Abstract

We present here the current status of our high-sensitivity gravity-gradiometer based on atom interferometry. In our apparatus, two clouds of laser-cooled rubidium atoms are launched in a fountain configuration and simultaneously interrogated by a Raman-pulse interferometry sequence. The system has recently been upgraded and its stability re-evaluated. We also discuss the recent progress of the experiment towards a precise determination of the Newtonian gravitational constant G. The signal-to-noise ratio and the long-term stability of the gravity gradiometer demonstrated interesting perspectives for pushing the G measurement precision below the 100 ppm level.

Highlights

  • We present here the current status of our high-sensitivity gravitygradiometer based on atom interferometry

  • In order to characterize the apparatus, we tested the sensitivity of the gravity gradiometer and its long-term stability

  • We presented a sensitive gravity gradiometer based on Raman atom interferometry

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Summary

Principle of measurement

A detailed description of the MAGIA experiment can be found in the previous papers [14, 16, 31, 42] and references therein. We use atom interferometry to perform a simultaneous measurement of the differential acceleration experienced by two clouds of cold rubidium atoms in the presence of a well-characterized set of source masses. In a Raman interferometry-based gravimeter, atoms in an atomic fountain are illuminated by a sequence of light pulses that split, redirect and recombine the atomic wave packets. In the presence of a gravity field, atoms experience a phase shift φ = keffgT 2 depending on the local gravitational acceleration g and on the time interval T between the Raman pulses [2]. Two spatially separated atomic clouds in free fall along the same vertical axis are simultaneously interrogated by the same Raman beams to provide a measurement of the differential acceleration induced by gravity on the two samples

Experimental apparatus
The Raman laser system
Experimental results
Influence of Raman laser power
Influence of atomic flux
Gradiometer sensitivity
Conclusions
Full Text
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