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Sixth Symposium on Novel Optoelectronic Detection Technology and Applications

Improvement of polarization uniformity in spin-exchange relaxation-free comagnetometer based on pump beam reflection compensation

JiaLu Meng, Feng Liu, Xihui Dou, Yuzhuo Pei, Shaowei Lv

Published May 11, 2026• 0 citations
Publisher

Abstract

Spin exchange relaxation free (SERF) comagnetometers, which use coupled alkali metal and noble gas spins, are promising for precision measurements due to their potential for miniaturization and high sensitivity. In these systems, alkali atoms are optically pumped with circularly polarized light, and their polarization is transferred to noble gas nuclei via spin-exchange collisions. However, spatial inhomogeneities in alkali polarization induced by factors such as optical absorption, gas diffusion, and temperature gradients generate effective magnetic field gradients for the noble gas spins. These gradients accelerate spin relaxation and degrade overall sensor performance. This work introduces a pump beam reflection compensation scheme to improve alkali polarization uniformity in a SERF comagnetometer. By retro reflecting the pump beam back along its original optical path with reversed helicity, alkali atoms are repolarized from the opposite direction. This counter propagating beam compensates polarization gradients through reverse optical pumping, thereby homogenizing the effective field experienced by the noble gas spins. The modified pumping configuration enhances spatial uniformity while maintaining a simple and compact sensor architecture. A revised polarization rate model incorporating the retro reflected beam is presented. Simulations comparing single beam, 90% reflection, and total reflection configurations confirm a marked reduction in alkali polarization gradients for reflection based designs. Experimentally, the transverse relaxation time of the noble gas spins is extended by 77.66%, indicating significantly suppressed gradient induced decoherence. The proposed method supports the development of miniaturized, high performance SERF comagnetometers.

