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Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE

Proper temperature for Cs atomic magnetometer

Qiang Liu, Junhai Zhang, Xianjin Zeng, Jiuxing Li, Qingmeng Li, Qiang Huang, Simiao Han, Zongjun Huang, Weimin Sun

Published Nov 18, 2011• 0 citations
Publisher

Abstract

Alkali atomic magnetometer is a good choice for magnetic testing devices with very-high sensitivity. Many parameters could affect the sensitivity of the atomic magnetometer. In this paper we described a Cs atomic magnetometer operating at normal temperature. A circularly polarized pumping light is used to polarize Cs atoms, while a linear polarized probing light is used to test the magneto-caused polarization rotation. During the experiment, we found the temperature is a very important parameter for the signal-to-noise ratio(SNR) enhancement. On the one hand, the higher temperature makes the SNR higher, which is good for sensitivity. On the other hand, the higher temperature causes more frequent collisions between the Cs atoms and the Cs atom and container wall, so that the polarization is easy to be broken, which reduces its sensitivity. So there must be a proper temperature for the high-sensitivity atomic magnetometer. We measured the magnetometer linewidth and sensitivity in the experiment. At optimum temperature the magnetometer achieves magnetic field sensitivity of 3.2pT/Hz1/2.

DOI
10.1117/12.907133

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Alkali atomic magnetometer is a good choice for magnetic testing devices with very-high sensitivity. Many parameters could affect the sensitivity of the atomic magnetometer. In this paper we described a Cs atomic magnetometer operating at normal temperature. A circularly polarized pumping light is used to polarize Cs atoms, while a linear polarized probing light is used to test the magneto-caused polarization rotation. During the experiment, we found the temperature is a very important parameter for the signal-to-noise ratio(SNR) enhancement. On the one hand, the higher temperature makes the SNR higher, which is good for sensitivity. On the other hand, the higher temperature causes more frequent collisions between the Cs atoms and the Cs atom and container wall, so that the polarization is easy to be broken, which reduces its sensitivity. So there must be a proper temperature for the high-sensitivity atomic magnetometer. We measured the magnetometer linewidth and sensitivity in the experiment. At optimum temperature the magnetometer achieves magnetic field sensitivity of 3.2pT/Hz1/2.
The basic principle of atomic magnetometer is to measure the precession frequency of polarized atomic spins in a magnetic field. The paper describes the optical pump, probe process and spin relaxation mechanisms. The magnetometer based on Cs atom is demonstrated in the experiment. At normal temperature 30°C the magnetometer achieves 8nT magnetic resonance widths and magnetic field sensitivity of 4.8pT/Hz1/2. It is more convenient for miniature structure design due to operate in lower temperature.
The paper describes a new magnetometer with Cs vapor in the spin exchange relaxation free (SERF) regime. Because cesium atom has a higher saturated vapor pressure than other alkali metallic atoms, so the magnetometer has required lower operated temperature. We have discussed the effect of different pumping intensities on the polarization and the pumping rate at 105°C in theory; and the result shows out the magnetometer will have maximum sensitivity when the pumping intensity is 52mW/cm2. Taking into account all relaxations including collision relaxations, diffusion relaxation and pumping relaxation from pump light, we find the relaxation rate will be about 6Hz for the cesium magnetometer with SERF.
Abstract The polarization of light affected by the birefringence of optical elements, such as vapor cell walls, mirrors, and windows, may introduce systematic errors that can be minimized by precisely measuring and correcting the light polarization with a highly sensitive atomic polarimeter. In high precision measurements, it is necessary to measure the light polarization with a high precision where the light interacts with atoms. However, it is inconvenient or even impossible to use the presented method to measure the light polarization, for example, in a cell or cavity. We present a precise and relatively straightforward method to measure the light polarization based on a cesium (Cs) atomic magnetometer configuration. The pump-probe scheme is involved in our experiment. The pump light polarizes atomic spins and the probe light measures the spins polarization. The optical rotation of the probe light significantly depends on the pump light ellipticity, which can be used to measure the light polarization with a high precision. In our work, we present a method to measure the pump light ellipticity with a sensitivity of 2.1 × 10 −8 rad Hz −1/2 for linearly polarized light, which has approximately an order of magnitude improvement than previous research results.
