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A 81 4 , Leefer, S. Ferrell, A. Lapierre, A. Nguyen, V. Yashchuk, D. Budker, S. Lamoreaux, and J. Torgerson, A laboratory search for variation of the fine-structure constant using atomic dysprosium, Eur. Special Topics , Tsigutkin, D. Dounas-Frazer, A. Family, J. Stalnaker, V. Mikhail V. Balabas, Todor Karaulanov, Micah P.

Ledbetter, and Dmitry Budker, Polarized alkali vapor with minute-long transverse spin-relaxation time, Phys. Higbie, S. Rochester, B. Patton, R. Bonaccini Calia, D. Acosta, E. Bauch, A. Jarmola, L. Zipp, M. Ledbetter, and D. Budker, Broadband magnetometry by infrared-absorption detection of diamond NV centers, Appl. Damon English, Valeriy V. Review article: D. Budker and M. Romalis, Optical Magnetometry, Nature Physics 3, - Cingoz, A.

Nguyen, N. Lamoreaux, A. Sushkov, and O. Sushkov, On the sensitivity of condensed-matter P- and T-violation experiments, Phys. Stalnaker, D. Software Images icon An illustration of two photographs. Images Donate icon An illustration of a heart shape Donate Ellipses icon An illustration of text ellipses.

Optical Magnetometry Item Preview. EMBED for wordpress. Want more? Field dependence of spin relaxation in a dense Rb vapor. Allred, J. A high-sensitivity atomic magnetometer unaffected by spin-exchange relaxation. Seltzer, S. Unshielded three-axis vector operation of a spin-exchange-relaxation-free atomic magnetometer.

Appelt, S. Light narrowing of rubidium magneticresonance lines in high-pressure optical-pumping cells. A 59 , — Jau, Y. Intense, narrow atomic-clock resonances. Smullin, S. A low-noise high-density alkali metal scalar magnetometer. Stahler, M. Picotesla magnetometry with coherent dark states. Andreeva, C. Two-color coherent population trapping in a single Cs hyperfine transition, with application in magnetometry. B 76 , — Alipieva, E. Coherent population trapping for magnetic field measurements.

SPIE , — Acosta, V. Nonlinear magneto-optical rotation with frequency-modulated light in the geophysical field range. A 73 , Synchronous optical pumping of quantum revival beats for atomic magnetometry. Observation of four-quantum resonance in the Zeeman structure of the ground-state of 39 K. ADS Google Scholar. Yashchuk, V. Selective addressing of high-rank atomic polarization moments. Pustelny, S. Pump-probe nonlinear magnetooptical rotation with frequency-modulated light. Gravrand, O. On the calibration of a vectorial 4 He pumped magnetometer.

Earth Planets Space 53 , — Three-component variometer based on a scalar potassium sensor. Matsko, A. Magnetometer based on the opto-electronic microwave oscillator. Schwindt, P. Self-oscillating rubidium magnetometer using nonlinear magneto-optical rotation.

Higbie, J. Robust, high-speed, all-optical atomic magnetometer. Bechhoefer, J. Feedback for physicists: A tutorial essay on control. Rife, D. Single-tone parameter estimation from discrete-time observations. IEEE Trans. Theory 20 , — Weissman, M. Li, Z. Parametric modulation of an atomic magnetometer. Balabas, M. Magnetometry with millimeter-scale antirelaxation-coated alkali-metal vapor cells.

B 23 , — Chip-scale atomic magnetometer. Influence of magnetic-field inhomogeneity on nonlinear magneto-optical resonances. A 74 , Wildermuth, S. Sensing electric and magnetic fields with Bose-Einstein condensates.

Vengalattore, M. High-resolution magnetometry with a spinor Bose-Einstein condensate. Zhao, K. Evanescent wave magnetometer. Fenici, R. Clinical application of magnetocardiography. Magnetoencephalography theory, instrumentation, and applications to noninvasive studies of the working human brain. Papanicolaou, A. A review of clinical applications of magnetoencephalography.

Livanov, M. The most essential elements of lock-in. The nonlinear Faraday rotation is a very sensitive method for measuring magnetic fields, yet it is limited to weak fields only and cannot be directly extended to fields higher than the widths of the typical resonance. An additional drawback of the method is its limitation to scalar measurements, which yields absolute intensity of the magnetic field but no information on its direction.

Both limitations can be successfully overcome with the Fig. Apparatus for measuring the rotation of a polarization plane in experiments with AM light. DL symbolizes the external-cavity diode help of modulated light. External magnetic field causes rotation of of high-field resonances Fig. If the light modulation is not amplitude comparable to the zero-field resonance. This synchronized with the Larmor precession, after many opens the possibility of applying these resonances for pulses the net birefringence averages to zero in the whole measuring magnetic field of higher intensities.

High-field medium and no NFE signal is observed. However, if the resonances can be created either by using amplitude pulse repetition and the Larmor frequencies are modulation AM [9] or frequency modulation FM [10]. Consequently, the polarization plane of the transmitted light rotates in time and the amplitude reaches its maximum when the modulation and Larmor frequencies are synchronized.

The magneto-optical sample is a glass cell about 2 cm long filled with rubidium atoms isotope 87 Rb. The inner cell walls are coated with an anti- Fig.

Typical rotation signal in the experiment with amplitude relaxation paraffin layer. A semiconductor diode laser is modulation of light intensity. Such measurement can be The authors acknowledge D. Budker, D. Jackson automated if feedback is used to run the magnetometer in Kimball, and M.

Ledbetter for the fruitful discussion. In a self- They would like to express their thankfulness to oscillating magnetometer the rotation signal which D. Budker for the opportunity of presenting Fig.

The oscillates at twice the Larmor frequency is fed back to the work was supported by the Polish Ministry of Science laser intensity modulator. Consequently, the modulation and Higher Education grants NN 33 and NN frequency tracks the Larmor frequency and for each value Then it suffices to measure the oscillation frequency to determine the References magnetic field intensity B.

An alternative to self- oscillating mode is the passive-mode developed in Ref. Faraday, Trans. London , 1 Barczak and S. Pustelny, J. IV , 15 In such a mode, the magnetic-field tracking is [3] W. Gawlik, J.



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