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Direct comparison of nuclear-spin-gyroscope schemes

Haifeng Dong, Yang Gao

Published Jun 29, 2016• 0 citations
OpenAlex

Abstract

We demonstrate that NMR gyroscope and comagnetometer SERF gyroscope can be described with a common model, which explains the compensation and enhancement effects in the same way. The error models and the advantage/disadvantage of two kinds of atomic spin gyroscope are also discussed.

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Nuclear Spin Gyroscope Based on an Atomic Comagnetometer

Thomas W. Kornack, Rajat K. Ghosh, Michael V. Romalis

We describe a nuclear spin gyroscope based on an alkali-metal--noble-gas comagnetometer. Optically pumped alkali-metal vapor is used to polarize the noble-gas atoms and detect their gyroscopic precession. Spin precession due to magnetic fields as well as their gradients and transients can be cancelled in this arrangement. The sensitivity is enhanced by using a high-density alkali-metal vapor in a spin-exchange relaxation free regime. With a $\mathrm{K}\mathrm{\text{\ensuremath{-}}}^{3}\mathrm{He}$ comagnetometer we demonstrate rotation sensitivity of $5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}\text{ }\text{ }\mathrm{rad}\text{ }{\mathrm{s}}^{\ensuremath{-}1}\text{ }{\mathrm{Hz}}^{\ensuremath{-}1/2}$, equivalent to a magnetic field sensitivity of $2.5\text{ }\text{ }\mathrm{fT}/{\mathrm{Hz}}^{1/2}$. The rotation signal can be increased by a factor of 10 using $^{21}\mathrm{Ne}$ with a smaller magnetic moment. The comagnetometer is also a promising tool in searches for anomalous spin couplings beyond the standard model.

arXiv:physics/0505089•Physical Review Letters•Nov 29, 2005•566 citations
There are two kinds of atomic vapor cell gyroscopes, one is nuclear-magnetic-resonance (NMR) gyroscope and the other is spin-exchange-relaxation-free (SERF) gyroscope. We demonstrate that there is a common model for these two kinds of gyroscope. The output signals of NMR and SERF gyroscopes are compared directly, which provides an important guidance for the scheme choosing and optimization of atomic gyroscope. Although this expose of the equivalence cannot solve the current problems of atomic gyroscopes, such as the narrow response bandwidth of SERF gyroscope and the drift due to the different Fermi-contact interaction coefficient in NMR gyroscope, it provides a simple understanding of atomic gyroscopes and may inspire new schemes combining advantages of both NMR and SERF gyroscopes.
In recent years, developments in quantum sensing, laser, and atomic sensor technologies have also enabled advancement in the field of quantum navigation. Atomic-based gyroscopes have emerged as one of the most critical atomic sensors in this respect. In this review, a brief technology statement of spin exchange relaxation free (SERF) and nuclear magnetic resonance (NMR) type atomic comagnetometer gyroscope (CG) is presented. Related studies in the literature have been gathered, and the fundamental compositions of CGs with technical basics are presented. A comparison of SERF and NMR CGs is provided. A basic simulation of SERF CG was carried out because of its high theoretic bias stability limit. Besides, some highly critical challenges for CGs were examined and reported with compensation methods. The objective of this review is to offer a guide for researchers to develop high-precision atomic gyroscopes and to encourage further research.
We describe a new nuclear spin gyroscope based on K-3He comagnetometer. In this type of Gyroscope, there is much space in improving the sensitivity of measurement, therefore, it's significant to study it. In the comagnetometer, the state equation of the system is very complicated, and we just give the relationship between comagnetometer signal and the rotation angle of gyroscpoe in Bloch picture. Finally, we extend the equation of system to quantum filtering equation, so that we could improve the stability of system and sensitivity of measurement by continuous measurement and quantum feedback control.
We describe a nuclear spin gyroscope based on an alkali-metal--noble-gas comagnetometer. Optically pumped alkali-metal vapor is used to polarize the noble-gas atoms and detect their gyroscopic precession. Spin precession due to magnetic fields as well as their gradients and transients can be cancelled in this arrangement. The sensitivity is enhanced by using a high-density alkali-metal vapor in a spin-exchange relaxation free regime. With a $\mathrm{K}\mathrm{\text{\ensuremath{-}}}^{3}\mathrm{He}$ comagnetometer we demonstrate rotation sensitivity of $5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}\text{ }\text{ }\mathrm{rad}\text{ }{\mathrm{s}}^{\ensuremath{-}1}\text{ }{\mathrm{Hz}}^{\ensuremath{-}1/2}$, equivalent to a magnetic field sensitivity of 2.5  fT/Hz1/22.5\text{ }\text{ }\mathrm{fT}/{\mathrm{Hz}}^{1/2}2.5  fT/Hz1/2. The rotation signal can be increased by a factor of 10 using 21Ne^{21}\mathrm{Ne}21Ne with a smaller magnetic moment. The comagnetometer is also a promising tool in searches for anomalous spin couplings beyond the standard model.