DOI
10.1117/12.3108337

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Spin exchange relaxation free (SERF) comagnetometers, which use coupled alkali metal and noble gas spins, are promising for precision measurements due to their potential for miniaturization and high sensitivity. In these systems, alkali atoms are optically pumped with circularly polarized light, and their polarization is transferred to noble gas nuclei via spin-exchange collisions. However, spatial inhomogeneities in alkali polarization induced by factors such as optical absorption, gas diffusion, and temperature gradients generate effective magnetic field gradients for the noble gas spins. These gradients accelerate spin relaxation and degrade overall sensor performance. This work introduces a pump beam reflection compensation scheme to improve alkali polarization uniformity in a SERF comagnetometer. By retro reflecting the pump beam back along its original optical path with reversed helicity, alkali atoms are repolarized from the opposite direction. This counter propagating beam compensates polarization gradients through reverse optical pumping, thereby homogenizing the effective field experienced by the noble gas spins. The modified pumping configuration enhances spatial uniformity while maintaining a simple and compact sensor architecture. A revised polarization rate model incorporating the retro reflected beam is presented. Simulations comparing single beam, 90% reflection, and total reflection configurations confirm a marked reduction in alkali polarization gradients for reflection based designs. Experimentally, the transverse relaxation time of the noble gas spins is extended by 77.66%, indicating significantly suppressed gradient induced decoherence. The proposed method supports the development of miniaturized, high performance SERF comagnetometers.
Ultrasensitive spin exchange relaxation-free (SERF) comagnetometers have been widely applied in various new physics experiments and show great potential for inertial navigation. However, the spatially nonuniform spin polarization of alkali metal (AM) and noble gas (NG) atoms results in an effective magnetic field gradient on the order of 100 nT/cm which is much larger than that is produced by the coils and remanence on the magnitude of 1 nT/cm, thereby reducing the suppression ability of the magnetic noise and limiting the scale factor and noise floor of the comagnetometers. In this study, we establish a model of the effective magnetic field gradient caused by uneven spin polarization and analyze the influencing factors. Our results indicate that optimizing the density ratio of hybrid AM atoms can suppress the effective magnetic field gradient. Nevertheless, the available pump light power imposes a limitation on the density ratio. To further address this issue, we propose a balanced light-assisted hybrid spin exchange optical pumping (HSEOP) method. Our experimental results confirm the effectiveness of the mentioned approach, with 67% suppression of the nuclear transverse relaxation rate and a nearly threefold increase in the scale factor. Furthermore, the optimal density ratio in experimental applications can be reduced from 200 to below 80, thereby overcoming the limitation of laser power in SERF comagnetometers and providing the possibility for wider applications. Finally, the suppression factor of magnetic noise is enhanced by 89% by optimizing the density ratio and the balanced light-assisted HSEOP method. This research sheds light on the fundamental physics experiments and potential for inertial navigation.
Abstract Atomic spin comagnetometers based on the spin-exchange relaxation-free (SERF) effect offer significant potential for inertial sensing and support the development of long-endurance, high-precision navigation technologies. However, limited nuclear spin polarization constrains the long-term stability of these systems. Here, a flat-top optical pumping configuration is introduced for SERF comagnetometers, expanding the uniform-intensity region of the beam to approximately 62 % , which enhances atomic polarization by around 19 % and improves magnetic noise suppression by 32 % . Experimental results demonstrate notable improvements in both sensitivity and long-term stability, highlighting the effectiveness of flat-top beams in overcoming atomic polarization uniformity limitations and advancing SERF co-magnetometer performance.
Alkali metal-noble gas comagnetometers operated in the regime of spin-exchange relaxation-free (SERF) have been widely used in fundamental physics tests and rotation sensing as gyroscope. Spin-exchange relaxation is an important systematic bias of the comagnetometer, which could limit sensitivity significantly. However, the suppression effect of the spin-exchange relaxation has not been examined quantitatively so far. Herein, we systematically investigate the relaxation of the alkali metal atoms and find that the spin-exchange relaxation is not completely eliminated under the normal operating condition of the K-Rb-21Ne comagnetometer. In addition to the optical pumping rate, the spin-exchange relaxation still plays a dominant role in the broadening of electron Zeeman resonances due to the large electron magnetic field. This is the first demonstration that the alkali metal atoms are operated in the near-SERF regime in the alkali metal-noble gas comagnetometer with a large election magnetic field, which will shed light on the way to reduce the relaxation of the alkali metal atoms and enhance the sensitivity of the comagnetometer.
Self-compensated comagnetometers, employing overlapping samples of spin-polarized alkali and noble gases (for example K-3He{}^{3}\mathrm{He}3He) are promising sensors for exotic beyond-the-standard-model fields and high-precision metrology such as rotation sensing. When the comagnetometer operates in the so-called self-compensated regime, the effective field, originating from contact interactions between the alkali valence electrons and the noble-gas nuclei, is compensated with an applied magnetic field. When the comagnetometer begins operation in a given magnetic field, spin-exchange optical pumping establishes an equilibrium between the alkali electron-spin polarization and the nuclear-spin polarization. Subsequently, when the magnetic field is tuned to the compensation point, the spin polarization is brought out of the equilibrium conditions. This causes a practical issue for long measurement times. We report on a method for closed-loop control of the compensation field. This method allows optimization of the operating parameters, especially magnetic field gradients, in spite of the inherently slow (hours to days) dynamics of the system. With the optimization, higher stable nuclear polarization, longer relaxation times, and stronger electron-nuclear coupling are achieved which is useful for nuclear-spin-based quantum memory, spin amplifiers, and gyroscopes. The optimized sensor demonstrates a sensitivity comparable to the best previous comagnetometer but with four times lower noble-gas density. This paves the way for applications in both fundamental and applied science.
The single-beam comagnetometer working in the spin-exchange relaxation-free (SERF) state is being developed into a miniaturized atomic sensor with extremely high precision in rotation measurement. In this paper, we propose a reflective configuration for the single-beam SERF comagnetometer. The laser light simultaneously used for optical pumping and signal extraction is designed to pass through the atomic ensemble twice. In the optical system, we propose a structure composed of a polarizing beam splitter and a quarter-wave plate. With this, the reflected light beam can be separated entirely from the forward propagating one and realize a complete light collection with a photodiode, making the least light power loss. In our reflective scheme, the length of interaction between light and atoms is extended, and because the power of the DC light component is attenuated, the photodiode can work in a more sensitive range and has a better photoelectric conversion coefficient. Compared with the single-pass scheme, our reflective configuration has a stronger output signal and performs better signal-to-noise ratio and rotation sensitivity. Our work has an important impact on developing miniaturized atomic sensors for rotation measurement in the future.
In spin-exchange-relaxation-free (SERF) atomic magnetometers (AMs), the attenuation of circularly polarized pump beam introduces spatial-dependent artificial magnetic fields in atomic spin polarization and light shift. In general, such a spatial-dependent effective magnetic field, especially prevalent in single-cell magnetometer arrays, cannot be uniformly compensated over the entire excitation region, resulting in a complex distributed compensation mask effect. In addition, any external effective-field-compensation methods inevitably complicate the final analysis of the unknown magnetic field measured. Here, we report a new excitation scheme that can substantially suppress spatial nonuniformity due to pump beam attenuation. Using counter-propagating pump beams with symmetrically red- and blue-detuning-paired frequencies, we demonstrate a significant reduction of spatial inhomogeneity in atomic spin polarization and light shift in comparison with the usual single-frequency unidirection and counter-propagating pump schemes. Employing this red-/blue-detuning-paired pump scheme, we construct a single-cell, four-channel SERF magnetometer array with high spatial homogeneity. We demonstrate ~10-fT/Hz1/2^{{1}/{2}}1/2sensitivity in the 5–45-Hz band for all four channels, with a gradient sensitivity of 2 fT/Hz1/21/2^{{1}/{2}}1/2/cm in the same band. This new scheme enables the development of single-vapor-cell, high-uniformity multichannel magnetic field mapping devices with potential applications in magnetoencephalography (MEG) and magnetocardiography (MCG), or in searching for exotic spin-dependent interactions.