustrate this presentation with a description of our three grating interferometer, including data taken with it.
We have demonstrated an interferometer for atoms. A three-grating geometry is used, in which the interfering beams are distinctly separated in both position and momentum. We used a highly collimated beam of sodium atoms with a de Broglie wavelength of 16 pm and high-quality 0.4-\ensuremath{\mu}m-period free-standing gratings which we fabricated using a novel method. The interference signal is 70 counts/s, which allows us to determine the phase to 0.1 rad in 1 min. Applications of atom interferometers are briefly discussed.
Abstract : An atom interferometer is constructed in which the atom waves are physically separated prior to being recombined. Fabricated transmission gratings are used as optical elements for the matter waves. Atom interferometers should be useful in studies of atomic properties, tests of basic quantum physics, for metrology, as rotation sensors, and perhaps ultimately as devices to make ultra- small structures using atom holograms. During the last year our atom interferometer has evolved from a rough plan to an essentially complete device. At present all the major components of the interferometer have been built, and tested at least once. The system will be given its first real try in the next year. Our interferometer consists of three 0.2 microns - period diffraction gratings equally spaced approx. 0.65 m apart in our atomic beam machine. The maximum separation of the beams will be approx. 60 microns. The first two gratings separate and redirect the atomic beam forming a standing wave interference pattern in the atomic flux at the third grating, which acts like a mask to sample this pattern. A principle technical obstacle is the mechanical vibrations of our machine which will blur the interference pattern.