Laser & Optoelectronics Progress, Volume. 62, Issue 7, 0700006(2025)

Research Progress and Development Trend of Atomic Magnetometers

Xinran Zong and Haijun Chen*
Author Affiliations
  • National Key Laboratory of Science and Technology on Vacuum Electronics, Beijing Vacuum Electronics Research Institute, Beijing 100015, China
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    Figures & Tables(14)
    Principle of optical pumping atomic magnetometer. (a) Larmor precession occurs when the spin magnetic moment of an electron is deflected by an external magnetic field; (b) alkali metal atom pumping polarization process; (c) the nucleus undergoes Larmor precession in the static magnetic field B.
    Miniaturization and application of optical pumping atomic magnetometer. (a) Photograph of the used vapor cell[20]; (b) photograph of the sensor module, including the main optical components, atomic vapor cell, outer housing, rf coil, electrical wires and optical fibers[20]; (c) microscope image of the micrometer Rb cell[46]; (d) magnetic field distribution measured with the HEDscan system in six different subjects[46]; (e) photograph of the setup inside the MSR, used for both OPM MEG and cryoMEG recordings[46]
    Schematic diagrams of the CPTM theory and apparatus. (a) Three-level atomic system with Λ configuration; (b) schematic diagram of two-photo transitions in the hyperfine structure of D1 line of 87Rb atoms; (c) CPT resonance measurement apparatus
    CPT magnetometer development research. (a) CPTM sensor probe of the National Space Science Center, Chinese Academy of Sciences[62]; (b) its CPTM electronics box[62]; (c) magnetometer experimental facility at China Jiliang University[63]; (d) experimental facility for measuring CPT resonance linewidth in 87Rb gas chamber at Beihang University[64]; (e) CPT signal obtained by VCSEL[64]
    Miniaturization and chip-scale design. (a) Schematic of the magnetic sensor[40]; (b) photograph of the magnetic sensor[40]; (c) optical image of the substrate[66]; (d) the micro-fabricated vapor cell[66]; (e) flexible printed circuit board frame[66]; (f) the printed circuit board with a socket used for interfacing the signal from the physics package[67]; (g) microfabricated vapor cells with the radius size of optical cavity about 2.5 mm[66]; (h) microminiature CPT atomic magnetometer probe[66]; (i) iicro atomic vapor cell[66]; (j) magnetometer performance test[66]
    Measurement of vector magnetic fields. (a) Diagram of the experimental set-up[70]; (b) experimental setup of vector CPT magnetometer[70]; (c) self-fabricated Helmholtz coils on a 3D-printed frame[17]; (d) experimental setup to study the vector magnetic field effects on CPT[71]; (e) experimental schematic of the vector magnetometer using a SCPT resonance in a feedback compensation system[72]
    The coupled dark state magnetometer developed by the Austrian Academy of Sciences established the CDSM flight model for the low Earth orbit China Seismo-Electromagnetic Satellite (CSES) mission[75]
    Schematic diagrams of the SERF magnetometer theory and apparatus. (a) Working principle of SERF atomic magnetometer; (b) schematic diagram of basic experimental device of double beam SERF atomic magnetometer
    Study of long relaxation time. (a) Experimental setup of SERF-like magnetometry in room-temperature environment[84]; (b) relaxation of atomic spins change with different repumping scheme[84]; (c) signal amplitude under different temperatures[84]; (d) rero-field resonance linewidth as a function of the incident power at different temperatures[84]; (e) normalized frequency response curves under different incident optical powers at 160 °C[85]
    Three-axis magnetic field compensation technique. (a)(b) Schematic diagram of the proposed experimental scheme[89]; (c) the practical dual-cell experimental scheme of the three-axis OPM[89]; (d) experimental implementation of the 87Rb magnetometer based on the pump-probe scheme[90]; (e) experimental implementation of the 87Rb magnetometer based on the pump-probe scheme[91]
    MicroSERF zero field vector magnetometer[98]
    Schematic diagram of the NMOR magnetometer apparatus
    Biological weak magnetic signal detection. (a) Spontaneous alpha rhythm signal[109]; (b) the overall arrangement of the practical unshielded MEG system[109]; (c) auditory evoked fields detected unshielded in Earth's field with a portable first-order gradiometer[110]; (d) a picture of the in-the-field MEG recording apparatus with a subject[110]; (e) schematic representation of the NPOM modular system[111]
    • Table 1. Current status of commercial atomic magnetometers

      View table

      Table 1. Current status of commercial atomic magnetometers

      CompanyProductAtomic specieSensitivityDynamic rangeAbsolute accuracyBandwidth
      GEMGSMP-3547K0.0002 nT@1Hz15000‒120000 nT±0.5 nT1 Hz‒20 Hz
      GEMGSMP-2547K0.022 nT@1Hz15000‒120000 nT±0.5 nT1 Hz‒20 Hz
      QuSpinTotal-Field Mag QTFM Gen-248Rb

      Scalar:<3 pT/Hz1/2

      Vector:<0.1 nT/Hz1/2

      1000 nT‒150000 nT500 Hz
      QuSpinZero-Field Mag QTFM Gen-349Rb

      Dual Axis:<15 fT/Hz1/2

      Triax Variant:<23 fT/Hz1/2

      ±5 nT150 Hz
      GeometricsG-822A50Cs0.001 nT/Hz1/220000‒100000 nT<3 nT
      ScintexCS-351Cs0.0006 nT/Hz1/215000‒105000 nT<2.5 nT
      TwinleafOMG52Rb<0.2 pT/Hz1/21‒100 μT
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    Xinran Zong, Haijun Chen. Research Progress and Development Trend of Atomic Magnetometers[J]. Laser & Optoelectronics Progress, 2025, 62(7): 0700006

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    Paper Information

    Category: Reviews

    Received: Nov. 15, 2024

    Accepted: Jan. 2, 2025

    Published Online: Apr. 10, 2025

    The Author Email: Haijun Chen (chenhaijun@cetc.com.cn)

    DOI:10.3788/LOP242262

    CSTR:32186.14.LOP242262

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