Magnetometry with a space-based differential atom interferometer
Fig. 2, panel (a)
Atom paths in the $x$-$z$ plane, $z$ (mm) against $x$ (mm): the Bragg beam centre line (dashed), the in-trap transport (solid) from the evaporation trap (diamond) to the release trap (square), and the $m_{\mathrm{F}} = 2$ and $m_{\mathrm{F}} = 0$ trajectories (dotted). Not hosted: the chip, the beam profile shading, the solid interferometry segments and the inset (b).
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- Data: data.csv
Provenance
This panel was computed from the authors' public data deposit (Nature Communications Source Data: https://doi.org/10.1038/s41467-026-75230-2, CC BY 4.0). The plot shown here is re-rendered for interactive viewing and analysis. See the paper for the original figure and full scientific context.
License: CC BY 4.0.
Nat. Commun. 17, 6089 (2026) · DOI: 10.1038/s41467-026-75230-2 · arXiv: 2505.23532
Other panels of Fig. 2: (c) (d)
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