Ultraweak magnetic field measurement, as one of the quantum precision measurement techniques, holds important significance in the forefront of explorations in physics and advanced medical technologies. The atomic magnetometer, serving as a typical instrument for measuring extremely weak magnetic fields, utilizes the Larmor precession frequency of electrons in alkali metal atoms to quantify magnetic field magnitudes at subfemtotesla levels. Additionally, atomic magnetometers boast advantages such as high sensitivity, miniaturization and high spatial resolution. Hence, arrays of atomic magnetometer sensors have become a reliable solution for measuring ultraweak magnetic fields in spatial dimensions. This paper proposes an ultracompact and highly sensitive atomic magnetometer array integrated structure via a highly stable polarization volume grating (PVG)-based waveguide structure for beam splitting. Instead of the traditional four polarizing beam splitters and polarizors, the structure integrates parallel beam splitting and polarization conversion functions using PVGs, which are then incorporated into an ultracompact atomic magnetometer array. This integration enables high sensitivity magnetic field measurements in four channels. The light separated by the structure exhibits power fluctuations along a single polarization axis below 0.2% during a 30 min period. The overall volume of the proposed integrated structure is approximately 0.6 cm 3, representing at least an order of magnitude reduction compared to other spatial optical atomic magnetometer array structures. The final validation demonstrates the system can measure magnetic fields on the order of femtotesla, with an average sensitivity of 16.1 fT/Hz 1/2 . This approach holds significant potential for applications in quantum precision sensing, high resolution medical imaging, and biological science exploration.
Ultraweak magnetic field measurement, as one of the quantum precision measurement techniques, holds important significance in the forefront of explorations in physics and advanced medical technologies. The atomic magnetometer, serving as a typical instrument for measuring extremely weak magnetic fields, utilizes the Larmor precession frequency of electrons in alkali metal atoms to quantify magnetic field magnitudes at subfemtotesla levels. Additionally, atomic magnetometers boast advantages such as high sensitivity, miniaturization and high spatial resolution. Hence, arrays of atomic magnetometer sensors have become a reliable solution for measuring ultraweak magnetic fields in spatial dimensions. This paper proposes an ultracompact and highly sensitive atomic magnetometer array integrated structure via a highly stable polarization volume grating (PVG)-based waveguide structure for beam splitting. Instead of the traditional four polarizing beam splitters and polarizors, the structure integrates parallel beam splitting and polarization conversion functions using PVGs, which are then incorporated into an ultracompact atomic magnetometer array. This integration enables high sensitivity magnetic field measurements in four channels. The light separated by the structure exhibits power fluctuations along a single polarization axis below 0.2% during a 30 min period. The overall volume of the proposed integrated structure is approximately 0.6 cm 3, representing at least an order of magnitude reduction compared to other spatial optical atomic magnetometer array structures. The final validation demonstrates the system can measure magnetic fields on the order of femtotesla, with an average sensitivity of 16.1 fT/Hz 1/2 . This approach holds significant potential for applications in quantum precision sensing, high resolution medical imaging, and biological science exploration.
We demonstrate a single-beam atomic magnetometer (AM) capable of measuring a three-axis magnetic field with high-sensitivity, achieved by applying a small DC offset field and a high frequency modulation field. To satisfy the miniaturization demand of AMs, an elliptically polarized light detuned by 50 GHz from the resonance transition center is employed. The circularly polarized component is used to polarize the alkali-metal atoms, while the linearly polarized light is used to detect the dynamics of the polarized spin under a magnetic field. Based on theoretical analysis, parameters that significantly affect the performance are optimized, and a sensitivity of 20 fT/Hz 1/2 in x -axis, 25 fT/Hz 1/2 in y -axis, 30 fT/Hz 1/2 in z -axis is achieved with a miniature 4 × 4 × 4 mm 87 Rb vapor cell. Moreover, we also verify that the operation principle of AMs can be used to null background magnetic fields in-situ with isotropic compensation resolution of 6.7 pT, which provides an effectively precise method for zeroing ambient magnetic field. The high-sensitivity operating of an elliptically-polarized-laser-based magnetometer provides prospective futures for constructing a compact, low-cost AM, which is particularly applicable for non-invasive bio-magnetic imaging such as array-based magnetoencephalography (MEG) and magnetocardiography (MCG).
Atomic magnetometers with magnetic field modulation have emerged as pivotal sensors for biomagnetic measurements. However, challenges such as crosstalk between adjacent modulation fields and the complexity of signal circuitry become increasingly serious in the development of array-based equipment with the magnetometers, especially in the miniaturized atomic magnetometer. This paper proposes an all-optical, fully integrated fiber-coupled atomic magnetometer that employs pump beam modulation. A miniaturized atomic magnetometer with a volume of 10 cm³ has been designed, incorporating an active measurement area of 3 × 3 × 3 mm3. The magnetometer operates in the spinexchange relaxation-free (SERF) regime with an 87Rb vapor cell. An amplitude-modulated pump beam directly modulates the rubidium atomic ensembles, rather than the magnetic field modulation. The optical rotation angle is detected by an unmodulated probe beam oriented orthogonally to the pump beam. In light of the discontinuous pumping characteristics, we developed a modified theoretical model to clarify the output response of the proposed atomic magnetometer. The experimental results demonstrate that the new design achieves the same sensitivity as conventional magnetometer configurations with a smaller volume and without crosstalk of the magnetic field. This research highlights the significant potential for advancing the development of highly sensitive, miniaturized atomic magnetometers, making them particularly suitable for applications in magnetocardiography (MCG) and magnetoencephalography (MEG).
