{ "id": "1802.03845", "version": "v1", "published": "2018-02-12T00:16:36.000Z", "updated": "2018-02-12T00:16:36.000Z", "title": "Improved sensitivity to magnetic fields by rotation of quantum sensors", "authors": [ "A. A. Wood", "A. G. Aeppli", "E. Lilette", "Y. Y. Fein", "A. Stacey", "L. C. L. Hollenberg", "R. E. Scholten", "A. M. Martin" ], "comment": "7 pages, 4 figures", "categories": [ "quant-ph" ], "abstract": "Magnetic sensors are typically much more sensitive to oscillating (AC) magnetic fields than static (DC) fields, due to the presence of more noise at lower frequency, typically scaling with a $1/f$ dependence. For quantum magnetometers, this characteristic noise is reflected in the ensemble dephasing time $T_2^*$, the relevant sensing time for a DC field, being much lower than the spin coherence time $T_2$, which determines the sensitivity to AC fields. Here, we demonstrate measurement of DC magnetic fields using a physically rotating ensemble of nitrogen-vacancy centres at a precision limited by the electron spin coherence time, $T_2$. We rotate the host diamond with a period comparable to $T_2$, such that the angle between the NV axis and the magnetic field to be detected changes as a function of time, upconverting the static magnetic field to an oscillating field in the physically rotating frame. Using spin-echo interferometry, we observe an order of magnitude improvement in DC magnetometer response compared to a conventional Ramsey experiments. Enhancements to our scheme could realise DC sensitivities equivalent to demonstrated AC magnetic field sensitivities with NV centres.", "revisions": [ { "version": "v1", "updated": "2018-02-12T00:16:36.000Z" } ], "analyses": { "keywords": [ "sensitivity", "quantum sensors", "demonstrated ac magnetic field sensitivities", "electron spin coherence time", "realise dc sensitivities equivalent" ], "note": { "typesetting": "TeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable" } } }