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Journal of Physics B Atomic Molecular and Optical Physics

Longitudinal Stern-Gerlach atomic interferometry using velocity selected atomic beams

Síle Nic Chormaic, V. Wiedeman, Christian Miniatura, Jacques Robert, S. Le Boiteux, V. Lorent, O. Gorceix, S. Feron, J. Reinhardt, J. Baudon

Published Apr 14, 1993• 13 citations
Publisher

Abstract

New experiments have been carried out on a velocity selected beam of H(D)*(2s 1 2/) atoms using a longitudinal Stern-Gerlach atomic interferometer. A large number of fringes of the interference pattern has been observed. The results are in good agreement with theoretical predictions. An application to a topological phaseshift of the Aharonov-Anandan type is given.

DOI
10.1088/0953-4075/26/7/011

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Physical Review A•Feb 10, 2000•13 citations
New experiments have been carried out on a velocity selected beam of H(D)*(2s 1 2/) atoms using a longitudinal Stern-Gerlach atomic interferometer. A large number of fringes of the interference pattern has been observed. The results are in good agreement with theoretical predictions. An application to a topological phaseshift of the Aharonov-Anandan type is given.
As shown recently by Zawisky, Rauch, and Hasegawa in neutron interferometry [Phys. Rev. A 50, 5000 (1994)], the interference pattern obtained with a low-intensity particle beam is deeply modified when a selection is made of the time intervals between successive detected events. Experiments of the same type performed with a Stern-Gerlach interferometer using a metastable hydrogen atom beam are described. Results very similar to those of the neutron experiment are obtained, in particular a strong enhancement of the contrast when large time intervals are selected.
The use of comoving magnetic fields in Stern-Gerlach atom interferometry allows, in principle, one to reach a range of very low kinetic energies (a few tens of neV); it also allows the device to be used as an interference filter for atomic waves. The technique used to produce such fields moving at atomic velocities is described. Experimental interference patterns obtained with a beam of H∗(2S){\mathrm{H}}^{*}(2S)H∗(2S) atoms are in good agreement with the calculations, which clearly demonstrates the feasibility of the method.
By use of a longitudinal Stern-Gerlach polarization atomic device, we have demonstrated the manifestation of a topological phase for a beam of H∗{\mathrm{H}}^{\mathrm{*}}H∗(2s) atoms traveling through a conical magnetic field configuration.
An atom interferometer using two Stern-Gerlach magnets as polariser and analyser is described. The interferometer was first operated with a thermal beam of ground state potassium atoms. In that case the beam splitters are two radio-frequency zones within a transverse homogeneous magnetic field building a coherent superposition of Zeeman states. Ramsey fringes are obtained by scanning the RF-frequency through the resonance profile. Pulsing the RF power allows to get the time-of-flight distribution of the beam. Atomic interference fringes (``Stern-Gerlach fringes'') are observed when the magnitude of an inhomogeneous magnetic field located in between the beam splitters is scanned. When the inhomogeneous field is also pulsed, the scalar Bohm-Aharonov effect is observed. The use of metastable helium atoms (He*23S) in place of potassium atoms is proposed. In addition to the usual advantages provided by metastable atoms of high internal energy, this atom offers the specific advantage to behave as an ideal spin-one particle. This allows us to greatly simplify the polarisation scheme of the interferometer. Possible applications involving transversally inhomogeneous magnetic fields are given and limitations due to the finite source size and angular aperture are discussed.
A quadrupolar static magnetic field used as a phase object in a Stern-Gerlach atom interferometer produces phase shifts proportional to the distance to the zero-field line. As a consequence the transverse intensity profile of the atomic beam beyond the interferometer is modulated by an interference pattern which is a ``phase portrait'' of the field configuration. This pattern---a central bright spot surrounded by annular fringes---can be translated as a whole in any transverse direction by adding a homogeneous field to the quadrupolar field. These effects have been investigated experimentally with a beam of metastable hydrogen atoms H∗(2s),{\mathrm{H}}^{*}(2s),H∗(2s), either by measuring the atom flux through a fixed slit or by scanning the beam profile through a movable hole. The results are in good agreement with the theoretical predictions.