In order to availably solve the crosstalk of the traditionally optically pumped magnetometer,in which an oscillating magnetic field drives transitions between Zeeman magnetic sublevels,an all-optical cesium(Cs)atomic magnetometer based on Bell-Bloom structure has been investigated and demonstrated experimentally in this paper.When there is an external magnetic field,by analyzing the Larmor precession spectrum of the polarized ground state atoms induced by a modulated pump laser,the atomic magnetometer with high sensitivity is achieved.First,we present the operating principle of the magnetometer with amplitude modulation and set up the experimental system by means of a three-layer magnetic shield.Then in the case of 100 nT field by optimizing the experimental parameters,i.e.,the frequency and intensity of the pump laser,we have obtained the atomic precession spectrum with line width(full width at half maximum)of 22 Hz and signal noise ratio(SNR)of 3.2×104 per unit hertz band width,and then have evaluated the magnetometer with an intrinsic sensitivity of 100fT/Hz1/2 and spatial resolution smaller than 1.2cm,while the experimentally closed loop test shows that the cesium atomic magnetometer would have the sensitivity of 120fT/Hz1/2 and response time of 300 ms.
A cesium atomic magnetometer based on laser-pumped rf resonance has been investigated and demonstrated experimentally. Atoms are polarized and pumped to dark states by circularly polarized light. When there exists a magnetic field, the corresponding magnetization will be precessing around the magnetic field at Larmor frequency. By means of adding a resonant rf magnetic field, the atoms will be depolarized and absorb photons again. By detecting the spectrum of the transmitted light, one can obtain the information about the external magnetic field. We build an 894nm external cavity diode laser with a frequency stabilization device, and a low noise magnetic field measurement environment. After the optimization of the magnetometer parameter and closed-loop measurement, an ultimate sensitivity of 19 fT/Hz1/2 and an intrinsic sensitivity of 1.8 pT/Hz1/2 have been achieved with the spatial resolution smaller than 2 cm.
We report a rubidium atomic magnetometer based on pump-probe nonlinear magneto-optical rotation. The rubidium vapor cell is placed in a five-layer magnetic shield with inner coils that can generate uniform magnetic fields along the direction of pump beam, and the cell is also placed in the center of a Helmholtz coil that can generate an oscillating magnetic field perpendicular to the direction of pump beam. The atoms are optically pumped by circularly polarized pump beam along a constant magnetic field in a period of time, then the pump beam is turned off and a /2 pulse of oscillating magnetic field for 87Rb atoms is applied. After the above process, the individual atomic magnetic moments become phase coherent, resulting in a transverse magnetization vector precessing at the Larmor frequency in the magnetic field. The linearly polarized probing beam is perpendicular to the direction of magnetic field, and can be seen as a superposition of the left and right circularly polarized light. Because of the different absorptions and dispersions of the left and right circularly polarized light by rubidium atoms, the polarization direction of probing beam rotates when probing beam passes through rubidium vapor cell. The rotation of the polarization is subsequently converted into an electric signal through a polarizing beam splitter. Finally, the decay signal related to the transverse magnetization vector is measured. The Larmor frequency proportional to magnetic field is obtained by the Fourier transform of the decay signal. The value of magnetic field is calculated from the formula:B=(2/) f, where and f are the gyromagnetic ratio and Larmor frequency, respectively. In order to measure the magnetic field in a wide range, the tracking lock mode is proposed and tested. The atomic magnetometer can track the magnetic field jump of 1000 nT or 10000 nT, indicating that the atomic magnetometer has strong locking ability and can be easily locked after start-up. The main performances in different magnetic fields are tested. The results show that the measurement range of the atomic magnetometer is from 100 nT to 100000 nT, the extreme sensitivity is 0.2 pT/Hz1/2, and the magnetic field resolution is 0.1 pT. The transverse relaxation times of the transverse magnetization vector in different magnetic fields are obtained, and the relaxation time decreases with the increase of the magnetic field. When the measurement range is from 5000 nT to 100000 nT, the magnetic field sampling rate of the atomic magnetometer can be adjusted in a range from 1 Hz to 1000 Hz. The atomic magnetometer in high sampling rate can measure weak alternating magnetic field at low frequency. This paper provides an important reference for developing the atomic magnetometer with large measurement range, high sensitivity and high sampling rate.