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      The polarization and the fundamental sensitivity of \(^{\text{39}}\)K (\(^{\text{133}}\)Cs)-\(^{\text{85}}\)Rb-\(^{\text{4}}\)He hybrid optical pumping spin exchange relaxation free atomic magnetometers

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          Abstract

          The hybrid optical pumping spin exchange relaxation free (SERF) atomic magnetometers can realize ultrahigh sensitivity measurement of magnetic field and inertia. We have studied the \(^{\text{85}}\)Rb polarization of two types of hybrid optical pumping SERF magnetometers based on \(^{\text{39}}\)K-\(^{\text{85}}\)Rb-\(^{\text{4}}\)He and \(^{\text{133}}\)Cs-\(^{\text{85}}\)Rb-\(^{\text{4}}\)He (\(^{\text{39}}\)K (\(^{\text{133}}\)Cs)-\(^{\text{85}}\)Rb-\(^{\text{4}}\)He, then found that the polarization of \(^{\text{85}}\)Rb varies with the number density of buffer gas (\(^{\text{4}}\)He) and quench gas (N\(_{\text{2}}\)), the optical pumping rate of pump beam (\(^{\text{39}}\)K and \(^{\text{133}}\)Cs) and cell temperature respectively, which will provide an experimental guide for the design of the hybrid optical pumping SERF magnetometer. We obtain a general formula on the fundamental sensitivity of the hybrid optical pumping SERF magnetometer due to the shot-noise of a probe laser, which describes that the fundamental sensitivity of the magnetometer varies with the cell effective radius, the number density of buffer gas and quench gas, the optical pumping rate of pump beam (\(^{\text{39}}\)K and \(^{\text{133}}\)Cs), probe relaxation rate, external magnetic field, measurement volume, cell temperature and measurement time. We obtain a highest fundamental sensitivity of \(25.438 aT/Hz^{1/2}\) (\(1 aT=10^{-18} T\)) with \(^{\text{39}}\)K-\(^{\text{85}}\)Rb-\(^{\text{4}}\)He magnetometer among above two types of magnetometers when the polarization of \(^{\text{85}}\)Rb atom is \(% 0.0121\). Optimizing the magnetometer parameters is advantageous to improve the sensitivity of the hybrid optical pumping SERF magnetometer in measuring weak magnetic field. We estimate the fundamental sensitivity limit of the hybrid optical pumping SERF magnetometer to be superior to \(1.847\times10^{-2} aT/Hz^{1/2}\).

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          Precision measurement of magnetic field based on the transient process in a K-Rb-21Ne co-magnetometer.

          We demonstrate a novel method of measuring magnetic field based on the transient signal of the K-Rb- 21 Ne co-magnetometer operating in nuclear spin magnetization self-compensation magnetic field regime. The operation condition for self-compensation magnetic field by nuclear spin magnetization of 21 Ne in steady state is presented. We characterize the dynamics of the coupled spin ensembles by a set of Bloch equations, and formulate the expression of transient output signal. After verifying the stability of this method, the measurement range and error are studied. This method is also verified to be valid in various temperature and pumping light power density.
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            Optimal densities of alkali metal atoms in an optically pumped K-Rb hybrid atomic magnetometer considering the spatial distribution of spin polarization.

            An optically pumped K-Rb hybrid atomic magnetometer can be a useful tool for biomagnetic measurements due to the high spatial homogeneity of its sensor property inside a cell. However, because the property varies depending on the densities of potassium and rubidium atoms, optimization of the densities is essential. In this study, by using the Bloch equations of K and Rb and considering the spatial distribution of the spin polarization, we confirmed that the calculation results of spin polarization behavior are in good agreement with the experimental data. Using our model, we calculated the spatial distribution of the spin polarization and found that the optimal density of K atoms is 3 × 1019 m-3 and the optimal density ratio is nK/nRb ~ 400 to maximize the output signal and enhance spatial homogeneity of the sensor property.
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              Far off-resonance laser frequency stabilization using multipass cells in Faraday rotation spectroscopy.

              We propose a far off-resonance laser frequency stabilization method by using multipass cells in Rb Faraday rotation spectroscopy. Based on the detuning equation, if multipass cells with several meters optical path length are used in the conventional Faraday spectroscopy, the detuning of the lock point can be extended much further from the alkali metal resonance. A plate beam splitter was used to generate two different Faraday signals at the same time. The transmitted optical path length was L=50  mm and the reflected optical path length was 2L=100  mm. When the optical path length doubled, the detuning of the lock points moved further away from the atomic resonance. The temperature dependence of the detuning of the lock point was also analyzed. A temperature-insensitive lock point was found near resonance when the cell temperature was between 110°C and 130°C. We achieved an rms fluctuation of 0.9 MHz/23 h at a detuning of 0.5 GHz. A frequency drift of 16 MHz/h at a detuning of -5.6  GHz and 4 MHz/h at a detuning of -5.2  GHz were also obtained for the transmitted and reflected light Faraday signal.
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                Author and article information

                Journal
                2017-02-23
                Article
                1702.07755
                4a00b384-c41c-4b9b-951b-e5622d446d77

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                29 pages, 6 figures
                physics.atom-ph

                Atomic & Molecular physics
                Atomic & Molecular physics

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