The ultrasensitive magnetometer has a vital importance in fundamental research and applications. Currently, the spin-exchange relaxation-free (SERF) atomic magnetometer has been reported with a sensitivity around the level of fT/Hz 1/2 . To enhance the sensitivity, a gradiometer configuration has usually been introduced to cancel the common-mode noise between two separate channels. However, the signal and response from different channels are not the same due to the attenuation of the pump beam. Here, we proposed a counter-propagating optical sideband pumping method to polarize the atoms, using the electro-optic modulator to modulate the single-pump beam, generating two symmetrically red- and blue-detuned sidebands of frequency. This scheme leads to a significant reduction of undesirable effects coming along with the optical pumping, such as light shifts and spatial inhomogeneity in atomic spin polarization. With the help of this pumping scheme, the two channels have the same magnetic response, and we have built a gradiometer atomic magnetometer with a sensitivity of 0.5 fT/Hz 1/2 ranging from 5 to 40 Hz. Our results propose the possibility of creating larger arrays of atomic magnetometers (AMs) with high sensitivity and spatial resolution based on single-vapor cells for magnetocardiography and magnetoencephalography imaging or searching for exotic spin-dependent interactions.
Abstract The magnetic field is one of the most fundamental and ubiquitous physical observables, carrying information about all electromagnetic phenomena. For the past 30 years, superconducting quantum interference devices (SQUIDs) operating at 4 K have been unchallenged as ultrahigh-sensitivity magnetic field detectors1, with a sensitivity reaching down to 1 fT Hz-1/2 (1 fT = 10-15 T). They have enabled, for example, mapping of the magnetic fields produced by the brain, and localization of the underlying electrical activity (magnetoencephalography). Atomic magnetometers, based on detection of Larmor spin precession of optically pumped atoms, have approached similar levels of sensitivity using large measurement volumes2, 3, but have much lower sensitivity in the more compact designs required for magnetic imaging applications4. Higher sensitivity and spatial resolution combined with non-cryogenic operation of atomic magnetometers would enable new applications, including the possibility of mapping non-invasively the cortical modules in the brain. Here we describe a new spin-exchange relaxation-free (SERF) atomic magnetometer, and demonstrate magnetic field sensitivity of 0.54 fT Hz-1/2 with a measurement volume of only 0.3 cm3. Theoretical analysis shows that fundamental sensitivity limits of this device are below 0.01 fT Hz-1/2. We also demonstrate simple multichannel operation of the magnetometer, and localization of magnetic field sources with a resolution of 2 mm.
Abstract With the development of Spin-Exchange Relaxation Free (SERF) atomic magnetometers, human weak magnetic measurement has become a hot research direction in the medical field. Cardio-cerebromagnetic monitoring is a new medical detection method in the medical field. Array magnetometer is the core device of cardio-cerebromagnetic accurate monitoring. The volume and accuracy of the array magnetometer directly determine the wearability and sensitivity of the device, and the laser beam splitting system has a great influence on its accuracy and volume. Because the diffraction beam splitting method has the advantages of high beam splitting efficiency, good beam performance consistency, small space occupation, etc., it is suitable for the laser beam splitting module of array magnetometer, which does not reduce the accuracy while reducing the volume. In this paper, we innovatively apply the diffraction beam splitting scheme to the laser beam splitting module of the array magnetometer, with the goal of miniaturizing the integration of the beam splitting module and improving the output accuracy of the array magnetometer. The design and fabrication of a high-performance diffraction beam splitter applied to the beam splitting system of the SERF atomic magnetometer, as well as the output beam quality and power balance of multiple laser beams, ensure the detection accuracy of the array magnetometer. It is important to carry out related studies of laser beam splitter technology for magnetometer development.
The SERF atomic magnetometer is nowadays the most sensitive equipment for magnetic field measurement. As used in triaxial magnetic field measurements, however, the weak interaction of the polarized atoms with the magnetic field in the pump light direction results in low sensitivity in that direction. To solve this issue, a single-beam orthogonal pumping triaxial atomic magnetometer based on a double-cell structure is demonstrated. In this paper, we use a beam-splitter to split the pumping light beam equally, so that the proposed triaxial atomic magnetometer can respond to magnetic fields in all three axes simultaneously, and with no sacrifice in sensitivity. The experiments have shown that the magnetometer has a sensitivity of 46fT/Hz1/2on the x-axis, 32fT/Hz1/2on the y-axis, and 40fT/Hz1/2on the z-axis. This magnetometer has great potential for applications where the three components of the magnetic field need to be measured.