Abstract

In this article, operation of optical magnetometers detecting static (DC) and oscillating (AC) magnetic fields is studied and comparison of the devices is performed. To facilitate the comparison, the analysis is carried out in the same experimental setup, exploiting nonlinear magneto-optical rotation. In such a system, a control over static-field magnitude or oscillating-field frequency provides detection of strength of the DC or AC fields. Polarization rotation is investigated for various light intensities and AC-field amplitudes, which allows to determine optimum sensitivity to both fields. With the results, we demonstrate that under optimal conditions the AC magnetometer is about ten times more sensitive than its DC counterpart, which originates from different response of the atoms to the fields. Bandwidth of the magnetometers is also analyzed, revealing its different dependence on the light power. Particularly, we demonstrate that bandwidth of the AC magnetometer can be significantly increased without strong deterioration of the magnetometer sensitivity. This behavior, combined with the ability to tune the resonance frequency of the AC magnetometer, provide means for ultra-sensitive measurements of the AC field in a broad but spectrally-limited range, where detrimental role of static-field instability is significantly reduced.

Highlights

  • Over the past 15 years, research on magneto-optical phenomena led to the development of various types of optical magnetometers[1]

  • We demonstrated and analyzed the difference in operation of the detection of (quasi-)static (DC) and AC optical magnetometers based on nonlinear magneto-optical rotation

  • The measurements of static and oscillating magnetic fields were performed in the same experimental arrangement under very similar experimental conditions

Read more

Summary

Introduction

Over the past 15 years, research on magneto-optical phenomena led to the development of various types of optical magnetometers[1]. The measurements are carried out in the same experimental arrangement This goal is achieved by application of radio-frequency nonlinear magneto-optical rotation (NMOR)[17,18], i.e., rotation of the polarization plane of linearly polarized, resonant light, propagating through a medium subjected to static and oscillating magnetic fields[19]. In such an arrangement, the strongest polarization rotation is observed when the frequency of the oscillating field is tuned to the frequency splitting of adjacent Zeeman sublevels (the Larmor frequency). Determination of dependences allow us to optimize the performance of the devices

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call